the radiation chemistry of gases at the interface with
Post on 15-Nov-2021
1 Views
Preview:
TRANSCRIPT
1
The Radiation Chemistry of Gases at the Interface with Ceramic Oxides
A thesis submitted to the University of Manchester for the degree of Doctor of Philosophy
in the Faculty of Engineering and Physical Sciences
2015
Luke Jones
School of Chemistry Dalton Cumbrian Facility
7161060
1
List of Contents
List of Contents ................................................................................................................ 1
List of Figures ................................................................................................................... 6
List of Tables .................................................................................................................. 14
Abbreviations and Acronyms .......................................................................................... 16
Abstract ......................................................................................................................... 17
Declaration .................................................................................................................... 18
Copyright Statement ...................................................................................................... 19
Acknowledgements ........................................................................................................ 20
The Author ..................................................................................................................... 22
Thesis Structure .............................................................................................................. 23
1 Introduction ............................................................................................................ 25
The Challenge .................................................................................................................................... 25
1.1 Background ........................................................................................................................... 26
1.2 Radiation Chemistry .............................................................................................................. 32
1.2.1 Sources of Radiation ..................................................................................................... 32
1.2.2 Radiation Interactions with Matter .............................................................................. 35
1.2.3 Radiolytic Track Formation ........................................................................................... 44
2 Literature Review .................................................................................................... 47
2.1 ππ’π2 Storage Canisters ........................................................................................................ 47
2.2 Water Adsorption on ππ’π2 .................................................................................................. 50
2.3 Radiolysis of Adsorbed Water ............................................................................................... 51
2.4 Radiolysis of Gases in Contact with ππ’π2 ............................................................................. 52
2.5 Radiolysis of π»2 β π2 in Contact with Other Materials ........................................................ 55
2.6 Radiolysis of Hydrogen and Oxygen ...................................................................................... 56
2.7 Air Radiolysis ......................................................................................................................... 58
Aims and Objectives .......................................................................................................................... 60
7161060
2
3 Experimental ........................................................................................................... 61
3.1 Materials ............................................................................................................................... 61
3.1.1 Gases ............................................................................................................................. 61
3.1.2 Chemicals ...................................................................................................................... 61
3.2 Irradiation Sources ................................................................................................................ 62
3.2.1 Cobalt-60 Source ........................................................................................................... 62
3.2.2 Pelletron Ion Accelerator .............................................................................................. 64
3.3 Analytical Techniques ........................................................................................................... 65
3.3.1 Gas Chromatography (GC) ............................................................................................ 65
3.3.2 Ion Chromatography (IC) ............................................................................................... 66
3.3.3 Surface Area Measurements......................................................................................... 66
3.3.4 Thermogravimetric Analysis (TGA) ............................................................................... 67
3.3.5 Diffuse Reflectance Infra-red Spectroscopy (DRIFT) ..................................................... 67
3.3.6 UV-Vis Spectroscopy ..................................................................................................... 68
3.3.7 Scanning Electron Microscopy (SEM)............................................................................ 68
3.4 Experimental ......................................................................................................................... 69
3.4.1 Mixing of π»2 β π2 β π΄π Samples ................................................................................. 69
3.4.2 Air Radiolysis ................................................................................................................. 71
3.4.3 Oxide Regeneration ...................................................................................................... 73
3.4.4 Accelerator Experiments ............................................................................................... 73
4 Development of Ξ³-Irradiation Reaction Vessel .......................................................... 76
4.1 Initial Vessel Design .............................................................................................................. 76
4.1.1 GC Configuration and Calibration ................................................................................. 77
4.2 Reaction Vessel Mark II ......................................................................................................... 82
4.2.1 GC Calibration ............................................................................................................... 83
4.3 Reaction Vessel Mark III ........................................................................................................ 86
4.3.1 GC Configuration and Calibration ................................................................................. 86
4.4 Gas Mixing ............................................................................................................................. 92
7161060
3
5 Dosimetry ................................................................................................................ 97
5.1 Background ........................................................................................................................... 97
5.2 Aqueous Dosimetry ............................................................................................................... 99
5.3 Calculation of Absorbed Dose using 60πΆπ Source ............................................................... 103
5.3.1 Adsorbed Dose in Gaseous Systems ........................................................................... 105
5.3.2 Literature Review of Heterogeneous System Dosimetry ............................................ 107
5.4 Disadvantages of Fricke Dosimetry with Metal Vessels ..................................................... 109
5.5 Gas Phase Dosimetry .......................................................................................................... 110
5.5.1 Gas Phase Dosimetry Literature.................................................................................. 110
5.5.2 Ethylene Dosimetry Results ........................................................................................ 113
5.6 Ion Accelerator Dosimetry .................................................................................................. 114
6 Oxide Powder Characterisation .............................................................................. 118
6.1 Properties of πΆππ2 .............................................................................................................. 118
6.1.1 As Received ................................................................................................................. 118
6.1.2 Regenerated πΆππ2 Properties .................................................................................... 121
6.1.3 Comparison of βAs Receivedβ and Regenerated πΆππ2 ................................................ 125
6.2 Properties of πππ2 .............................................................................................................. 127
6.2.1 As Received ................................................................................................................. 127
6.2.2 Regenerated πππ2 Properties..................................................................................... 130
6.2.3 Comparison of βAs Receivedβ and Regenerated πππ2 ................................................ 135
6.3 Comparison of Regenerated πΆππ2 and πππ2 ..................................................................... 137
7 π―2 β πΆ2 Radiolysis Results and Discussion .............................................................. 139
7.1 Discussion of πΆ2π»4 Dosimetry in Comparison with Fricke Dosimetry ................................ 139
7.2 Source of Errors in Ethylene Dosimetry .............................................................................. 142
7.3 Mechanism of Ethylene (πΆ2π»4) Radiolysis .......................................................................... 146
7.4 π»2 Production from Adsorbed Water on Oxide Powders................................................... 149
7.5 Radiolysis of Ethylene in Contact with Oxides .................................................................... 152
7.6 Gamma Radiolysis of π»2 β π2 β π΄π Gas Mixtures ............................................................. 162
7161060
4
7.6.1 Discussion .................................................................................................................... 168
7.7 Gamma Radiolysis of π»2 β π2 β π΄π in the Presence of an Oxide Surface ......................... 172
7.8 Comparison of Homogeneous and Heterogeneous Radiolysis ........................................... 177
7.9 Discussion of Pelletron Dosimetry ...................................................................................... 181
7.9.1 Source of Errors in Ethylene Analysis .......................................................................... 183
7.9.2 Source of Errors in Current Measurements ................................................................ 184
7.10 π»2 β π2 β π΄π Radiolysis using an Ion Accelerator ............................................................. 186
7.11 Comparison of Ξ³ and π»π2+ Irradiation of Gaseous π»2 β π2 β π΄π Samples ..................... 187
8 Air Radiolysis Results and Discussion ..................................................................... 191
8.1 Ion Chromatogram Calibration ........................................................................................... 191
8.2 Air Radiolysis ....................................................................................................................... 193
8.3 Air Radiolysis in the Presence of an Oxide Surface ............................................................. 195
8.3.1 Comparison of πΆππ2 Data ........................................................................................... 202
8.3.2 Discussion .................................................................................................................... 203
8.3.3 Comparison of πππ2 Data ........................................................................................... 206
8.4 Explanation of Scatter in 50% and 90% (by volume) πππ2 Results .................................... 208
8.5 Refinement of Experimental Data in the Presence of an Oxide Surface ............................ 214
8.5.1 Compiled Data ............................................................................................................. 217
8.5.2 Discussion .................................................................................................................... 220
8.6 Oxalate ................................................................................................................................ 224
8.6.1 Oxalate Discussion ...................................................................................................... 227
8.7 Synthetic Air ........................................................................................................................ 232
8.8 Sintered πΆππ2 ..................................................................................................................... 234
8.8.1 Oxide Properties ......................................................................................................... 234
8.8.2 Nitrate Production over Sintered πΆππ2 ...................................................................... 237
8.8.3 Comparison with Un-sintered πΆππ2 Results ............................................................... 238
8.8.4 Discussion .................................................................................................................... 239
7161060
5
9 Final Conclusions ................................................................................................... 244
9.1 π»2 β π2 System .................................................................................................................. 244
9.2 Air Radiolysis System .......................................................................................................... 245
10 Future work ........................................................................................................... 247
10.1 π»2 β π2 β π΄π System ......................................................................................................... 247
10.2 Air Radiolysis System .......................................................................................................... 248
10.3 πΆ2π»4 System ....................................................................................................................... 248
10.4 Generic Recommendations ................................................................................................. 249
10.5 Future Work with Accelerated Ions .................................................................................... 251
11 Bibliography .......................................................................................................... 254
Word Count: 51,594
7131060
6
List of Figures
Figure 1.1: ππ’π2 surface area as a function of calcination temperature ............................................ 28
Figure 1.2: SEM images of ππ’π2 stored at the Sellafield site .............................................................. 29
Figure 1.3: Stainless steel three can system used to package THORP ππ’π2 ....................................... 30
Figure 1.4: Comparison of path length and penetration for a Ξ² particle .............................................. 36
Figure 1.5: Emission of Bremsstrahlung ............................................................................................... 37
Figure 1.6: Positron annihilation ........................................................................................................... 38
Figure 1.7: Overview of Auger electron emission ................................................................................. 39
Figure 1.8: Ξ³-ray interaction processes and their dependence on photon energy and Z of medium ... 40
Figure 1.9: The photoelectric effect at i) low photon energies and ii) high photon energies ............... 41
Figure 1.10: Compton scattering .......................................................................................................... 41
Figure 1.11: Pair production followed by positron annihilation ........................................................... 43
Figure 1.12: Radiolytic track structure of i) Ξ± particle and ii) fast electron .......................................... 45
Figure 2.1: Postulated mechanism of water adsorption onto a ππ’π2 surface .................................... 50
Figure 3.1: Foss Therapy Model 812 60πΆπ Irradiation source ............................................................... 62
Figure 3.2: Decay scheme for cobalt-60 isotopes ................................................................................. 63
Figure 3.3: Schematic of 5 MV Ion accelerator located at DCF ............................................................ 64
Figure 3.4: Bespoke gas mixing manifold system ................................................................................. 70
Figure 3.5: Picture of l-r 1 g, 50% oxide (by volume) and 90% oxide (by volume) for πππ2 samples ... 71
Figure 3.6: Bespoke glassware for π»π2+ ion radiolysis of π»2 β π2 β π΄π gaseous mixtures ............... 74
Figure 3.7: Configuration of window assembly through which the beam travels before reaching the
sample ................................................................................................................................. 75
Figure 4.1: Reaction vessel for gamma radiation studies of π»2 β π2 system ...................................... 76
Figure 4.2: Sample holder for gamma irradiation of π»2 β π2 system ................................................. 77
Figure 4.3: GC valve configuration for βin-lineβ analysis i) βLoadβ position ii) βInjectβ position .............. 78
7131060
7
Figure 4.4: Calibration of the gas chromatograph using certified calibration standards in the range
0.1-4% π»2/π΄π ..................................................................................................................... 79
Figure 4.5: Gas chromatograms of 2% π»2/π΄π and 0.5% π»2/π΄π calibration gases .............................. 79
Figure 4.6: Overlain chromatograms of initial trials of π»2 β π2 radiolysis experiments ..................... 81
Figure 4.7: Mechanical degradation of πππΉπΈ taps .............................................................................. 82
Figure 4.8: Stainless steel sampling cylinder for π»2 β π2 gamma irradiation experiments ................ 83
Figure 4.9: Calibration plot for pure π»2 using the direct injection methodology ................................. 84
Figure 4.10: Overlay of gas chromatograms highlighting varying injection volumes of pure π»2 ........ 85
Figure 4.11: Final vessel iteration to investigate radiolysis of π»2 β π2 systems .................................. 86
Figure 4.12: Final GC valve configuration i) βLoadβ position ii) βInjectβ position .................................... 87
Figure 4.13: Plot of sample loop pressure as a function of time for six repeat injections with vacuum
GC configuration ............................................................................................................... 88
Figure 4.14: GC calibration curve of hydrogen partial pressure as a function of peak area for vacuum
sampling system ............................................................................................................... 89
Figure 4.15: Plot of π»2 peak area as a function of sample loop pressure for a series of samples
containing 5:5:90 π»2: π2: π΄π ............................................................................................ 91
Figure 4.16: Plots of π»2 peak area as a function of sample loop pressure of four different gas mixes i)
2% π»2/π΄π calibration gas, ii) pure hydrogen gas, iii) 10:90 π»2: π΄π gas mix from manifold
and iv) 5:5:90 π»2: π2: π΄π gas mix from manifold ............................................................. 93
Figure 4.17: Manifold schematic with new mixing cylinder and πππΉπΈ stirrer bar addition ................ 95
Figure 4.18: Final iteration of manifold design ..................................................................................... 95
Figure 4.19: Mixing efficiency of manifold with mixing cylinder for a three component gas mixture . 96
Figure 5.1: Fricke dosimetry results for the test tube rack array showing i) Unattenuated dose rate
ii) Fully attenuated dose rate (units β Gy min-1) ............................................................... 102
Figure 5.2: Ξ³-ray interaction processes and their dependence on photon energy and Z of medium . 105
Figure 5.3: Results of ethylene dosimetry (units β Gy min-1) .............................................................. 114
7131060
8
Figure 5.4: Plot of current as a function of time for a 15 min irradiation using the ion accelerator
showing the current measured on the ππ window ............................................................ 116
Figure 6.1: Scanning electron micrograph of πΆππ2 (as received) ....................................................... 118
Figure 6.2: EDS spectrum of πΆππ2 (as received) ................................................................................. 119
Figure 6.3: BET adsorption (solid trace) - desorption (dashed trace) of πΆππ2 (as received) .............. 119
Figure 6.4: DRIFT spectra of πΆππ2 (as received) ................................................................................. 120
Figure 6.5: SEM images of regenerated πΆππ2 illustrating the macrostructure of the powder (top) and
a large particle (bottom) ................................................................................................... 122
Figure 6.6: BET adsorption (solid trace) β desorption (dashed trace) isotherm for regenerated πΆππ2
.......................................................................................................................................... 123
Figure 6.7: Thermogram of regenerated πΆππ2 decomposed under π2 (blue) and static air (red).
Heating rate 10 Β°C min-1 .................................................................................................... 124
Figure 6.8: DRIFT spectrum of regenerated πΆππ2 .............................................................................. 125
Figure 6.9: DRIFT spectra of πΆππ2 (as received) and regenerated πΆππ2 upto five subsequent
regeneration cycles ........................................................................................................... 126
Figure 6.10: SEM image of πππ2 (as received) ................................................................................... 127
Figure 6.11: EDS spectrum of πππ2 (as received) ............................................................................... 128
Figure 6.12: BET adsorption (solid trace) β desorption (dashed trace) isotherm of πππ2 (as received)
........................................................................................................................................ 128
Figure 6.13: DRIFT spectrum of πππ2 (as received) ............................................................................ 129
Figure 6.14: SEM images of regenerated πππ2 illustrating large agglomerated particles ................ 131
Figure 6.15: EDS spectrum of regenerated πππ2 ................................................................................ 132
Figure 6.16: Thermogram of regenerated πππ2 decomposed under π2 (blue) and static air (red).
Heating rate 10 Β°C min-1 .................................................................................................. 133
Figure 6.17: BET adsorption (solid trace)-desorption (dashed trace) isotherm of regenerated πππ2 134
Figure 6.18: DRIFT spectrum of regenerated πππ2 ............................................................................ 135
7131060
9
Figure 6.19: DRIFT spectra of πππ2 (as received) and regenerated πππ2 upto four subsequent
regeneration cycles ......................................................................................................... 137
Figure 7.1: Comparison of dose rates obtained by different chemical dosimeters (units Gy min-1)
i) Fricke dosimetry and ii) ethylene dosimetry .................................................................. 140
Figure 7.2: Plot of scatter in each sample of ethylene as a function of the peak area of π»2 in the first
injection ............................................................................................................................. 142
Figure 7.3: Gas chromatogram overlay of three subsequent injections of post irradiated ethylene
highlighting the π»2 signal ................................................................................................. 143
Figure 7.4: Gas chromatogram of two separate ethylene samples irradiated for i) 540 min and
ii) 5760 min ....................................................................................................................... 144
Figure 7.5: Results of ethylene dosimetry at increased pressure (units β Gy min-1) ........................... 146
Figure 7.6: Hydrogen production as a function of absorbed dose from water adsorbed to πππ2
(primary y-axis) and πΆππ2 (secondary y-axis) ................................................................... 150
Figure 7.7: Gas chromatograms showing a comparison of the π»2 signal of irradiated ethylene (πΆ2π»4)
(blue trace), πΆππ2 in π΄π atmosphere (green trace) and πΆππ2 in ethylene (πΆ2π»4) (red trace)
irradiated for 9 h in identical radiation fields ................................................................... 153
Figure 7.8: Gas chromatograms showing a comparison of the π»2 signal of irradiated ethylene (πΆ2π»4)
(blue trace β secondary y-axis), πππ2 in π΄π atmosphere (green trace β secondary y-axis)
and πππ2 in ethylene (πΆ2π»4) (red trace β primary y-axis) irradiated for 9 h in identical
radiation fields .................................................................................................................. 154
Figure 7.9: Postulated schematic of ethylene interaction with an oxide surface ............................... 156
Figure 7.10: DRIFT spectra of regenerated πΆππ2 pre-irradiation (blue) and post-irradiation (red) in an
ethylene atmosphere ...................................................................................................... 158
Figure 7.11: DRIFT spectra of regenerated πππ2 pre-irradiation (blue) and post-irradiation (red) in an
ethylene atmosphere ...................................................................................................... 159
7131060
10
Figure 7.12: DRIFT spectra of irradiated πΆππ2 in an ethylene atmosphere analysed between
20 β 400 Β°C ...................................................................................................................... 160
Figure 7.13: DRIFT spectra of irradiated πππ2 in an ethylene atmosphere analysed between
20 β 400 Β°C ...................................................................................................................... 161
Figure 7.14: Results of gamma radiolysis of different ratios of π»2 β π2 β π΄π illustrating π»2 depletion
as a function of absorbed dos ........................................................................................ 163
Figure 7.15: Plot of G(-π»2) as a function of absorbed dose for several different ratios of π»2 β
π2 β π΄π gas using gamma radiation using the data in Figure 7.14 .............................. 165
Figure 7.16: π2 depletion as a function of absorbed dose using gamma radiation of different ratios of
π»2 β π2 β π΄π gas mixtures ........................................................................................... 166
Figure 7.17: Plot of G(-π2) as a function of absorbed dose for several different ratios of π»2 β
π2 β π΄π gas using gamma radiation using the data in Figure 7.16 .............................. 167
Figure 7.18: π»2 consumption as a function of absorbed dose for various π»2 β π2 β π΄π gas mixtures
in contact with πΆππ2 ...................................................................................................... 173
Figure 7.19: Plot of G(-π»2) as a function of absorbed dose for several different ratios of π»2 β
π2 β π΄π gas in contact with πΆππ2 ................................................................................. 174
Figure 7.20: Plot of π»2 consumption as a function of absorbed dose for the five gaseous systems of
relevance in contact with πππ2 ...................................................................................... 175
Figure 7.21: G(-π»2) as a function of absorbed dose for five gaseous mixtures of π»2 β π2 β π΄π
irradiated in contact with πππ2 ..................................................................................... 176
Figure 7.22: π»2 consumption as a function of absorbed dose in samples of 5: 5: 90 π»2 β π2 β π΄π
concentration in contact with πΆππ2 and πππ2 and in pure gas system only ................. 177
Figure 7.23: π»2 consumption as a function of absorbed dose in samples of 5: 2.5: 92.5 π»2 β π2 β π΄π
concentration in contact with πΆππ2 and πππ2 and in pure gas ..................................... 179
Figure 7.24: π»2 consumption as a function of absorbed dose in samples of 2.5: 5: 92.5 π»2 β π2 β π΄π
concentration in contact with πΆππ2 and πππ2 and in pure gas ..................................... 180
7131060
11
Figure 7.25: Plot of π»2 production as a function of absorbed dose for ethylene experiments using an
ion accelerator ................................................................................................................ 182
Figure 7.26: Plot of pressure as a function of time for a sample of ethylene irradiated using 5.5 MeV
π»π2+ ions. Irradiation time 30 min, 10 nA current on sample ....................................... 183
Figure 7.27: π»2 depletion as a function of absorbed dose for three different mixtures of
π»2 β π2 β π΄π utilising 5.5 MeV π»π2+ accelerated ions ................................................ 186
Figure 7.28: π»2 depletion as a function of absorbed dose for three various mixtures of π»2 β π2 β π΄π
utilising 60πΆπ Ξ³-rays and 5.5 MeV π»π2+ accelerated ions .............................................. 188
Figure 8.1: Calibration plot of ππ3β peak area as a function of ππππ3 concentration using ion
chromatography ............................................................................................................... 192
Figure 8.2: Effect of Ξ³ radiation dose on nitrate production from laboratory air ............................... 193
Figure 8.3: Effect of Ξ³ radiation dose on the production of nitrate in water saturated and unsaturated
laboratory air. Volume of air = 11.9-12.0 cm3 at 35 Β°C ..................................................... 194
Figure 8.4: Nitrate production as a function of dose for systems containing 1 g of either πΆππ2 or πππ2
powder and water saturated air (no oxide) ...................................................................... 196
Figure 8.5: Nitrate production as a function of absorbed dose for systems containing 50% oxide (by
volume) and for water saturated air (no oxide) ................................................................ 199
Figure 8.6: Nitrate production as a function of dose for systems containing 90% oxide (by volume)
and for water saturated air (no oxide) .............................................................................. 201
Figure 8.7: Nitrate production as a function of absorbed dose for 1 g, 50% and 90% (by volume) πΆππ2
systems and for water saturated air (no oxide) ................................................................ 202
Figure 8.8: Nitrate production as a function of absorbed dose for 1 g, 50% and 90% (by volume) πΆππ2
systems and for water saturated air (no oxide) up to an absorbed dose of 2.0x1019 eV .. 203
Figure 8.9: i) Face-centred cubic crystal structure unit cell, and ii) atomic structure of each face in the
unit cell ........................................................................................................................... 205
7131060
12
Figure 8.10: Nitrate production as a function of absorbed dose for 1 g, 50% and 90% (by volume)
πππ2 systems and for water saturated air (no oxide) .................................................... 207
Figure 8.11: Three ion chromatograms of samples containing: i) 1 g, ii) 50% and iii) 90% πππ2 (by
volume) illustrating the emergence of a second signal at 6.6 min................................. 209
Figure 8.12: Ion chromatogram of 50 ΞΌM oxalic acid, 0.1 mM sodium nitrate and a mixed solution of
both ................................................................................................................................ 212
Figure 8.13: Chromatogram of 0.1 mM ππππ3 and 50 ΞΌM oxalic acid mixed solution using eluent
concentration of 14 mM πΎππ» ....................................................................................... 213
Figure 8.14: Nitrate production as a function of dose for samples containing 1 g of oxide powder and
for water saturated air (no oxide) .................................................................................. 214
Figure 8.15: Nitrate production as a function of dose for samples containing 50% (by volume) πΆππ2
and πππ2 and from water saturated air (no oxide) ....................................................... 215
Figure 8.16: Nitrate production as a function of dose for samples containing 90% (by volume) πΆππ2
and πππ2 and from water saturated air (no oxide) ....................................................... 216
Figure 8.17: Nitrate production as a function of absorbed dose for 1 g, 50% and 90% (by volume)
πΆππ2 systems and for water saturated air (no oxide) .................................................... 217
Figure 8.18: Nitrate production as a function of absorbed dose for 1 g, 50% and 90% (by volume)
πππ2 systems and water saturated air (no oxide) ......................................................... 219
Figure 8.19: Pictorial representation of ππ3β bonding modes with metal centres depicting (l-r)
monodentate, bidentate and bridging adsorption modes ............................................. 222
Figure 8.20: Calibration plot of πΆ2π42β peak area as a function of π»2πΆ2π4 concentration using ion
chromatography ............................................................................................................. 224
Figure 8.21: Plot of oxalate production as a function of absorbed dose for samples containing 1 g,
50% and 90% (by volume) of πΆππ2 and from water saturated air (no oxide) ................ 225
Figure 8.22: Plot of oxalate production as a function of absorbed dose for samples containing 1 g,
50% and 90% (by volume) of πππ2 and from water saturated air (no oxide) ................ 226
7131060
13
Figure 8.23: Thermogravimetric analysis of cerium oxalate under π2 (blue) and static air (red)
atmospheres. Heating rate 2 Β°C min-1 ............................................................................. 227
Figure 8.24: Plot of nitrate production as a function of absorbed dose for synthetic air, laboratory air
and water saturated laboratory air. Volume of air =11.9 - 12.0 cm3 at 35 Β°C ................ 233
Figure 8.25: BET adsorption (solid trace) β desorption (dashed trace) isotherm of πΆππ2 sintered at
950 Β°C for 2 h................................................................................................................... 235
Figure 8.26: i) Scanning electron micrograph and ii) EDS spectra for sintered πΆππ2 ......................... 236
Figure 8.27: Nitrate production as a function of absorbed dose for samples containing 1 g, 50% and
90% (by volume) sintered πΆππ2 and from water saturated air (no oxide) ..................... 237
Figure 8.28: Compiled data plot of nitrate production as a function of dose for systems containing
1 g, 50% and 90% (by volume) regenerated πΆππ2, 1 g, 50% and 90% (by volume) sintered
πΆππ2 and from water saturated air (no oxide) .............................................................. 238
Figure 8.29: Plot of G(ππ3β) as a function of surface area for the three oxide systems utilised in this
research and for reference, the water saturated air (no oxide) yield ............................ 240
Figure 10.1: Sketch of possible reaction vessel to study heterogeneous systems using an ion
accelerator ...................................................................................................................... 252
Figure 10.2: Second possible reaction vessel for heterogeneous system experiments using an ion
accelerator ...................................................................................................................... 253
7131060
14
List of Tables
Table 7-1: Calculated G(-π»2) values for several different ratios of π»2 β π2 β π΄π gas using gamma
radiation ............................................................................................................................ 164
Table 7-2: Calculated G(-π2) values for several different ratios of π»2 β π2 β π΄π gas using gamma
radiation ............................................................................................................................ 166
Table 7-3: Ionisation energy of the three gas molecules in the initial system .................................... 168
Table 7-4: Calculated G(-π»2) in samples containing 5: 5: 90 π»2 β π2 β π΄π (by volume) in the
presence of πΆππ2, πππ2 and in pure gas phase ................................................................ 178
Table 7-5: Calculated G(-π»2) values from experiments utilising 5.5 MeV π»π2+ accelerated ions ..... 187
Table 7-6: Calculated G(-π»2) values and associated errors for three different mixtures of
π»2 β π2 β π΄π utilising 60πΆπ Ξ³-rays and 5.5 MeV π»π2+ accelerated ions ........................ 188
Table 8-1: Calculated G(ππ3β) values and standard deviation of the gradient for 1 g oxide systems
and water saturated air (no oxide) ................................................................................... 196
Table 8-2: Calculated mass of water in systems containing 1 g πΆππ2, 1 g πππ2 and water saturated
air (no oxide) ..................................................................................................................... 197
Table 8-3: Calculated mass of water in systems containing 50% πΆππ2 and 50% πππ2 (by volume) and
water saturated air (no oxide) .......................................................................................... 198
Table 8-4: Calculated G(ππ3β) values and standard deviation of the gradient for experiment with 50%
oxide (by volume) and with water saturated air (no oxide) .............................................. 199
Table 8-5: Calculated mass of water in systems containing 90% πΆππ2 and 90% πππ2 (by volume) and
water saturated air (no oxide) .......................................................................................... 200
Table 8-6: Calculated G(ππ3β) values and standard deviation of the gradient for systems with 90%
oxide (by volume) and for water saturated air (no oxide) ................................................ 201
Table 8-7: Calculated G(ππ3β) values for the πΆππ2 containing systems and for water saturated air
(no oxide) .......................................................................................................................... 202
Table 8-8: Initial yield of nitrate pre-irradiation ................................................................................. 204
Table 8-9: Calculated G(ππ3β) values for the system containing πππ2 and for water saturated air
(no oxide) .......................................................................................................................... 207
Table 8-10: Anions and corresponding retention times (in minutes) present in deionised water ...... 210
Table 8-11: Calculated G(ππ3β) values and standard deviation of the gradient for systems with 1 g
oxide and water saturated air (no oxide) ....................................................................... 214
Table 8-12: Calculated G(ππ3β) values and standard deviation of the gradient for systems with 50%
oxide (by volume) and water saturated air (no oxide) ................................................... 215
7131060
15
Table 8-13: Calculated G(ππ3β) values and standard deviation of the gradient for systems with 90%
oxide (by volume) and water saturated air (no oxide) ................................................... 216
Table 8-14: Calculated G(ππ3β) values and standard deviation of the gradient for systems with 1 g,
50% and 90% (by volume) πΆππ2 and water saturated air (no oxide) ............................ 218
Table 8-15: Calculated G(ππ3β) values and standard deviation of the gradient for systems with 1 g,
50% and 90% (by volume) πππ2 and water saturated air (no oxide) ............................ 219
Table 8-16: Calculated G(ππ3β) values and standard deviation of the gradient for systems containing
1 g, 50% and 90% (by volume) sintered πΆππ2 and water saturated air (no oxide) ........ 237
Table 8-17: Comparison between calculated G(ππ3β) for samples containing either regenerated πΆππ2
or sintered πΆππ2 and water saturated air (no oxide) ..................................................... 239
7131060
16
Abbreviations and Acronyms
AGR - Advanced Gas-Cooled Reactor
B.E.T. - Brunauer β Emmett β Teller Theory
DCF - Dalton Cumbrian Facility
DRIFT - Diffuse Reflectance Infrared Fourier Transform Spectroscopy
ECD - Electrochemical Detector
EDS - Energy Dispersive X-ray Spectroscopy
G (Β±X) - yield of change (units: molecules 100 eV-1)
G.C. - Gas Chromatography
Gray - SI unit of ionising radiation dose (units: J kg-1)
I.C. - Ion Chromatography
LANL - Los Alamos National Laboratory
L.E.T. - Linear Energy Transfer
Magnox - Magnesium Non-Oxidising Fuel
MOX - Mixed Oxide Fuel
NNL - National Nuclear Laboratory
PUREX - Plutonium and Uranium Recovery by Extraction
SEM - Scanning Electron Microscopy
SSA - Specific Surface Area
TCD - Thermal Conductivity Detector
TGA - Thermogravimetric Analysis
THORP - Thermal Oxide Reprocessing Plant
TORVIS - Toroidal Volume Ion Source
UHV - Ultra-high vacuum
7131060
17
Abstract
The University of Manchester Luke Jones
Thesis submitted for the degree of Doctor of Philosophy
The Radiation Chemistry of Gases at the Interface with Ceramic Oxides
October 2015
As of 2011, the UK had 112 tonnes (t) of plutonium dioxide (ππ’π2) in interim storage at the Sellafield site and this is increasing by approximately 5 t per annum with the continued reprocessing of spent nuclear fuel. ππ’π2 is stored in small quantities in a sealed multi-canister system for security and ease of handling. During long term storage, radiolysis of the gas phase and adsorbed species could potentially lead to canister pressurisation and/or failure. It is of great importance to understand the mechanisms occurring in the gas phase and to understand the resulting gas phase composition after decades of storage.
This research investigates the radiation chemistry of two gas phase systems in the presence or absence of inactive ππ’π2 surrogate material (namely cerium dioxide (πΆππ2 ) and zirconium dioxide (πππ2)).
The systems of interest are, firstly, radiolysis of hydrogen (π»2), oxygen (π2) and argon gas mixtures utilising both 60πΆπ gamma rays and π»π2+ accelerated ions. Depletion of π»2 and π2 has been investigated using gas chromatography. A bespoke manifold has been designed to mix these gases in various ratios, suitable reaction vessels and a subsequent sampling system has been developed to undertake this research. The rate of π»2 depletion is independent of initial π»2 concentration and radiation type. In the presence of an oxide surface, the rate of π»2 depletion is vastly increased when compared to homogeneous studies using 60πΆπ gamma rays. Depletion is greatest in the presence of πππ2. In all systems, depletion of π»2 is linear with increasing absorbed dose.
The second system of interest is the radiolysis of moist air utilising 60πΆπ gamma rays. Formation of nitric acid (π»ππ3) has been investigated using ion chromatography to determine nitrate (ππ3
β) anion production. Nitrate production increases linearly with absorbed dose and is greater in the presence of an oxide powder. The rate of production increases with increasing mass of oxide. Oxalate (πΆ2π4
2β) was produced radiolytically from dimerisation of carbon dioxide and was greatest in the presence of πππ2. Reducing the specific surface area of πΆππ2 reduced the concentration of nitrate formed when compared to higher surface area πΆππ2.
7131060
18
Declaration
No portion of the work referred to in the thesis has been submitted in support of an
application for another degree or qualification of this or any other university or other
institute of learning
β¦β¦β¦β¦β¦β¦β¦β¦β¦β¦β¦β¦β¦β¦β¦..
Luke Jones November 2015
7131060
19
Copyright Statement
The author of this thesis (including any appendices and/or schedules to this thesis) owns
certain copyright or related rights in it (the βCopyrightβ) and he has given The University of
Manchester certain rights to use such Copyright, including for administrative purposes.
Copies of this thesis, either in full or in extracts and whether in hard or electronic copy, may
be made only in accordance with the Copyright, Designs and Patents Act 1988 (as amended)
and regulations issued under it or, where appropriate, in accordance with licensing
agreements which the University has from time to time. This page must form part of any
such copies made.
The ownership of certain Copyright, patents, designs, trademarks and other intellectual
property (the βIntellectual Propertyβ) and any reproductions of copyright works in the
thesis, for example graphs and tables (βReproductionsβ), which may be described in this
thesis, may not be owned by the author and may be owned by third parties. Such
Intellectual Property and Reproductions cannot and must not be made available for use
without the prior written permission of the owner(s) of the relevant Intellectual Property
and/or Reproductions.
Further information on the conditions under which disclosure, publication and
commercialisation of this thesis, the Copyright and any Intellectual Property and/or
Reproductions described in it may take place is available in the University IP Policy (see
http://documents.manchester.ac.uk/DocuInfo.aspx?DocID=487), in any relevant Thesis
restriction declarations deposited in the University Library, The University Libraryβs
regulations (see http://www.manchester.ac.uk/library/aboutus/regulations) and in The
Universityβs policy on Presentation of Theses
7131060
20
Acknowledgements
There are many people I would like to thank for their input throughout the course of this
research.
Firstly, I would like to thank Professor Simon M. Pimblott for selecting me to undertake this
research. I am grateful for his supervision and input and advice with regards to literature
components and experimental suggestions.
Thanks to the EPSRC and Sellafield Sites Ltd. for providing funding for this research.
My gratitudeβs go to Martin Jennings from the School of Chemistry and Alastair Bewsher
from the School of Earth, Atmospheric and Environmental Sciences for undertaking
thermogravimetric analysis and ion chromatography troubleshooting respectively.
I would like to acknowledge Dr Sven Koehler for helping me with the design of the bespoke
gas mixing manifold and other bespoke experimental equipment. His insight into surface
and gas phase chemistry was much appreciated. Also for his non-related bicycle knowledge.
Thanks to Paul Cook and Jeff Hobbs (both of Sellafield Sites Ltd.) for their advice and being
useful sources of reference, and for putting this research into context.
I am extremely grateful to both Howard E. Sims and Robin M. Orr (both of National Nuclear
Laboratory) for their pseudo-supervision and source of encouragement throughout this
research. They have both given an almighty amount of time and effort to enhance this
project and ensured momentum was maintained. Howard, for his never-ending knowledge
of radiation chemistry and his in-depth mechanistic discussions and Robin, for his steel
trap-esque data analysis and his help with gas chromatography and experimental advice.
I would like to thank all the staff and researchers at the Dalton Cumbrian Facility for making
it an enjoyable (and sometimes challenging) place to work. In particular I would like to thank
fellow researchers Logan Barr, Gregory Horne and Rhiannon Monckton (the fellow trolls) for
helping me maintain my sanity and providing an atmosphere for my sense of humour to
flourish, to help stave off cabin fever during the first year of this project and finally, for their
scientific discussions on anything radiation related.
7131060
21
My largest thanks go to Jan, Dave and Adam (a.k.a. mum, dad and big brother) for their help
in making the transition from Oldham to West Cumbria as smooth as possible, for always
being at the end of the telephone to offer reassurance and advice and mostly just for being
themselves.
Finally (and by no means least) to my partner Rebecca, for putting up with my occasional
moods and sarcastic nature, for always being there and offering a sympathetic ear to my
random nonsensical rants, for proof-reading all of my reports and for always being able to
put a smile on my face.
Throughout the highs and lows of this research, many people have reassured me with the
phrase βit builds characterβ and in a way, they have all been right.
βMost people say that it is intellect which makes a great scientist. They are wrong: it is character.β
- Albert Einstein 1879-1955 German-born theoretical physicist
7131060
22
The Author
The author graduated from the University of Manchester in 2011 with an MChem. (Hons)
degree in Chemistry with Industrial Experience. He spent the third year of his degree course
as an industrial placement student at AMEC Power and Process Europe (name has
subsequently changed) based at Birchwood, Warrington as part of the Waste Processing
Technology team. This placement included working on projects for several customers
including Dounreay Site Restoration Limited (DSRL) and Sellafield Sites Ltd. He spent the
final year of his degree undertaking a research project in the Centre for Nanoporous
Materials investigating the synthesis conditions on the crystal morphology of zeolite T.
In September 2011, he joined the Radiation Science research group under the supervision of
Professor Simon Pimblott at the brand new Dalton Cumbrian Facility as a PhD researcher to
investigate the radiation chemistry of gaseous systems at the interface with ceramic oxides.
7131060
23
Thesis Structure
Chapter One outlines the challenge this project hopes to address and gives background
information to put this research into context. It concludes with a basic introduction to
radiation chemistry and how ionising radiation interacts with matter.
Chapter Two reviews the literature relevant to this research. It highlights gaps in the
knowledge base that this research hopes to contribute to. Finally, it outlines the aims and
objectives of this project.
Chapter Three highlights the facilities and experimental equipment utilised to undertake this
research. It details the materials necessary to carry out this project and details the
experimental methods employed to execute this research project.
Chapter Four details the development undertaken in designing a reaction vessel suitable to
implement part of this research. It also details the development in analysis techniques to
complement the evolving reaction vessel.
Chapter Five introduces the concept of dosimetry and the challenges this provides with
regards to this research. Relevant literature is reviewed to provide information on how
these challenges are addressed in other systems and concludes with how dosimetry is
undertaken in the different systems of interest to this research.
Chapter Six details the physical properties of the solid materials utilised throughout the
course of this research.
Chapter Seven details the results pertaining to hydrogen-oxygen radiolysis in homogeneous
and heterogeneous systems. These results are discussed and hypotheses given throughout
the chapter. Finally preliminary results using accelerated ions are detailed and discussed.
7131060
24
Chapter Eight details the results from air radiolysis experiments. These results are analysed
and discussed throughout the chapter.
Chapter Nine pulls together the conclusions drawn from the results detailed in Chapters
Seven and Eight and places these results in the context of the research.
Chapter Ten recommends further experiments that can be undertaken to develop this
research further and answer the questions that have been posed as a result of this research
project.
Chapter Eleven is a bibliography of all the literature sources used throughout this thesis as a
source of information and reference.
Chapter 1 Introduction 7131060
25
1 Introduction
This chapter gives context to this research, to outline the challenges this research hopes to
address and the information it aims to contribute to. It also provides an introduction to
radiation chemistry including sources of radiation and how radiation interacts with matter,
forming radiolytic tracks.
The Challenge
There is currently ~120 t of plutonium dioxide (ππ’π2) in storage at the Sellafield site inside
sealed metal canisters. Some of this plutonium stockpile has been in storage for several
decades, and will continue to be stored for several more. Whilst in storage, these canisters
are dynamic systems, with the overlying gas phase undergoing irradiation from plutonium as
it radioactively decays. The centre-line temperature of the majority of these canisters can be
several hundred Β°C. During long term storage, it is possible that some of these canisters may
pressurise and could potentially fail. Due to the quantity and contents of the canisters, it is
difficult to monitor each canister for possible swelling and/ or failure. There is also minimal
knowledge of the composition of the gas phase as a function of time during the long term
storage of this plutonium stockpile.
This research aims to investigate the gas phase radiation chemistry of two gaseous systems
of interest at the interface of a ππ’π2 surrogate material.
This research aims to deliver a better mechanistic understanding of the gas phase radiation
chemistry in contact with an oxide powder.
It also hopes to aid the safety case for long term storage of ππ’π2.
Chapter 1 Introduction 7131060
26
1.1 Background
The UK currently has the largest stockpile of civil separated plutonium in the world.
Plutonium is a by-product of using uranium metal and uranium oxide (ππ2), as fuel in
nuclear reactors. The spent fuel from the reactor contains approximately 96% uranium and
1% plutonium by weight [1], whilst the remainder is made up of highly radioactive fission
products and minor actinides. It is possible to reuse the spent uranium as new reactor fuel,
however, it must be separated from the fission products and minor actinides first. This
recycling is achieved by reprocessing the spent fuel. Recycling of the uranium allows more
energy to be generated without the use of new supplies, leading to a more sustainable
energy source. In addition, separating uranium from the spent fuel, reduces the volume of
waste generated significantly. Separation of the highly radioactive fission products from the
spent fuel allows for them to be treated separately before going to disposal. The plutonium
generated in spent fuel can also be used as a reactor fuel by blending plutonium dioxide
(ππ’π2) with ππ2 in ratios of 7:93 to create a mixed oxide fuel (MOX). This approach leads to
further energy generation from a single batch of reactor fuel [1].
At present, most nuclear reactors that utilise uranium fuels are allowed a maximum of 33%
loading of MOX fuel in the core due to safety concerns [2]. A different type of nuclear
reactor (termed βfastβ reactor) can utilise plutonium on its own as a fuel type, however,
there are no operational commercial βfastβ reactors in the world at this moment in time and
construction is unlikely to begin until the 2040s. These facts, along with continued
reprocessing of spent fuel leads to large inventories of ππ’π2 stored around the world.
As of 2011, the UK currently had 112 t of civil separated plutonium in storage [3], the
majority of which is stored at the Sellafield site as ππ’π2 powder. There are two product
Chapter 1 Introduction 7131060
27
streams at Sellafield by which this powder is formed. Magnox ππ’π2 is obtained from spent
fuel from Magnesium non-oxidising (Magnox) reactors which used uranium metal, while
ππ’π2 product from the THermal Oxide Reprocessing Plant (THORP) is obtained from spent
fuel from Advanced Gas-Cooled (AGR) reactors which use ππ2 as the fuel type.
To separate the uranium and plutonium from the fission products and minor actinides, the
Plutonium and Uranium Recovery by EXtraction (PUREX) process is employed. This process
has been used globally for several decades as a means of reprocessing spent fuel. The spent
fuel is first dissolved in nitric acid (π»ππ3) before using an organic ligand, tri-butyl phosphate
(ππ΅π) and odourless kerosene (ππΎ) to separate the dissolved species based on their
relative solubility in the organic and aqueous phases [4]. This PUREX process is highly
specific for uranium and plutonium and allows over 99% recovery of these species. Control
of the π»ππ3 concentration allows separation of uranium from plutonium due to their
differing redox chemistry. Once separated, each component is put through an individual
purification cycle to generate an oxide material. There are several steps involved in each
purification cycle which will not be covered in detail here. The main process involved in the
plutonium purification cycle is the reaction of the dissolved plutonium species with oxalic
acid (π»2πΆ2π4) to form a plutonium oxalate (ππ’(πΆ2π4)2. 6π»2π) precipitate. The oxalate
derivative is then washed and thermally decomposed in an oxygen (π2) environment to
produce the finished oxide product (Reaction 1.1):
3ππ’(πΆ2π4)2. 6π»2π + π2 β 3ππ’π2 + 8πΆπ2 + 4πΆπ + 8π»2π Reaction 1.1
Chapter 1 Introduction 7131060
28
After the oxalate decomposition step (Reaction 1.1), the oxide powder is calcined at higher
temperatures to remove adsorbed volatiles and moisture. The moisture content is required
to be less than 0.5 wt.% before the product can go into storage, in accordance with the
United States Department of Energy standard [5]. The temperature at which the ππ’π2
product is calcined can have an effect on the physical properties of the powder. One such
property is the surface area of the finished product. Figure 1.1 shows how increasing the
calcination temperature reduces the surface area as the powder starts to sinter and loses
any porosity.
Figure 1.1: ππ’π2 surface area as a function of calcination temperature (derived from [6])
Higher calcination temperatures remove more of the adsorbed species and reduce the
quantity of residual carbon from the oxalate. In the United States, ππ’π2 is calcined in an
oxidising atmosphere at 950 Β°C for a minimum of two hours before being stored. The trade-
off is that lower surface area reduces the efficiency of potential MOX fuel. There is little
open source information on the calcination conditions used for ππ’π2 produced in the UK,
however, the calcination temperature employed is thought to be nearer to 600 Β°C.
0.0
2.0
4.0
6.0
8.0
10.0
12.0
14.0
400 600 800 1000 1200
B.E
.T. S
urf
ace
Are
a /
m2 g
-1
Calcination temperature / oC
Chapter 1 Introduction 7131060
29
The calcination temperature can also affect the morphology of the resulting ππ’π2 grains.
Machuron-Mandard and Madic [6] discovered two distinct morphologies of ππ’π2 grains.
One is a smooth grain shape corresponding to a truncated octahedra, which is consistent
with a cubic crystal structure. The second structure is less defined with a rough surface.
With increasing calcination temperature, the quantity of the octahedral grains increases.
However it is dependent on the synthesis procedure. Figure 1.2 shows electron micrographs
of ππ’π2 currently in storage in the UK [7, 8].
Figure 1.2: SEM images of ππ’π2 stored at the Sellafield site
The image on the left shows the truncated octahedra crystal morphology typical of the
fluorite structured oxides. The image on the right shows a more agglomerated structure
with flat platelet type crystals. The ππ’π2 products from the two streams at Sellafield have
both types of crystal morphology.
After calcination, the ππ’π2 product is packaged in multi-can containers. In the UK there are
two designs. Magnox ππ’π2 is packaged in a screw top aluminium can, placed inside a
polyethylene bag and welded into a stainless steel outer can. The atmosphere inside the can
is a 50:50 mix of argon and air. ππ’π2 from the THORP product line is packaged in a stainless
steel three can system with a pure argon atmosphere [7, 9]. Figure 1.3 illustrates the cans
Chapter 1 Introduction 7131060
30
used to package THORP ππ’π2 product. Only small quantities (< 1 kg) of ππ’π2 are packaged
in each can for ease of handling and to avoid criticality.
Figure 1.3: Stainless steel three can system used to package THORP ππ’π2
There has been growing national and international pressure to determine a long term
management strategy for the UKβs plutonium stockpile. At the highest level, there are three
credible options [10]:
long term storage in a time bound manner;
immobilisation and disposal as waste; and
re-use as reactor fuel followed by management of spent fuel and subsequent
disposal.
The default option is long term storage, with the Sellafield site plan suggesting the material
will be stored until the site end point in 2120. The continued storage of plutonium materials
will require new stores and infrastructure to be built at a substantial cost.
Prolonged storage of plutonium, results in the gradual conversion into different isotopes as
the isotopes move along their natural radioactive decay sequence. Plutonium-241 (241ππ’),
may be present in the stored material, which undergoes Ξ²-decay to americium-241 (241π΄π),
Chapter 1 Introduction 7131060
31
which is an Ξ±-emitter and also emits Ξ³-rays. The half-life of 241ππ’ is fourteen years, therefore
prolonged storage leads to a significant in-growth of 241π΄π. The presence of this isotope
creates significant challenges in storage of this material and also leads to other options
becoming harder to execute.
There are several options for immobilisation of the plutonium stockpile, these being:
encapsulation in cement, vitrification in glass or immobilisation in a ceramic matrix. There
are concerns, however, about the maturity of the technologies; about the possibility of
extracting the plutonium material at a later date; and about the environmental impact of
disposing of 120 t of plutonium.
Conversion of the stockpile into MOX fuel for use in thermal reactors or conversion to fuel
to be utilised in fast reactors has many advantages, including power generation and good
proliferation resistance. Considerable research and development into the use of plutonium
fuels in next generation reactors such as fast and high temperature reactors [10] is being
undertaken in France, however, this option comes with the substantial financial costs of
building fabrication plants, new reactors, and waste remediation facilities and supporting
infrastructure.
Whichever option is to be selected in the future by the UK government, all require opening
of the multi-can system in Figure 1.3. Whilst in storage, the cans are a dynamic system.
ππ’π2 and its radioactive daughters undergo decay and generate heat. This environment will
potentially lead to chemistry occurring with the overlying headspace and any adsorbed
species on the oxide surface. A number of processes may occur which could lead to
pressurisation of the cans and possible can failure. Therefore an understanding of the
radiation chemistry of the gas phase in the presence of an oxide surface is of importance.
Chapter 1 Introduction 7131060
32
1.2 Radiation Chemistry
The following section outlines the sources of ionising radiation, how these interact with
matter and, finally, how this interaction leads to radiation induced chemistry.
1.2.1 Sources of Radiation
Radiation is a process by which energetic particles or photons travel through a medium. It is
generally split into two types: ionising and non-ionising. Non-ionising radiation has either no
mechanism to transfer energy to the electrons of the material or insufficient energy to
ionise matter and instead, on interaction with an atom or molecule, may cause excitation
within it leading to processes such as luminescence, dissociation, etc... Examples of non-
ionising radiation include visible light, infra-red and microwaves. This type of radiation is not
utilised in this research. Ionising radiation is radiation that does have enough energy to
ionise a given species. This is mostly done by ejection of an electron out of a valence shell
to produce a positively charged ion and an energetic electron. Ionising radiation can also
lead to excitation when interacting with matter.
Radiation chemistry is the study of chemical and physical effects that are produced when a
material is exposed to high energy, ionising radiation. There are two sources of ionising
radiation, firstly, natural or artificial radioactive isotopes and, secondly, those that rely on a
form of particle accelerator.
Radioactive isotopes: These are unstable elements that undergo decay emitting particles
and/or photons. Radioactive decay is a spontaneous nuclear transformation that is
unaffected by pressure, temperature and chemical form of the decaying species. This allows
radioactive decay to be characterized by the decay period and the mode and energy of the
decay [11].
Chapter 1 Introduction 7131060
33
Half-life: The decay period is expressed as a half-life (symbol π‘12). The half life is the time
required for half of the radioactive atoms in a sample to undergo decay. Half-lives can range
from less than a second to 1x1019 years.
Ξ±- decay: An Ξ± particle is a helium atom that has been stripped of both electrons and is
denoted by π»π2+24 . Alpha decay is observed naturally for elements heavier than lead and
certain lanthanides. Alpha particles are emitted by nuclei with discrete energies that are
characteristic of the decaying nuclei, meaning different Ξ± emitters are easy to distinguish by
alpha spectroscopy. Alpha particles usually have energies in the range of 4-9 MeV, with Ξ±-
decay from 239ππ’ having energy of 5.593 MeV. The energy of Ξ± decay is split between the
daughter nuclide and the Ξ± particle. The majority of which goes to the lighter Ξ± particle.
Ξ²- decay: Beta decay is any one of three processes: negatron emission, positron emission and
electron capture. Beta particles are fast moving electrons or positrons that donβt have
discrete energies. Their energy ranges from zero to a maximum energy, (denoted πΈπ½), that is
characteristic of the decaying element. The value of πΈπ½ determines the greatest range the
particle will have in a given medium.
Negatron decay is characteristic of lighter, neutron rich nuclei such as tritium ( π»13 ). At the
atomic level, a neutron is transformed into a proton with the emission of a negatron
(electron).
Positron decay occurs for low and medium mass, neutron poor nuclei. At the atomic level, a
proton is transformed into a neutron with the emission of a positron.
Along with positron and negatron emission, another particle is emitted; this is the neutrino
(symbol Ξ½). It has zero mass and charge, but does have spin and energy. The neutrino is
Chapter 1 Introduction 7131060
34
emitted alongside positron decay and the anti-neutrino (symbol π) is emitted alongside
negatron decay.
Another process of Ξ² decay that does not involve the emission of a negatron or positron is
electron capture. In this intra-molecular transformation process, a proton and an atomic
electron are transformed into a neutron.
Ξ³- decay: Isotopes that undergo gamma decay emit electro-magnetic radiation with energies
ranging between 40 keV to 4 MeV. The electro-magnetic radiation reflects the transition
between energy levels of the same nucleus. Gamma rays either have monoenergetic
energies or a small number of discrete energies that are characteristic of the decaying
nucleus.
Gamma decay occurs alongside other types of radioactive decay (either Ξ± or Ξ²). When a
parent nucleus undergoes Ξ± or Ξ² decay, the daughter nuclide may be in an excited state. It
then loses this excess energy by emitting one or several Ξ³-rays.
The second source of ionising radiation employs particle accelerators. These produce a
focused beam of accelerated electrons or positive particles with energies usually ranging
from keV to MeV. The most commonly used positive particles are protons, deuterons and
helium ions, but heavier ions can be produced if needed. More detail of the ion accelerator
at the Dalton Cumbrian Facility (DCF) will be given in Chapter Three.
Chapter 1 Introduction 7131060
35
1.2.2 Radiation Interactions with Matter
Ξ±-particles: Alpha particles predominantly lose their energy by inelastic collisions with
electrons of the medium in their path. Some of the kinetic energy of the Ξ± particle is
transferred to the electron in an excitation event. However, due to the alpha particles
heavier mass when compared to an electron, only a small fraction of its energy is transferred
to the electron, thus only slight deflection occurs.
The maximum energy transferred from the alpha particle to the electron can be calculated
using the conservation of both energy and momentum and is given by Equation 1.1 [12]:
ππππ₯ = [4ππ
(π+π)2] πΈ Equation 1.1
πΈ = 1
2ππ2 Equation 1.2
where π and π are the mass and velocity of the incident alpha particle and π is the mass of
the electron.
Alpha particles only have a small penetration in liquids and solids (a few Β΅m) before losing
the majority of their energy. In addition, as their mass is much larger than the electron there
is little deflection of the alpha particle when it collides with electrons. Its track through a
medium is fairly straight, creating a column of excited and ionised species.
Ξ²-particles: Like alpha particles, Ξ² particles lose their energy predominantly by inelastic
collisions with electrons. As their mass is equivalent to the electrons of the material, a Ξ²
particle can lose all of its energy in a single collision and can be deflected by a large angle. It
is difficult to differentiate between an incoming and the ejected electron, so the maximum
energy transfer in this case is half the kinetic energy of the incident electron. Deflection may
Chapter 1 Introduction 7131060
36
also occur when a Ξ² particle passes close to an atomic nucleus. As a result of these
deflections, Ξ² particles with the same initial energy can have different ranges in a medium,
however, there will be a maximum distance of penetration. As a consequence of these
deflections, the path length travelled by the Ξ² particle will be far greater than the
penetration into a medium (Figure 1.4):
Figure 1.4: Comparison of path length and penetration for a Ξ² particle
The relative importance of Bremsstrahlung, inelastic and elastic collisions depends heavily
on the energy of the incident particle and the nature of the absorbing material.
Bremsstrahlung (breaking radiation) occurs when an electron passes close to an atomic
nucleus and is decelerated, thus changing direction. With this change in velocity there is a
decrease in energy of the particle. The lost energy is emitted as an X-ray (Figure 1.5):
Chapter 1 Introduction 7131060
37
Figure 1.5: Emission of Bremsstrahlung
This process is favoured for high energy electrons and high atomic number, (Z), stopping
materials. The emitted X-ray has an energy range from near zero to the energy of the
incident electron and is equal to the energy lost by the particle as it is decelerated. The X-ray
does not produce excitation or ionisation unless it subsequently interacts with the medium.
If the initial electron energy is below 100 keV, then Bremsstrahlung emission is negligible.
Lower energy electrons (such as negatrons) lose their energy predominantly by inelastic
collisions with the medium and may also undergo elastic scattering, where they are
deflected by the Coulomb field of the atomic nucleus. Eventually they will be absorbed by
the medium.
The positron is an antiparticle of an electron and is short lived; undergoing positron
annihilation (Figure 1.6). During annihilation, two electron masses are converted to
electromagnetic radiation. The kinetic energy of the particles is near zero and so the total
energy of the annihilation process is 1.02 MeV. This value is two times the value of the
equivalent electron mass (511 keV):
Chapter 1 Introduction 7131060
38
Figure 1.6: Positron annihilation
In order to conserve momentum, the photons are emitted 180 Β° to each other.
During Ξ² and Ξ³ decay, and following collisions and ionisation of a core electron, electrons
may be emitted that have distinct energies. These monoenergetic electrons are known as
conversion electrons and Auger electrons. Conversion electrons may accompany gamma ray
emission from the nucleus. The gamma ray can interact with atomic electrons and be
absorbed which gives the electron enough energy to be ejected. The energy of a conversion
electron is the energy of the gamma ray minus the binding energy of the electron in the
atom.
Auger electrons originate from electron rearrangement. After electron capture or ionisation
of a core electron occurs, there is a core electron vacancy that is immediately filled by an
electron from an outer orbital. This electron rearrangement means there is excess energy in
the system which can either be lost by X-ray emission or the emission of another electron
from the atom (an Auger electron). If an Auger electron is emitted, a vacancy is created
which is then filled by another electron from an outer orbital. This can lead to an electron
cascade unless an X-ray is emitted (Figure 1.7). If an electron cascade does occur, this will
Chapter 1 Introduction 7131060
39
lead to a highly charged species which will eventually capture electrons from the
surroundings to create a stable species.
Figure 1.7: Overview of Auger electron emission
Electromagnetic Radiation
There are 4 main processes by which Ξ³-rays interact with matter:
coherent (Rayleigh) scattering;
photoelectric effect;
Compton scattering; and
pair production
The latter three are the most important in radiation chemistry and depend greatly on the
photon energy and the atomic number of the stopping material as is shown in Figure 1.8:
Chapter 1 Introduction 7131060
40
Figure 1.8: Ξ³-ray interaction processes and their dependence on photon energy and Z of medium (replicated from [13])
Photons can scatter with little loss of energy when they are absorbed and re-emitted by
atomic electrons; this is coherent scattering and is most likely to take place when the
photons have low energies (< 0.1 MeV) and high atomic number materials. It occurs when
the probability for the photoelectric effect to take place is large. It is often neglected
because the small angle of scatter makes these photons hard to differentiate from the main
beam of photons unless a narrow beam is used.
Photoelectric effect: This is predominant for low energy photons. The process involves the
entire energy of an incident photon (πΈπ) being transferred to a single atomic electron which
is then ejected from the atom with energy (πΈπΈ) equal to the difference between the incident
energy and the binding energy of the electron in the atom (πΈπ).
At lower photon energies, the electron is ejected close to 90 Β° from the incident beam. As
photon energy increases, the ejection angle gets smaller and the electron is ejected in the
same direction as the beam (Figure 1.9):
0
20
40
60
80
100
120
0.01 0.1 1 10 100
Z o
f m
ediu
m
hΞ½ / MeV
photoelectric effect
Compton effect
pair production
Chapter 1 Introduction 7131060
41
i) ii)
Figure 1.9: The photoelectric effect at i) low photon energies and ii) high photon energies
Energy and momentum are conserved by recoil of the remaining atom.
Compton scattering: This occurs when a photon is scattered by interaction with an electron.
This interaction leads to the acceleration of the electron and scattering of the photon with
less energy. The energy and momentum of the incident photon is shared between the
scattered photon and the recoiling electron (Figure 1.10):
Figure 1.10: Compton scattering
The more the photon is scattered (i.e. greater ΞΈ value), the larger the amount of energy
transferred to the electron. The energy of the recoil electron is equal to the incident photon
energy minus the energy of the scattered photon.
Ξ
Chapter 1 Introduction 7131060
42
The energy of the recoiling electron has a range from zero to a maximum which can be
calculated by assuming the photon scatter angle is 180 Β° (i.e. photon rebounds off the
electron). The most probable values for πΈπΈ are those near zero or the maximum energies
(maximum energy is favoured if πΈπ is high). The direction of the recoil electron follows the
initial incident photon path when more of the energy is transferred from the photon to the
electron.
Pair production: This occurs when a photon is completely absorbed in the vicinity of an
atomic nucleus (or less frequently, an electron). This absorption produces two particles: an
electron and a positron. The energy of the photon is shared between the kinetic energy of
the electron and positron minus the rest energy of the two particles (both equivalent,
therefore both πππ2). A small almost negligible amount of energy is transferred to the
nucleus. The momentum is shared by the recoiling nucleus and the emitted particles. The
positron is slowed down similar to an electron and eventually undergoes positron
annihilation (Figure 1.6). The overall process is shown in Figure 1.11:
Chapter 1 Introduction 7131060
43
Figure 1.11: Pair production followed by positron annihilation
Pair production can only occur if the incident photon has greater energy than 1.02 MeV (the
rest mass of the two particles).
Another process that occurs with photons is photonuclear reactions. This process requires
very high energy photons which are not utilised as part of this research
Electromagnetic radiation can lose relatively large amounts of its energy in a few
interactions with matter, however, only a fraction of Ξ³-rays are absorbed by the medium
with the rest being transmitted through with the same incident energy. The total linear
attenuation coefficient is given by Equation 1.3:
π = π + π + π Equation 1.3
where π, π and π are the linear attenuation coefficients (in cm-1) for the photoelectric,
Compton and pair production processes respectively. Their values are constant for a given
photon energy and a given stopping material [12].
A further type of radiation that may occur in radioactive systems is neutron radiation. These
are not utilised in this research, therefore are not detailed in this thesis.
Chapter 1 Introduction 7131060
44
1.2.3 Radiolytic Track Formation
When a charged particle or photon interacts with matter, it gives rise to a track of ionised
and excited species. The nature of the species will be identical for a given medium
irrespective of the type of radiation utilised. Different types of radiation lose energy at
different rates. The concentration of the ionised and excited species will differ and the
length of the track will differ. This non-homogeneous concentration profile in turn leads to a
difference in observed chemical effects for differing types of radiation, especially for liquid
and solid media. For example, π»2 production from the radiolysis of an aqueous solution
containing potassium nitrate (πΎππ3) and nitrous oxide (ππ), is two and a half times greater
using 12 MeV π»π2+ ions compared to 60πΆπ Ξ³-rays [14]. In gaseous media, where the density
is much lower, the effect is less prominent. The formation of ethane (πΆ2π»6) from radiolysis
of methane (πΆπ»4), is not greatly affected by using either Ξ³-rays from spent fuel elements or
2.8 MeV electron beams [15, 16].
Along with the primary charged particle or photon, ejected electrons (termed secondary
electrons) may also cause ionisation and excitation within the medium. If the secondary
electron has less than 100 eV of energy, then its range will be short and lead to secondary
ionisation events close to the primary track and give rise to a cluster or βspurβ of
ionisation/excitation events. If the electrons have energies larger than 100 eV, however,
then their range increases and can lead to extended secondary tracks of ionised/excited
species. Figure 1.12 shows a comparison of track structure from an Ξ± particle and a fast
electron. These tracks only persist for a short period of time before dissipating in the
medium.
Chapter 1 Introduction 7131060
45
Figure 1.12: Radiolytic track structure of i) Ξ± particle and ii) fast electron
The amount of chemical change a medium undergoes when interacting with ionising
radiation depends both on the total energy of the radiation and the rate at which its energy
is deposited. The first factor will determine the yield of reactive species and the second
factor, their proximity. Linear Energy Transfer (LET) is a term used in radiation chemistry to
parameterise these factors. It is defined as the rate of energy loss by an ionising particle or
photon traversing a medium (Equation 1.4). The most common units are keV Β΅m-1:
πΏπΈπ = ππΈ
ππ Equation 1.4
where ππΈ is the change in particle energy and ππ is the path length of the particle.
Equation 1.4 does not take into consideration the fact that the rate of energy loss decreases
as the particle slows down and loses energy. Furthermore, it does not reflect the fact that
secondary ionisation/excitation events may take place away from the primary track. For a
given energy, photons and high energy electrons have the lowest LET due to the fact they
have a high penetration (ππ) but deposit only a small quantity of energy. In contrast, Ξ±
i)
ii)
Chapter 1 Introduction 7131060
46
particles and fission fragments have the highest LET as they have low penetration and
deposit the majority of their energy in a single collision.
To denote yields in radiation chemistry, the term G-value is used throughout journals and
texts. It has the following symbol G(Β±π₯) and represents the number of molecules of species
π₯, either lost or produced in the system per 100 eV of energy deposited in the said system.
Chapter 2 Literature Review 7131060
47
2 Literature Review
This chapter gives a review of the work previously undertaken in this area of research. This
review includes the limited data available with respect to plutonium storage canisters and
possible mechanisms occurring inside during storage. Focus is given to one such mechanism;
the radiolysis of adsorbed moisture and subsequent gas phase radiation chemistry. With
respect to storage of plutonium-bearing materials in the UK, attention is given to the
radiolysis of air in the presence of an oxide surface. Finally, this chapter outlines the aims
and objectives this research hopes to achieve and how the knowledge base may be
enhanced.
2.1 π·ππΆπ Storage Canisters
A substantial amount of work has been undertaken by the Los Alamos National Laboratory
(LANL) with regards to hazards associated with long term storage of ππ’π2. Eller et al. have
investigated the pressurisation of ππ’π2 storage canisters and have hypothesised four
possible mechanisms that could lead to pressurisation [17], these are:
thermal heating;
helium accumulation from radioactive decay;
radiolytic and chemical degradation; and
radiolysis of adsorbed moisture
The centre line temperature in ππ’π2 storage canisters can be several hundred Β°C, this can
lead to pressurisation of the gas phase. Eller et al. used a computer model to predict the
temperature of the gas phase from this centre-line temperature. The model predicted that
Chapter 2 Literature Review 7131060
48
the gas phase would increase in temperature from ambient to 211 Β°C once ππ’π2 had been
added to the canisters. This temperature increase would lead to an increase in pressure
from 14 psi to 23 psi. This mechanism was discounted, as this increase in pressure would be
visible after several weeks of storage.
The Ξ±-decay of plutonium could lead to helium accumulation inside the canisters. It was
predicted that the pressure inside the canister would increase by 13 psi over a period of 50
years of storage for a canister containing 5 kg of ππ’π2. However, this value is an over-
estimation as helium would be trapped in the solid matrix [18].
Chapter One outlined the finishing process for ππ’π2, which involved calcination at high
temperatures, this process would remove any organics from the product. No signs of
corrosion in the canisters further highlight the absence of organics.
The final mechanism discussed was that of radiolysis of adsorbed moisture. Before going
into storage the moisture content is kept below 0.5 wt.%. This quantity is insufficient to
generate significant pressurisation, however, it could lead to the formation of π»2 and π2 gas
atmospheres.
A fifth mechanism was postulated by Paffett and Bailey [19] which is a pressure pulse from
the deflagration or detonation of a combustible atmosphere. This mechanism ties in with
the radiolysis of moisture outlined by Eller et al.
Mason et al. carried out headspace gas analysis of ten sealed ππ’π2 storage canisters that
had come from a range of sources with varying purities and had been stored for various
timescales (1-18 y) [20]. From these analyses, several observations were noted. Even though
the canisters were not airtight, eight of the canistersβ had an internal pressure that was less
Chapter 2 Literature Review 7131060
49
than the atmospheric pressure of the site where they had been stored. Analysis of the gas
phase indicated that the main component was air, with only two samples having significant
concentrations of π»2. The final observation stated that canisters where π2 was present had
no π»2 present and vice-versa.
Almond et al. performed gas analysis on over thirty containers of plutonium bearing
materials from the Hanford and Rocky Flats sites that had been stored for 4-6 y [21]. They
found that seven of the containers had more than 0.1 mol% π»2 and very little π2 in the
resulting headspace. The other twenty four containers did not have a sizeable amount of π»2
present although four of these containers had a moisture content of β₯ 0.1%, which is within
the range for anticipated π»2 production.
From these references, it is clear that radiolysis of adsorbed moisture is the main
mechanism of pressurisation inside ππ’π2 storage containers. Therefore knowledge of how
this water adsorbs and the mechanisms leading to π»2 and π2 generation are important.
Chapter 2 Literature Review 7131060
50
2.2 Water Adsorption on π·ππΆπ
Stakebake has postulated that water adsorption to a ππ’π2 surface occurs in three steps
[22], which are shown pictorially in Figure 2.1.
Figure 2.1: Postulated mechanism of water adsorption onto a ππ’π2 surface (replicated from [22])
The first step involves bonding between the plutonium cation and the oxygen from water.
This step allows hydrogen bonding between the hydrogen atoms from water and the oxygen
atoms neighbouring the plutonium cation. This interaction leads to dissociation of the water
molecule into hydroxyl groups that become chemisorbed to the surface. The second step
involves interaction between the chemisorbed hydroxyl groups and unbound water. This
interaction may be mono or bi-dentate and is termed quasi-chemisorption [23]. The final
step is the physisorption of unbound water to the quasi-chemisorbed water molecules. This
+ H2O
+ 2H2O
Step 1
Step 2
Step 3
Chapter 2 Literature Review 7131060
51
final adsorption is very weak as there is no formal bond between the adsorbate and the
surface. It is not known what effect (if any) the oxide surface plays in this final step.
During calcination, it is likely that only the chemisorbed water will remain attached to the
surface, unless very high temperatures are used.
Haschke and Ricketts [23] have determined the mass of this chemisorbed monolayer of
water on ππ’π2. They have determined values between 0.21-0.24 mg m-2 depending on the
crystal plane and assuming association of one water molecule to one plutonium atom.
Work by Alexandrov et al. showed that this mechanism was also true for thorium dioxide
(πβπ2) and cerium dioxide (πΆππ2), which are often used as surrogates for ππ’π2 and heavy
actinide oxides [24].
From the mechanism outlined above, it is clear, that adsorbed species play a role in the
adsorption of further water molecules. This mechanism follows the BET theory of the
formation of multi-layers on a surface as opposed to the Langmuir theory that assumes
once a monolayer of molecules has been adsorbed there will be no further adsorption to
the surface as all the active sites have been filled.
2.3 Radiolysis of Adsorbed Water
Petrik et al. have investigated the Ξ³-irradiation of adsorbed water on several metal oxides to
determine the quantity of π»2 produced [25]. Their work classified oxides into three groups.
The first group had a lower yield (G-value) of π»2 than radiolysis of liquid water (G(π»2) = 0.45
molecules 100 eV-1 [26]). The second group had G(π»2) values close to bulk water radiolysis
and the final group have a higher G(π»2) value than bulk water. It is postulated that the
Chapter 2 Literature Review 7131060
52
increase in π»2 formation is due to an enhanced energy transfer between the oxide surface
and the adsorbed water. They highlighted a resonance between the band gap of the oxide
and the bond dissociation energy of water (5.15 eV [27]) The band gap is the energy needed
by electrons to move from the highest occupied band (valence band) to the lowest
unoccupied band (conduction band). Metal oxides that had a band gap or approximately
5 eV produced the greatest quantity of π»2.
Aleksandrov et al. highlighted that physisorbed water and surface hydroxyls had a negligible
contribution to π»2 yield during radiolysis of adsorbed water [28]. They found that the
energy adsorbed by the oxide was transferred entirely to the first layer of chemisorbed
water. They determined that the active layer of the oxide involved in the heterogeneous
system was no more than 100 nm thick.
LaVerne and Tandon investigated π»2 production from πΆππ2 and πππ2 using cobalt-60
gamma rays [29] and determined that π»2 yield increased with decreasing numbers of water
monolayers adsorbed to the surface. G(π»2) values of 20 and 150 molecules 100 eV-1 were
determined for samples containing πΆππ2 and πππ2, respectively.
2.4 Radiolysis of Gases in Contact with π·ππΆπ
An extensive amount of research has been undertaken on the radiolysis of adsorbed species
(e.g. water, nitrates) on ππ’π2 and other oxides. However, there are fewer publications on
gas phase radiolysis or gases as part of a heterogeneous system. A lot of the emphasis is on
post irradiation analysis of gases from either solutions or organics. However, some papers
have tried to rectify this.
Chapter 2 Literature Review 7131060
53
Haschke et al. exposed ππ’π2 to a 2:1 π»2 β π2 mixture and measured the pressure as a
function of time [30]. They reported a rapid drop in pressure before eventually (after 72 d)
staying constant. Mass spectrometer data from the gas phase found no water vapour
present even though mixtures of π»2 β π2 are thermodynamically unstable relative to water.
The results suggested there were two reactions occurring simultaneously. These are the
oxide catalysed recombination of π»2 and π2 (Reaction 2.1) and the subsequent water
catalysed oxidation of ππ’π2 (Reaction 2.2) to form the super-stoichiometric plutonium
dioxide, ππ’π2+π₯:
2π»2 + π2 + ππ’π2 β 2π»2π + ππ’π2 Reaction 2.1
ππ’π2 + π2 + π»2π β ππ’π2+π₯ + (1 β π₯)π2 + π»2π Reaction 2.2
The conclusion of this work was that ππ’π2 is a catalytically active metal that promotes the
formation of ππ’π2+π₯ below 200 Β°C.
It has been reported by others that π»2 and π2 are not produced stoichiometrically from the
radiolysis of absorbed water [31]. Headspace analysis from canisters that have been stored
for over twenty years show that π2 levels are depleted whilst π»2 levels are enriched,
although there is no overpressure. This is further evidence of the formation of the super-
stoichiometric oxide.
Subsequent work by Haschke et al. surmised that the system pressure decreases as ππ’π2+π₯
is formed at a constant rate by Reaction 2.2 [32]. Once π2 is depleted, formation of π»2 from
the radiolysis of the adsorbed water causes the pressure to increase. Therefore
pressurisation is possible over long periods if there is constant moisture adsorbed on the
oxide surface.
Chapter 2 Literature Review 7131060
54
Morales et al. also concluded that ππ’π2 acted as a catalyst for π»2 and π2 recombination
[33]. Their results showed that stoichiometric amounts of π»2 and π2 were lost from the gas
phase and the total pressure of the system decreased after the reactants had combined.
Like Haschke, water vapour was not observed in the final gas composition, suggesting that
any water formed is adsorbed to the surface of the oxide. Initially, the active sites on the
ππ’π2 are free and so can act as a catalyst in the reaction between π»2 and π2; this is
supported by the initial drop in pressure of the system. Eventually, these sites become
blocked by water molecules and ππ» moieties and so the reaction rate decreases. At
temperatures above 100 Β°C, there is enough thermal energy for these sites to be
regenerated thus the rate increases. The implication of this mechanism is that the reaction
is driven by surface catalysis and not by radiolytic formation of radicals. The establishment
of a steady state pressure indicates that the rate of recombination of π»2 and π2 is equal to
the rate of radiolysis of absorbed water.
Several papers have hypothesised about the production of the super-stoichiometric ππ’π2+π₯
from the reaction of ππ’π2 with water and π»2 β π2 mixtures. The mechanisms for this are
not fully understood and the fact that oxidation of ππ’π2 in π2 does not generate ππ’π2+π₯,
only with the presence of water does it occur, makes the mechanism more complex [34].
Korzhavyi et al. have proposed that the lack of observed oxygen by Haschke et al. [30, 32] is
potentially due to the formation of a more stable product than ππ’π2+π₯ , possibly a hydroxide
or peroxide compound of plutonium [34]. However more experimental data is needed.
Chapter 2 Literature Review 7131060
55
2.5 Radiolysis of π―π β πΆπ in Contact with Other Materials
Further papers have looked at the recombination rates of π»2 and π2 over different
materials in the absence of radiation. Quigley looked at the recombination rates over
several materials including stainless steel, strips of tin and πΆππ2 [35]. This was to address
the issue of over-pressurisation in stainless steel canisters relevant to nuclear waste storage.
Experiments carried out at 200 Β°C and 300 Β°C highlighted that πΆππ2 was by far the most
efficient at removing π»2 and π2 from the gas phase. Results for stainless steel also showed
that it acts as a catalyst for the recombination. The tin strips however became oxidised and
so were not as efficient in the recombination process.
Katz studied the reaction of π»2 and π2 in the presence of concrete that incorporated
simulated radioactive waste [36]. Their results revealed concrete that had been prepared at
higher temperatures and pressures (cured for 24 hrs at 100-250 Β°C below 600 psi) had a
higher recombination rate than the rate of gas production from radiolysis of water in the
system.
From the work already carried out, it is clear that the presence of a surface increases the
rate of π»2 β π2 recombination. However, different surfaces whether an oxide, cement or
steel all have the same effect; therefore more work on understanding the mechanism of
recombination is needed. Several papers also suggest the formation of the super-
stoichiometric ππ’π2+π₯, however, only in the presence of moisture. Work on other oxides
such as πΆππ2, should help to enhance the understanding of its formation.
Chapter 2 Literature Review 7131060
56
2.6 Radiolysis of Hydrogen and Oxygen
A significant quantity of work was undertaken by Lind and co-workers, who investigated the
recombination of π»2 and π2 using radium powder as a radiation source [37]. Only pressure
was measured and several assumptions were made, including that no steady state was
reached, radium had no catalytic effect on the system and the only reaction occurring is
Reaction 2.1 (π instead of ππ’π2). In earlier work, the π
π term was utilised instead of G-
values, where π is the number of molecules undergoing change (formed or reacted) and π
is the number of ion pairs formed. These values can be converted to G- values using
Equation 2.1.
πΊ = π
π 100
π Equation 2.1
where π, is the mean energy required to form an ion pair. A lot of early works use the value
for air which is 32.5 eV, therefore:
πΊ = 3π
π Equation 2.2
Lind et al. calculated G(π»2π) values of 11.76 molecules 100 eV-1. Further work investigating
the effect of added water vapour hypothesised that at ambient temperatures, water vapour
condenses on the vessel walls and plays no part in gas phase reactions, but at higher
temperatures, contributes significantly to the ionisation and reaction rates [38]. Work
replacing π»2 with deuterium, π·2, found that the recombination rate was approximately 25-
30% slower in comparison to π»2 β π2 recombination [39]. The discussion centred around a
lower efficiency in one of the preliminary reaction steps.
Benjamin and Isbin investigated π»2 β π2 recombination at high temperatures, of interest to
boiling water reactors [40]. They calculated G(-π»2) values in the range 3-6 molecules
Chapter 2 Literature Review 7131060
57
100 eV-1 and the rate of recombination was independent of temperature up to 138 Β°C. They
postulated that the reaction was first order in π»2 concentration, however, this statement
needs further clarification as to whether the effect the concentration has on absorbed dose
has been taken into account. Like Schifflett et al. [38], their data highlights the rate of
recombination is independent of water vapour concentration.
Dautzenberg irradiated mixtures of π»2 β π2 using gamma radiation and investigated the
effects of pressure, temperature and matrix gases on the reactivity of π»2 β π2 mixtures
[41]. He found that the G(-π»2) value was affected by all these parameters and achieved
values in the range of 5.5-160 molecules 100 eV-1, depending on reaction conditions. Unlike
Benjamin et al. [40], Dautzenberg determined that the rate of recombination was
independent of π»2 β π2 ratio. Furthermore, he found that pre-treating the reaction vessels
also had an effect. By heat treating the vessels at 500 Β°C for 24 hrs and then out-gassing
under vacuum at 200 Β°C for 30 min, he noted that the G(-π»2) value decreased. He surmised
that this was due to surface impurities helping the recombination of π»2 β π2 and so using a
βcleanβ surface decreased the reaction rate. Dautzenberg also proposed that the reaction
occurred by a radical chain scheme.
Summary
From the literature reviewed in the previous sections, it is clear that radiolysis of adsorbed
moisture is the primary mechanism by which ππ’π2 storage canisters can pressurise. A lot of
work has been undertaken on this system, and with other materials, however, there is much
debate as to a mechanism for the enhancement of π»2 yields.
Chapter 2 Literature Review 7131060
58
Early work has investigated the gas phase recombination of π»2 β π2, however there is a
broad range of G(-π»2) values quoted in the literature, there are also conflicting results as to
the order of the recombination.
There has been very little published literature on the radiation chemistry of gaseous species
in contact with an oxide surface (ππ’π2 or otherwise). Hopefully this research will help to
add to this area.
2.7 Air Radiolysis
Chapter One outlined the storage conditions for ππ’π2 in the UK. In one of the product
streams, the fill gas is a 50:50 mixture of air and argon. Irradiation of air could lead to
further chemistry occurring in the canisters, therefore an understanding of the radiation
chemistry of air is needed.
Willis et al. have investigated the radiolysis of π2 β π2 mixtures utilising electron pulses
[42]. They found ozone, π3, to be the dominant product. With nitrogen dioxide, ππ2, being
below the limits of detection.
Harteck and Dondes outlined the following reaction mechanism for radiolysis of air [43, 44]:
π2 β 2π Reaction 2.3
π2 β 2π Reaction 2.4
π + π2 β π + ππ Reaction 2.5
2ππ + π2 β 2ππ2 Reaction 2.6
Chapter 2 Literature Review 7131060
59
π + ππ2 β 2ππ Reaction 2.7
π + ππ2 β π + π2π Reaction 2.8
π + ππ β π + π2 Reaction 2.9
π + π2 + π β π3 Reaction 2.10
From this mechanism, it is clear that the dominant products are π3, π2π and ππ2.
In the presence of moisture, the dominant product is nitric acid (π»ππ3), (Reactions 2.11
and 2.12) [45, 46].
2ππ2 + π»2π β π»ππ3 + π»ππ2 Reaction 2.11
2π»ππ2 β ππ + ππ2 + π»2π Reaction 2.12
Kanda et al. measured G(π»ππ3 ) values of 1.46 molecules 100 eV-1 by irradiating
atmospheric air using a cyclotron radiation source [45]. Jones measured G(π»ππ3) values of
1.2 molecules 100 eV-1 and found that nitric acid disappeared on exhaustion of water
vapour in the system leading to formation of stoichiometric amounts of ππ2 and water [46].
This reformed water did not lead to further nitric acid formation.
Summary
The radiolysis of air is a well understood system and the dominant products are well known.
In the presence of moisture, nitric acid is the dominant product. Previous sections in this
chapter outlined that water would be present in the ππ’π2 storage canisters, therefore the
formation of nitric acid is a concern.
Chapter 2 Literature Review 7131060
60
There has been no attention given to the formation of nitric acid from radiolysis of air in the
presence of an oxide material. This research hopes to address this issue.
Aims and Objectives
In light of the findings of this literature review, the aim of this research project is to study
the gas phase radiation chemistry of two gaseous systems in the presence or absence of a
ππ’π2 surrogate material. These systems are firstly, mixtures of π»2 β π2 in an π΄π matrix and
secondly, moist air.
These aims were pursued via the following distinct objectives which are summarised below:
Develop an adequate reaction vessel to investigate the recombination of π»2 and π2
in homogeneous and heterogeneous systems using a 60πΆπ Ξ³ source
Determine a better mechanistic understanding of the π»2 β π2 system, and what role
an oxide surface may play in this system
Investigate the radiolysis of air in the presence of a ππ’π2 surrogate material and
determine the identity and yield of species produced
Determine the role an oxide surface plays (if any) in the radiation chemistry of air
Investigate both gaseous systems utilising a beam of accelerated 5.5 MeV π»π2+ ions
to simulate the Ξ±-decay of 238ππ’, which is the Ξ± emitter with the shortest half-life
(87.7 y) in the storage canisters
Chapter 3 Experimental 7131060
61
3 Experimental
The following chapter outlines the materials necessary to carry out this research and the
irradiation facilities used to perform the work. It also details the experimental techniques
utilised to execute this work. Finally, it details the experimental methodologies employed
during the course of this research.
3.1 Materials
3.1.1 Gases
All gases are supplied by BOC unless otherwise stated. Hydrogen (CP Grade 99.999%),
oxygen (N5.0 99.999%) and argon (Zero grade 99.999%) are utilised for the preparation of
known concentrations of gas mixtures used to carry out part of this research. Synthetic air
(supplied by BOC) is used during this research and is produced by mixing 20% π2 with 80%
π2. The impurities are certified as < 1 vppm πΆπ2, < 2 vppm π»2π and < 0.1 vppm πππ₯.
Calibration gases for the gas chromatograph are supplied by Scientific and Technical Gases
in lecture bottle size. Mixtures ranging from 5% π»2 π΄πβ down to 0.1% π»2 π΄πβ are used for
the calibration of the gas chromatograph. Each bottle has an accuracy of Β±0.1%.
3.1.2 Chemicals
Cerium oxide (πΆππ2) is purchased from Alfa Aesar in the form of a 14 Β΅m powder with
99.99% purity; the largest impurity is β€ 0.1% silicon dioxide (πππ2). Zirconium oxide (πππ2) is
also purchased from Alfa Aesar and has a more crystalline powder form than πΆππ2. It is
supplied as 99.978% pure and the largest impurity is certified as 29 ppm of tantalum and
9 ppm of hafnium. Cerium oxalate hydrate (πΆπ2(πΆ2π4)3. π₯π»2π), which is used for TGA
Chapter 3 Experimental 7131060
62
analysis, has a purity of 99.9% trace metals, and sodium hydroxide (reagent grade β₯ 98%)
(ππππ») which was utilised in the post irradiation analysis of the air radiolysis experiments
were both supplied by Sigma-Aldrich.
3.2 Irradiation Sources
Two sources of ionising radiation are used to induce a chemical change in the systems of
interest; 60πΆπ Ξ³ β rays and π»π2+ ions. The following section details how these sources are
used.
3.2.1 Cobalt-60 Source
A Foss Therapy Model 812 self-shielded irradiation source is utilised to perform gamma
irradiations. Figure 3.1 shows the 9 L irradiation chamber which is able to house a wide
range of samples. The irradiator has three source rods located at the front of the chamber,
however, only the two outer source rods have pellets of cobalt-60 inside. The irradiator is
capable of delivering a dose rate between 400 and 4 Gy min-1 depending on attenuation and
distance from the sources.
Figure 3.1: Foss Therapy Model 812 60πΆπ Irradiation source
Chapter 3 Experimental 7131060
63
The decay scheme for 60πΆπ is shown in Figure 3.2. There are two distinct types of radiation
emitted from the source, these are Ξ² and Ξ³, however, due to the stainless steel shielding,
the Ξ² particles will not penetrate through the source rods. Only the two Ξ³ emissions of 1.17
and 1.33 MeV contribute to the radiation chemical affect.
Figure 3.2: Decay scheme for cobalt-60 isotopes
The irradiator is controlled by computer, which can set irradiations to last for a desired time
or absorbed dose.
Due to the nature of the sample chamber and the location of the source rods, the dose rate
within the chamber can differ substantially due to the inverse square law.
πππ‘πππ ππ‘π¦ β 1
πππ π‘ππππ2 Equation 3.1
For this reason, precise dosimetry is required to assess the dose rate of a given position
within the chamber. This topic is discussed further in Chapter Five.
Chapter 3 Experimental 7131060
64
3.2.2 Pelletron Ion Accelerator
An NEC 5 MV tandem ion accelerator is utilised to perform ion irradiation studies on the
gaseous systems relevant to this research. The accelerator is capable of delivering a beam of
positive ions of light charged particles (π»+ and π»π2+) up to energies of 10 and 15 MeV
respectively. It is also a source of heavy charged particles of many elements within the
periodic table. Samples are placed at the end of one of the acceleratorβs six beam lines
where irradiations and/or analysis can be carried out in-situ. In this research, π»π2+ ions will
be used to simulate the Ξ± decay of ππ’π2 (specifically plutonium-238). Ions are generated by
feeding π»π gas into a Toroidal Volume Ion Source (TORVIS). A current is placed over a
filament to ionise the gas and form π»π+ ions. These ions are passed through a rubidium
vapour to add electrons forming π»πβ and π»π2β. The negative ions are accelerated to
ground and stripped of electrons to form positive ions which are accelerated from ground,
down the appropriate beam line to the sample. Figure 3.3 shows a schematic layout of the
accelerator. From left to right, the ions are generated at the source, accelerated into the
tank, converted to positive ions and accelerated down one of the beam lines.
Figure 3.3: Schematic of 5 MV Ion accelerator located at DCF
Chapter 3 Experimental 7131060
65
3.3 Analytical Techniques
The two primary analytical techniques utilised in this research are gas chromatography (GC)
and ion chromatography (IC). GC is used to determine the concentrations of π»2 and π2 in
the gas phase throughout this research. IC is primarily used to determine the concentration
of nitrate (ππ3β) anions in air radiolysis experiments, however, other anions can be detected
in parallel. Chromatography is a separation technique reliant on both a stationary phase
that is immobilised on a solid support and a mobile phase that pushes the analyte through
the stationary phase before separating the components of a mixture using a particular
property [47]. Other techniques are applied to study the solid phase during this research,
however, focus will be given to the two primary techniques named above.
3.3.1 Gas Chromatography (GC)
The GC used in this research is an SRI Instruments Multiple gas analyser #1, equipped with a
thermal conductivity detector (TCD) which can be used to detect molecular gaseous species
such as π»2, π2 and π2. The detector uses a set of filaments in a Wheatstone bridge
configuration to detect analytes which have a different thermal conductivity to the
reference gas flow. The stationary phase is a 6 ft. long, 1/8 β diameter packed column of
molecular sieve 13X beads. This column is particularly useful as it acts as a trap for moisture
which would subsequently interfere with the resulting chromatogram. The GC is also
equipped with a 10-port sampling valve which allows for switching between loading and
injecting positions and has a 50 ΞΌl sample loop attached. The mobile phase is high purity
argon (99.999% pure), specifically chosen to increase the sensitivity of the instrument
towards π»2 measurements due to the differing thermal conductivities of π΄π and π»2. The
instrument conditions are as follows: the carrier gas flow rate is set at 28 psi, thus allowing
Chapter 3 Experimental 7131060
66
for measurements to be acquired in several minutes; the valve temperature is 60 Β°C, the
oven temperature which houses the column is set at 80 Β°C and the detector is at 130 Β°C.
These conditions allowed for good separation of analytes without shortening the lifespan of
the instrument.
3.3.2 Ion Chromatography (IC)
The IC used in this research is a Thermo-Scientific ICS2100, consisting of an electrochemical
detector (ECD) and a Dionex Ion Pac AS-18 column. The stationary phase is composed of an
ion exchange resin in the form of 4 ΞΌm beads which are packed into the column. The mobile
phase is a potassium hydroxide (πΎππ») eluent which is made from an eluent generator to
tailor the concentration of ππ»β to the application. This setup allows for the determination
of inorganic anions and low molecular weight organic acids.
The instrument conditions are: column temperature 30 Β°C, πΎππ» eluent concentration
23 mM with a flow rate of 0.25 ml min-1. The injection volume for each sample is 0.25 ΞΌl.
These conditions allowed for analysis times of ten minutes for each sample. For large
numbers of samples, an auto sampler is used to increase efficiency.
3.3.3 Surface Area Measurements
To determine the surface area of the oxide powders of interest, a Tri-Star II surface area and
porosity analyser supplied by Micromeritics is used. It is important to know the specific
surface area (SSA) of the oxide powders as this may help to elucidate any catalytic affect the
surface may have on gas phase radiolysis. In all the experiments, π2 is used as the adsorbate
gas. Surface area is calculated using the BET theory and the following equation:
ππ΄π΅πΈπ = (π£πNAπ
ππ) Equation 3.2
Chapter 3 Experimental 7131060
67
where π£π is the volume of 1 monolayer of adsorbed gas, NA is Avogadroβs constant, π is the
cross sectional area of the gas adsorbate (for π2 this is 0.162 nm2) and ππ is the molar
volume of the adsorbate gas [48]. This value is then divided by the sample mass to calculate
the surface area in units of m2 g-1. Sample masses are in the range of 0.5-1 g before being
de-gassed under vacuum at 250 Β°C overnight. The samples are re-weighed and analysis
performed.
3.3.4 Thermogravimetric Analysis (TGA)
To determine whether there are any organic impurities absorbed on the oxide powders and
to investigate their thermal stabilities, samples were submitted for thermogravimetric
analysis. TGA involves heating a small amount of sample at a set heating rate and measuring
the difference in mass over a required temperature range. To carry out TGA, a small mass of
sample (< 10 mg) is placed inside an aluminium crucible and heated. For samples of πΆππ2
and πππ2, the heating rate employed is 10 Β°C min-1, heated up to 1000 Β°C and held for
10 min. A sample of cerium oxalate was also analysed, however, due to the decomposition
of the sample, a heating rate of 2 Β°C min-1 is employed and the sample is heated to 600 Β°C.
This temperature ensures the oxalate has decomposed fully. All samples are analysed in
both static air and nitrogen to provide a comparison between oxidative and inert
atmospheres.
3.3.5 Diffuse Reflectance Infra-red Spectroscopy (DRIFT)
A Vertex 70 FT-infra-red spectroscope supplied by Bruker is used to investigate the surface
of the oxide powders with respect to adsorbed organic species. A Praying Mantis diffuse
reflectance accessory is used to increase the spectral output due to the uneven nature of
the sample surface. The accessory has two parabolic mirrors to collect all of the reflected
Chapter 3 Experimental 7131060
68
light off the sample and focus it into the detector. A mercury cadmium telluride (π»ππΆπππ)
detector, which is cooled with liquid nitrogen to improve signal/noise ratio is used. The
resolution is set to 4 cm-1 and 250 scans of each sample are taken.
3.3.6 UV-Vis Spectroscopy
To perform Fricke dosimetry experiments, an Agilent Technologies Cary Series UV-Vis-NIR
spectrophotometer is utilised. Disposable 1 cm path length cuvettes are used to analyse the
solution and three repeats of each sample are taken. An average of these readings is used as
the absorption value compared to a reference blank.
3.3.7 Scanning Electron Microscopy (SEM)
To determine the morphology of the oxide grains, a small quantity of powder is mounted
onto a carbon stub and coated with a fine layer of carbon using a Cressington 208 high
vacuum carbon coater. The samples are loaded into the chamber of a JEOL 6400 scanning
electron microscope. The instrument is equipped with a Princeton Gamma Tech energy
dispersive X-ray spectroscope (EDS) which allows for elemental analysis of the sample to be
investigated. The beam energy used is 15 keV.
Chapter 3 Experimental 7131060
69
3.4 Experimental
The following section outlines how this research is carried out, detailing the equipment
needed to mix various gases together and how the air radiolysis experiments are
accomplished. Finally, details of experiments carried out using the ion accelerator are
explained.
3.4.1 Mixing of π―π β πΆπ β π¨π Samples
A bespoke manifold system has been designed and commissioned to be able to mix π»2, π2
and argon gas in various concentrations. Figure 3.4 shows a visual image of the manifold
and a schematic drawing showing its design features.
Chapter 3 Experimental 7131060
70
Figure 3.4: Bespoke gas mixing manifold system
The manifold is made from 316 stainless steel with Swagelok Β© fittings. It consists of a
rotary vane vacuum pump and a Pirani vacuum gauge and is able to evacuate the entire
system to a pressure of < 20 mTorr. Once this pressure is achieved, the vacuum pump is
isolated from the system and the gases can then be mixed by using two independent
pressure gauges to verify the ratios of each gas. Each gas cylinder is fitted with a one-way
check valve to ensure flashbacks cannot occur. The manifold is fitted with ultra-torr Β©
fittings which allow gases to be mixed in the reaction vessel directly. Throughout the course
of these experiments, all irradiations will be investigated at atmospheric pressure (1 bar
absolute), this is to simulate the conditions under which the majority of the ππ’π2 canisters
are stored.
Chapter 3 Experimental 7131060
71
A specialist reaction vessel had to be developed to perform π»2 β π2 studies, which involved
several iterations of design. This development will be discussed in Chapter Four.
3.4.2 Air Radiolysis
For this set of experiments, 12 ml sample vials with a butyl rubber crimp cap were
employed. Three quantities of oxide loading were used during the experiments. These were
1 g, 50% oxide (by volume) and 90% oxide (by volume). This can be seen for πππ2 samples in
Figure 3.5. All masses were within Β± 0.01 g of the required quantity.
Figure 3.5: Picture of l-r 1 g, 50% oxide (by volume) and 90% oxide (by volume) for πππ2 samples
The three loading choices give a wide range of gas to solid ratio. Samples that contain 1 g of
oxide contain over 95% air (by volume) therefore it is expected that these samples will
closely replicate the experiments without any oxide powder present. Samples with 50%
oxide present represent a much larger mass of oxide than the 1 g samples. These samples
should help to confirm if there is a catalytic effect on nitrate formation in the presence of an
oxide surface as there is a lot more oxide surface than is present in 1 g samples for any gas
phase species to adsorb to. Samples with 90% volume of oxide are analogous to the ππ’π2
Chapter 3 Experimental 7131060
72
storage cans where the cans are almost full of oxide powder to reduce the number of cans
required.
To perform irradiations, samples are placed inside a test tube rack and irradiated with
standard laboratory air atmospheres. Post irradiation, the samples are injected with 5/7 ml
of 5 mM ππππ» solution to extract any gaseous nitric acid into solution. Samples containing
1 g of oxide are washed with 5 ml of the base solution and the 50% and 90% samples are
washed with 7 ml of the base solution. These volumes are chosen to ensure firstly, that
there is an excess of base in all the samples and secondly, that all the nitric acid can be
extracted. Due to the βstickyβ nature of nitric acid [49] it is important to have enough
solution to wash all of the surfaces in the system. Also there needs to be enough supernate
above the oxide to be able to draw off the solution to be analysed. This is a similar analytical
approach utilised by Kanda et al. [45]. After the samples are washed with the base solution,
they are homogenised and left to settle. After a period of time where two separate layers
have started to form, a portion of the solution is drawn off and filtered through a
polyvinylidene fluoride (πππ·πΉ) syringe filter; this is to ensure any fine particulates do not
plug the instrument. The filtered solution is placed inside an IC auto-sampler vial and
analysed using the IC.
Throughout these experiments, disposable needles and syringes are used for transferring
solutions between vials; this is to reduce the chance of contamination between samples.
The 12 ml glass sample vials are only used for one experiment so as to avoid contamination.
When adding the base solution to the irradiated samples, a gas tight 5/10 ml syringe is used
with disposable needles in order to ensure the same volume of ππππ» solution is injected
into each sample to increase repeatability across the experiment range. Finally, the IC auto-
Chapter 3 Experimental 7131060
73
sampler vials are also disposable to ensure there is no cross-contamination from any
previous samples.
3.4.3 Oxide Regeneration
After analysis of the aqueous phase it is important to βregenerateβ the oxide powder to its
unirradiated state for future experiments. This is achieved by filtering the oxide with an
aliquot of 5 mM ππππ» solution, to wash the surface and remove any adsorbed species. It is
then washed with copious volumes of deionised water to remove any excess sodium cations
from the basic solution before baking the powder in a furnace at 400 Β°C for 6 h under a static
air atmosphere. This temperature is high enough to remove any organic species that havenβt
been removed by washing and physisorbed water but low enough that it will not change the
crystallographic nature of the powder. The baked powder is then filtered through an
appropriate sized sieve to break up any agglomerated powder.
3.4.4 Accelerator Experiments
Bespoke glassware has been developed to investigate heavy ion radiolysis of the π»2 β π2 β
π΄π system. The glassware has similar features to the glassware used by Schuler et al. [50]
and is presented visually and schematically in Figure 3.6.
Chapter 3 Experimental 7131060
74
Figure 3.6: Bespoke glassware for π»π2+ ion radiolysis of π»2 β π2 β π΄π gaseous mixtures
The vessel is cylindrical in shape to allow for the ion beam to penetrate into the sample and
to be fully attenuated in the sample, not the glass itself. The vessel is approximately 30 cm
in length to accommodate the greater penetration distance of heavy ions into gaseous
targets. It has a platinum wire that is used to obtain current measurements in the sample
during irradiation. It also contains two Rotaflo taps which allow the cell to be purged with
the required gas mixture and to be connected to the GC for post irradiation analysis. As the
ion beam is only irradiating the sample and the taps are not located inside the radiation
field, radiation resistant materials are not required for their construction. There is a side
port to which a pressure transducer is attached during irradiations to log the pressure
change in the vessel. The end of the vessel is open ended with a ground glass flange, to
which a thin sheet of mica is attached to the flange using an epoxy resin and secured in
Chapter 3 Experimental 7131060
75
place with the ground glass ring. Due to the fragility of the mica window, all experiments are
investigated at atmospheric pressure (1 bar absolute).
All experiments are carried out with π»π2+ ions to simulate Ξ± decay from 238ππ’. Before the
ions hit the sample, the beam has to traverse a series of material windows (Figure 3.7),
therefore a calculation is needed to account for the energy loss of the beam from the
accelerator terminal to the sample. This is achieved by inputting the density of each
window into a program called SRIM (Stopping Range of Ions in Matter) [51]. This software
calculates the final ion energy on the sample from a machine starting energy or the initial
ion energy needed from the machine to generate a certain ion energy on sample.
Calculations were done using the latter parameters. Due to the slight variation in the density
of the mica window in the different reaction vessels, the exact ion energy on sample ranged
from 5.52-5.96 MeV. The currents employed during the series of experiments were 10 and
20 nA and irradiation times ranged from 10-30 mins. This configuration allowed for
equivalent doses as achieved using the 60πΆπ source in 64 h.
Figure 3.7: Configuration of window assembly through which the beam travels before reaching the sample
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
76
4 Development of Ξ³-Irradiation Reaction Vessel
This chapter details the extensive development involved in designing a reaction vessel
suitable to perform Ξ³-irradiations of π»2 β π2 β π΄π mixtures. The chapter also outlines the
development in sampling and analysis techniques that coincide with the iteration of
reaction vessel development to enhance the sensitivity of the gas chromatograph towards
π»2 analysis.
4.1 Initial Vessel Design
The initial reaction vessel utilised to perform π»2 β π2 irradiations using the 60πΆπ source is
shown below (Figure 4.1):
Figure 4.1: Reaction vessel for gamma radiation studies of π»2 β π2 system
The vessel is made of borosilicate glass, with a βbulbβ volume of 10 cm3. It has two Rotaflo
taps which are made from polytetrafluoroethylene (πππΉπΈ) and are chemically inert and gas
tight. These taps are removable which allows for oxide powder to be installed into the
vessel. The two outlets allow for the vessel to be attached directly to the manifold and to be
attached to the GC for βin-lineβ analysis.
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
77
To perform irradiations, the glass vessels are mounted onto a rail system shown in Figure
4.2.
Figure 4.2: Sample holder for gamma irradiation of π»2 β π2 system
This allows for vessels to be mounted in a set position thus ensuring a constant dose rate
during irradiation. The sample can be moved closer/further from the radiation sources so
that a range of dose rates can be achieved.
4.1.1 GC Configuration and Calibration
To accommodate this experimental set-up, the sampling valve of the GC had to be
reconfigured to allow the carrier gas to βforceβ the irradiated gas mixture through to the
detector. Figure 4.3 shows the GC valve set up in i) load position, where the sample is
attached to the GC and ii) inject position as the carrier gas injects the sample into the GC.
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
78
Figure 4.3: GC valve configuration for βin-lineβ analysis i) βLoadβ position ii) βInjectβ position
When a vessel is not attached to the GC, the two outlets are connected together and
flushed with argon gas in order to minimise the volume of air within the system. When a
vessel is attached as shown in Figure 4.3i there is a delay of a couple of seconds between
disconnecting the bridge between the two outlets and attaching the vessel, allowing air to
ingress into the sample loop. The total volume of the sample loop and connections in
comparison with the 10 cm3 volume of the injected sample means that the air impurity will
be less than 1% of the injected sample.
The GC is calibrated using the π»2 calibration gases detailed in Section 3.1.2. This is achieved
by purging the glass bulb with the gas for 60 s before attaching the vessel to the GC for
analysis. Several repeats of each calibration gas are done to increase accuracy (Figure 4.4).
i) ii)
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
79
Figure 4.4: Calibration of the gas chromatograph using certified calibration standards in the range 0.1-4% π»2 π΄πβ
At lower concentrations of hydrogen (< 1%) there is a linear relationship between the
concentration and the peak area. Above this concentration however, the calibration is non-
linear and there is a higher degree of scatter between repeat samples. The explanation for
this scatter can be seen in Figure 4.5; this is an overlay of two chromatograms, one
containing 2% π»2 π΄πβ , and the second containing 0.5% π»2 π΄πβ .
Figure 4.5: Gas chromatograms of 2% π»2 π΄πβ and 0.5% π»2 π΄πβ calibration gases
The signal present at 10 s is a systematic βsatelliteβ caused by the pressure change in the
system as the sampling valve rotates between βloadβ and βinjectβ positions.
0
500
1000
1500
2000
2500
3000
3500
0 0.1 0.2 0.3 0.4 0.5
Pea
k ar
ea /
AU
H2 Volume / cm3
0
100
200
300
400
500
600
700
800
0 25 50 75 100 125 150 175 200 225 250
SIgn
al In
ten
sity
/A
U
Retention time / s
2% H2/Ar
0.5% H2/Ar
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
80
In the 0.5% π»2 π΄πβ chromatogram there are two distinct peaks, with retention times of 115
and 165 s, respectively. The first peak is from hydrogen and the second is from oxygen
which is present in small quantities from the sample loop. In the 2% π»2 π΄πβ chromatogram
there are three peaks, however, the first two at retention times of 90 and 135 s, respectively
are overlapping. These two peaks are π»2 and π2. There is a four-fold difference in hydrogen
concentration between the calibration gases, therefore it is easier to assign the relevant
peak to this gas. The third peak in the 2% π»2 π΄πβ chromatogram is due to nitrogen, again
present in small quantities in the sample loop. Nitrogen may also be present in the 0.5%
π»2 π΄πβ chromatogram, however, the program ended before it could reach the detector. Due
to the interference in the first two peaks it is impossible to integrate the peak and attain a
true peak area.
This effect is still as prevalent in irradiated samples that contain higher concentrations of
hydrogen. Figure 4.6 shows the resultant chromatograms from initial trials of π»2 β π2
radiolysis studies. The gas ratios in the samples are 3.75:2.65:90 π»2: π2: π΄π. Samples are
irradiated individually using the same position within the irradiator with doses received
ranging between 1 and 5 kGy. By assuming the dose is absorbed by all of the gas, the
absorbed doses have been calculated to be in the range of 7.07x1015 and 3.48x1016 eV.
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
81
Figure 4.6: Overlain chromatograms of initial trials of π»2 β π2 radiolysis experiments
(n.b. - data set superimposed on - data set)
From Figure 4.6 two things become apparent. The first is the issue of separation between
π»2 and π2 signals and the second is that in this absorbed dose range, there is very little
chemistry occurring that is affecting the concentrations of either hydrogen or oxygen.
Before any attempts could be made to increase the separation between π»2 and π2 signals,
it became apparent that irradiated samples and samples of pure argon had significant levels
of π2 and π2 present that are similar to pure air. Further inspection of the vessels showed
that the πππΉπΈ taps had mechanically degraded (Figure 4.7) which had led to the original
sample being lost. This is a major issue as higher absorbed doses are needed to investigate
the π»2 β π2 system, however, the current vessel design does not tolerate doses higher than
several 100 kGy. This led to a redesign of the reaction vessel and subsequent sampling
method.
0
200
400
600
800
1000
1200
1400
0 50 100 150 200 250 300
Sign
al In
ten
sity
/ A
U
Retention time / s
7.07x10^15 eV1.41x10^16 eV2.10x10^16 eV2.80x10^16 eV3.48x10^16 eV
H2
O2 N2
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
82
Figure 4.7: Mechanical degradation of πππΉπΈ taps
An initial idea was to replace the πππΉπΈ taps with borosilicate stopcocks, however, this
would require a grease to lubricate the taps and ensure a good seal. Although radiation
resistant greases are available these would eventually degrade and could be a source of
hydrocarbons such as methane or π2 into the system.
4.2 Reaction Vessel Mark II
After extensive research, a commercially available metal sampling cylinder was chosen as
the reaction vessel (Figure 4.8). This has the benefit of being pressure tested up to pressures
of 60 bar as well as tolerating a greater temperature range. As the vessel is made of 316
stainless steel there should be no source of foreign gases into the system. Also, with a
commercial product comes greater repeatability between sample vessels with regards to
volumes and thickness. The volume of the metal cylinder is 10 cm3. Due to the geometry of
the vessels, the initial sample holder seen in Figure 4.3 is obsolete. A metal test tube rack
that is affixed to the base plate was developed to accommodate more samples than the
previous design.
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
83
Figure 4.8: Stainless steel sampling cylinder for π»2 β π2 gamma irradiation experiments
4.2.1 GC Calibration
Due to this vessel only having one inlet, the analysis method using the GC was also revised.
After samples have been irradiated, a rubber septa is placed over the outlet and purged
with argon gas. A gas tight sample syringe is then driven through the septa and into the
sample directly. The syringe is then pumped several times to ensure adequate mixing of the
sample and its contents are then injected onto the GC column directly using the separate
injection port.
Figure 4.9 shows the resulting calibration plot using this sampling method. From this figure,
it is evident that there is less scatter in the data and there is a linear response of the
detector up to 1 cm3 of pure π»2.
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
84
Figure 4.9: Calibration plot for pure π»2 using the direct injection methodology
In Figure 4.4, a volume of 0.4 cm3 of π»2 produced a peak with an area of approximately
3000 AU. Compared to the injection method, this has decreased to approximately 1200 AU.
This is due to the decrease in the sample volume that is being analysed from 10 cm3 (volume
of glass βbulbβ) to 1 cm3 (volume of the gas syringe).
Although the volume has been decreased, the resultant chromatograms still show sharp
distinguishable peaks with a Gaussian profile (Figure 4.10). It is noticeable that the quantity
of π2 and π2 has decreased significantly with this sampling method. However only with the
1 ml injection volume are there signs of other components in the sample.
y = 3634.4x RΒ² = 0.999
0
500
1000
1500
2000
2500
3000
3500
4000
0 0.2 0.4 0.6 0.8 1
Pea
k ar
ea /
AU
H2 volume / cm3
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
85
Figure 4.10: Overlay of gas chromatograms highlighting varying injection volumes of pure π»2
After irradiating these vessels in a pure argon atmosphere, it was discovered that the valves
in Figure 4.8 had a ball and socket joint which was made of ultra-high molecular weight
polyethylene (ππ»ππππΈ). Under irradiation conditions, this polymer decomposes and cross
links [52] which leads to the evolution of π»2 gas and thus to interference with post
irradiation analysis of the hydrogen yield.
0
100
200
300
400
500
600
700
800
900
1000
100 150 200 250 300 350 400
Sig
nal
Inte
nsi
ty /
AU
Retention Time / s
0.2 ml
0.4 ml
0.6 ml
0.8 ml
1.0 ml
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
86
4.3 Reaction Vessel Mark III
The final iteration of the reaction vessel design is shown in Figure 4.11. This is a bellows
sealed valve which is non-wetted and made entirely of various metal components.
Figure 4.11: Final vessel iteration to investigate radiolysis of π»2 β π2 systems
4.3.1 GC Configuration and Calibration
To eradicate any air from the system and for increased repeatability, a new analysis system
was developed and commissioned. This system reverted back to using the sample loop and
sampling valve highlighted in Section 4.1.1. The load and inject configurations of the
sampling valve are shown in Figure 4.12.
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
87
Figure 4.12: Final GC valve configuration i) βLoadβ position ii) βInjectβ position
This sampling method has a vacuum pump attached to one end of the sample loop, with the
reaction vessel attached to the other side. The pump can evacuate the loop directly to the
valve on the reaction vessel, once a good vacuum has been achieved, the pump is isolated.
The valve on the sample vessel is opened to expand the gas volume into the sample loop,
after which the sample vessel is isolated and the sampling valve rotates to inject the sample
inside the loop onto the column and to the detector. The sample loop has a pressure
transducer attached which can log the pressure throughout the analysis. It has a span of
2.5 bar absolute and an accuracy of Β± 2.5 mbar.
This method allows for multiple injections of a single sample as a correlation can be made
between the pressure of the sample in the loop and the resulting peak area, however, due
to dead volume this is not a perfect correlation. Figure 4.13 is a plot of pressure where six
injections are made. Between each injection the sample loop is evacuated to remove the
remnants of the previous sample. At the end of each injection, the pressure increases in the
sampling loop due to the GC valve rotating back to the βloadβ position which contains carrier
gas at a higher pressure than the sampling loop.
i) ii)
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
88
Figure 4.13: Plot of sample loop pressure as a function of time for six repeat injections with vacuum GC configuration
This configuration is calibrated by evacuating the sample vessels using the manifold and
filling the vessels with a calibration gas of known π»2 concentration. Three injections of each
sample are taken and the results shown in Figure 4.14. The partial pressure of hydrogen is
calculated using Equation 4.1.
ππ»2=
%π»2 πππππ
100 Equation 4.1
where ππ»2 is the partial pressure of hydrogen, %π»2
is the concentration of hydrogen in the
calibration gas and πππππ is the pressure in the sample loop as the sample is injected into the
GC.
0
200
400
600
800
1000
1200
1400
0 100 200 300 400 500 600 700 800
Pre
ssu
re /
mb
ar
Time / s
1
2
3
4 5
6
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
89
Figure 4.14: GC calibration curve of hydrogen partial pressure as a function of peak area for vacuum sampling system
The standard error of the slope is Β±0.001. This value is within tolerable limits and reduces
the scatter from the initial sampling design significantly.
The following series of equations are used to retrospectively calculate the number of moles
of hydrogen in the post irradiated sample from the partial pressure of hydrogen in the
sample loop. This value will then be able to determine the number of moles of hydrogen
lost/formed during irradiation by comparison with the initial number of moles in the
sample. Equation 4.2 is used to calculate the partial pressure of hydrogen within the sample
loop
ππ»2(πππππ) = ππ»2
" π΄π»2(πππππ) + ππ»2
" Equation 4.2
where ππ»2(πππππ) is the partial pressure of π»2 in the sample loop, ππ»2
" and ππ»2
" are
calibration constants (from the trend line equation in Figure 4.14) and π΄π»2(πππππ) is the
peak area for π»2 from the sample at pressure πππππ.
y = 0.142x - 0.027 RΒ² = 0.999
0.0
5.0
10.0
15.0
20.0
25.0
30.0
35.0
40.0
45.0
50.0
0 50 100 150 200 250 300 350
H2 p
arti
al p
ress
ure
in s
amp
le lo
op
/
mb
ar
Peak area / AU
H2 conc. in Ar
5%
2%
1%
0.50%
0.10%
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
90
Assuming ideal gas behaviour, the mole fraction of hydrogen will remain constant during the
expansion of the sample from the vessel into the sample loop, giving the following
expression:
ππ»2
ππ πππππ=
ππ»2(πππππ)
πππππ Equation 4.3
where ππ πππππ is the pressure of the initial sample. The partial pressure of π»2 in the
irradiated sample (ππ»2) is calculated by substituting Equation 4.2 into Equation 4.3 to give
the following:
ππ»2=
ππ πππππ
πππππ [ππ»2
" π΄π»2(πππππ) + ππ»2
" ] Equation 4.4
and the number of moles in the irradiated sample is calculated thus:
ππ»2=
ππ πππππ
πππππ ππ πππππ
Rπ [ππ»2
" π΄π»2(πππππ) + ππ»2
" ] Equation 4.5
where ππ πππππ is the volume of the vessel.
To ensure there is no reaction between the steel vessels and the gaseous sample, processed
blanks are made for each set of experiments. These blanks have the same composition of
gas as the irradiated samples, however, are left on the bench for the same time as the
irradiated samples.
An initial indication of whether the radiation had any effect on the system was to plot the
π»2 peak area against the pressure in the sample loop and to compare the translation in
respect to the y-axis of the series with respect to the unirradiated blank. Figure 4.15 is
shown as an example. The R2 values are very consistent, however, as stated previously, the
dead volume leads to a slight offset in correlation.
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
91
Figure 4.15: Plot of π»2 peak area as a function of sample loop pressure for a series of samples containing 5:5:90 π»2: π2: π΄π
After the initial trials were completed, it became apparent that there was little
correspondence between the absorbed dose the samples had received and the loss of
hydrogen yield as determined from the GC. One hypothesis is the efficiency with which the
manifold mixed the gases pre-irradiation, as this random error could lead to the observed
differences in hydrogen yield in the GC results.
RΒ² = 0.9994 RΒ² = 0.9998 RΒ² = 0.9989 RΒ² = 0.9999
RΒ² = 0.9996
0
200
400
600
800
1000
1200
1400
1600
200 400 600 800 1000 1200 1400
H2 P
eak
are
a /
AU
Pressure / mbar
Unirradiated
Vessel 1
Vessel 2
Vessel 3
Vessel 4
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
92
4.4 Gas Mixing
To test this hypothesis, four experiments were trialled using different gas mixtures. A
minimum of four vessels were attached to the manifold and evacuated to a pressure below
20 mTorr. The vacuum pump was isolated and the vessels were filled to identical pressures
of the relevant gas mix. The samples were analysed consecutively on the GC. The four gas
mixtures were as follows:
A pre-mixed two component calibration gas of known hydrogen concentration;
A single component gas (in this case hydrogen);
A two component gas mixture of hydrogen and argon mixed within the vessels and
concentration determined by pressure; and
A three component gas mixture of hydrogen, oxygen and argon mixed in the vessels
and concentration determined by pressure.
Figure 4.16 shows the resulting plots of hydrogen peak area as a function of sample loop
pressure for the four gas mixtures.
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
93
i)
ii)
iii)
iv)
Figure 4.16: Plots of π»2 peak area as a function of sample loop pressure of four different gas mixes i) 2% π»2/π΄π calibration gas, ii) pure hydrogen gas, iii) 10:90 π»2: π΄π gas mix from
manifold and iv) 5:5:90 π»2: π2: π΄π gas mix from manifold
40
50
60
70
80
90
100
110
120
350 450 550 650 750
H2 p
eak
area
/ A
U
Pressure / mbar
2%H2/Ar calibration gas
Vessel 1Vessel 2Vessel 3Vessel 4
R.S.D. 0.18
2000
2500
3000
3500
4000
4500
5000
350 450 550 650 750
H2 p
eak
area
/ A
U
Pressure / mbar
Pure H2
Vessel 1
Vessel 2
Vessel 3
Vessel 4
R.S.D. 2.51
0
500
1000
1500
2000
350 450 550 650 750
H2 p
eak
area
/ A
U
Pressure / mbar
10:90 H2 - Ar
Vessel 1 Vessel 2
Vessel 3 Vessel 4R.S.D. 16.45
0
200
400
600
800
1000
1200
350 450 550 650 750
H2 p
eak
area
/ A
U
Pressure / mbar
5:5:90 H2-O2-Ar
Vessel 1 Vessel 2Vessel 3 Vessel 4Vessel 5 Vessel 6
R.S.D. 29.62
n.b. All four data sets
are superimposed
n.b. All four data sets
are superimposed
n.b. Vessel 1 and 3 data
sets are superimposed
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
94
From this series of graphs, it is evident that as more components are mixed with the
manifold system, the more scatter in the GC analysis. This can be seen with the values of the
relative standard deviation (RSD), starting at 2.51 for a single component gas and rising to
29.62 for a three component gas mix. It is not a question of number of components as the
calibration gas has the least scatter across a series of samples with a relative standard
deviation of 0.18 despite being a two component mixture. As the gases are mixed in series,
the manifold relies solely on diffusion of the components to mix homogeneously inside the
vessels. The timescales employed in the mixing of the gases (minutes) is not long enough for
displacement of the lighter gases by the denser gases assuming Brownian motion occurs,
therefore an alternative mixing method is needed.
To solve this issue, the gases need to be pre-mixed before being expanded into the vessels
(such as the calibration gases). To achieve this, a large volume mixing cylinder was added to
the manifold, shown schematically in Figure 4.17. The entire manifold is placed under
vacuum and once a good vacuum is achieved (< 20 mTorr), the vessels (red circles) are
isolated from the system. The gases are mixed in series inside the 1 L cylinder. To increase
the mixing speed of the gas mixtures, a πππΉπΈ coated stirrer bar is placed inside the mixing
cylinder and a magnetic stirrer placed under the cylinder. After approximately 30 mins, the
valve separating the irradiation vessels and the mixing cylinder is opened and the difference
in pressure leads the gas mixture to expand into the vessels. To achieve near atmospheric
pressure in the vessels once the mixture has been expanded, the mixing cylinder has to be
mixed at 1 bar above atmospheric pressure. As the entire manifold is made from 316 steel
there is no issue with pressure build up or leakage.
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
95
Figure 4.17: Manifold schematic with new mixing cylinder and πππΉπΈ stirrer bar addition
The initial pressure of each gas inside the mixing cylinder is used to calculate the
concentration of each gas and their partial pressures. The pressure inside the reaction
vessels (once the gas has been expanded) will be used as ππ πππππ. Equation 4.3 can be
adapted to relate the partial pressure of hydrogen inside the mixing cylinder to the partial
pressure of hydrogen inside the irradiation vessels (Equation 4.6)
ππ»2
πππ¦ππππππ=
ππ»2(ππ πππππ)
ππ πππππ Equation 4.6
Figure 4.18: Final iteration of manifold design
The final configuration of the manifold is illustrated in Figure 4.18.
Chapter 4 Development of Ξ³-Irradiation Reaction Vessel 7131060
96
Figure 4.19 highlights a repeat of the experiment seen in Figure 4.16iv where three gaseous
components are mixed and several samples are analysed to ascertain how much scatter
there is between them. This time however, the gases are mixed in the mixing cylinder first
and agitated for 30 mins before being expanded into the vessels.
Figure 4.19: Mixing efficiency of manifold with mixing cylinder for a three component gas mixture (n.b. all four data sets superimposed)
The relative standard deviation has significantly decreased from 29.62 to 1.02; this gives
significant confidence in the mixing ability of the manifold.
Summary
A significant quantity of time and effort has been expended to ensure that all aspects of this
part of the research, from initial gas mixing to sampling and final analysis are as accurate
and repeatable as possible.
50
100
150
200
250
300
350
200 300 400 500 600 700 800 900
H2 p
eak
area
/ A
U
Pressure / mbar
5:5:90 H2:O2:Ar
Vessel 1Vessel 2Vessel 3Vessel 4
R.S.D. 1.02
Chapter 5 Dosimetry 7131060
97
5 Dosimetry
The following chapter outlines what dosimetry is and why it is an important part in radiation
chemistry. It discusses the different types of dosimetry utilised in this research and the
advantages and disadvantages of each one for a particular system of interest. It will also
look at previous literature and how dosimetry is dealt with in similar systems and
circumstances to this research.
5.1 Background
It is important to quantify the amount of energy that is transferred between a radiation field
and an absorbing material and how this energy is distributed in the absorbing system. This
quantification constitutes radiation dosimetry and is termed absorbed dose, which has units
of amount of energy absorbed per unit mass of irradiated material. The SI derived unit of
absorbed dose is the Gray (Gy) (Equation 5.1), however, older sources of literature use the
rad. Conversion between Gray and rad is shown in Equation 5.2.
1 Gy = 1 J kgβ1 Equation 5.1
1 Gy = 100 rad Equation 5.2
The amount of energy transferred to a material and its distribution throughout the material
are dependent on many factors; these include the type of radiation (Ξ± particles transfer a
larger quantity of energy during collisions than Ξ³- rays and lead to a column-like structure of
ionisation and excitation events), the energy of the emitted radiation (higher energy
radiation will penetrate further into the material) and finally, the composition of the
absorbing material (a solid will absorb more energy than a gaseous material due to the
higher density and greater stopping power of the solid).
Chapter 5 Dosimetry 7131060
98
Dosimetry can be divided into two categories: absolute and secondary methods [12].
Absolute methods determine the absorbed dose by direct measurements of a physical
property of the system. This can be either ionisation of a gas or charge carried by a beam of
charged particles with a known energy. Secondary dosimeters are used in systems whose
response to radiation is known from previous absolute dosimeter measurements. The type
of system being irradiated will determine which dosimeter is of most use.
In radiation chemistry studies, the most common type of dosimeters employed are chemical
dosimeters. These are secondary dosimeters where the radiation dose is determined from
the chemical change produced by the radiation field in a particular system. To calculate the
absorbed dose in the system, a G-value is required for the reaction or product of interest for
a particular radiation type. This is found by comparison with absolute dosimetry
measurements.
To generate a G-value it is important to understand the primary radiolysis chemical yields of
the system composing the dosimeter. The information provided by a chemical dosimeter is
an average quantity of energy absorbed across the entire dosimeter.
Chapter 5 Dosimetry 7131060
99
5.2 Aqueous Dosimetry
The most widely used chemical dosimeter is that of the Fricke dosimeter [12]. As a result, it
is one of the most mechanistically understood systems. It concerns the redox chemistry of
the ferrous ion (πΉπ2+) and its oxidation to the ferric ion (πΉπ3+) by the products of π»2π
radiolysis. The dosimeter is composed of an aerated aqueous solution of iron (II) sulphate
(πΉπππ4) and sulphuric acid (π»2ππ4). The sulphuric acid acts as a proton source which helps
to convert reducing radicals to oxidising radicals and create an oxidising environment, in
turn leading to the oxidation of πΉπ2+ to πΉπ3+. The reaction scheme for the radiolysis of the
Fricke dosimeter is outlined in the following reactions:
πππβ + π2 β π2
β Reaction 5.1
π»+ + π2β β π»π2
. Reaction 5.2
πππβ + π»ππ
+ β π». Reaction 5.3
π». + π2 β π»π2. Reaction 5.4
πΉπ2+ + π». + π»2π β πΉπ3+ + π»2 + ππ»β Reaction 5.5
πΉπ2+ + ππ». β πΉπ3+ + ππ»β Reaction 5.6
πΉπ2+ + π»2π2 β πΉπ3+ + ππ». + ππ»β Reaction 5.7
πΉπ2+ + π»π2. + π»2π β πΉπ3+ + ππ». + ππ»β Reaction 5.8
πΉπ3+ + π». β πΉπ2+ + π»+ Reaction 5.9
Once irradiated, the resulting solution is analysed using UV-Vis spectrophotometry, as the
πΉπ3+ ion exhibits a characteristic absorption at 304 nm. The absorption value at this
wavelength is subtracted from an unirradiated βblankβ value to obtain the true absorption
value. The dose received by the irradiated solution is then determined using Equation 5.3:
Chapter 5 Dosimetry 7131060
100
Absorbed Dose, π·π· = 100 F π΄ππ
π π πΊ(πΉπ3+) πΏ Equation 5.3
where π΄ππ is the true absorption value at 304 nm for the irradiated Fricke solution, F is the
Faraday constant (9.648x104 C mol-1), Ξ΅ is the molar extinction coefficient of the πΉπ3+ ion
(2174 dm3 mol-1 cm-1), Ο is the density of the Fricke solution (1.024 g cm-3), πΊ(πΉπ3+) is the
radiolytic yield of πΉπ3+ (15.5 molecules 100 eV-1 for 60πΆπ gamma rays) and L is the path
length of the light in the measured Fricke solution. Once the absorbed dose is calculated,
the dose rate can be calculated by dividing the absorbed dose by the irradiation time.
The Fricke dosimeter has a linear absorption within the range of 0-400 Gy. Above this dose,
the oxygen dissolved in the solution is exhausted which leads to a reduction in the oxidation
of πΉπ2+. This oxidation can also occur with light; therefore all solutions must be kept in the
dark.
To make 500 ml of stock Fricke solution, 0.2 g πΉπππ4. π»2π (Fisher chemicals, laboratory
reagent grade) and 11 ml concentrated π»2ππ4 (Fluka Analytical, β₯ 97.5%) are combined with
deionised water. This gives a concentration of 1 mM πΉπππ4 in 0.4 M π»2ππ4 stock solution.
Irradiations are carried out by placing 3 ml of the stock solution into a vial that is
representative of the reaction vessel to be used in the research. This is irradiated for a short
period of time and the resulting solution is pipetted into a cuvette and analysed at 304 nm
in the UV-Vis spectrophotometer. All experiments use a test tube rack configuration for
irradiations, therefore dosimetry was carried out for each position within this rack. Both
60πΆπ source rods were used and no attenuation was in place due to the fact that this
configuration gave the highest dose rates achievable. To ascertain the relative dose rate of
each individual position in the rack, two different irradiation times and three repeats of
Chapter 5 Dosimetry 7131060
101
each time were carried out. This reduced the random error of transferring the stock solution
between the irradiation vessel and the cuvette to a minimum. To replicate multiple samples
being irradiated at once, empty vessels were placed in front of the irradiated solution to
investigate the attenuation of the reaction vessels. Figure 5.1 shows the results for the 4x6
rack showing i) the unattenuated dose rate and ii) fully attenuated dose rates.
Chapter 5 Dosimetry 7131060
102
i)
ii)
Figure 5.1: Fricke dosimetry results for the test tube rack array showing i) Unattenuated dose rate ii) Fully attenuated dose rate (units β Gy min-1) (correct as of 10th February 2015)
Chapter 5 Dosimetry 7131060
103
From Figure 5.1 it is clear that, as expected, the dose rate decreases significantly as the
samples are placed further away from the source rods (in accordance with Equation 3.1),
however, there is also dose rate variation across the rack where samples are equidistance
from the sources. As stated in Section 3.2.1, only sources A and C are filled with 60πΆπ,
therefore the central two columns of the rack are equal distance from the two sources,
however, the outside two columns are closer to one source than the other leading to a
reduction between 10-20% of the dose rate across the row. Figure 5.1ii shows that there is
an approximate 10% decrease of dose rate throughout the rack when positions are
attenuated by other samples. It is evident that source C contains more 60πΆπ than source A,
as the dose rate is not symmetrical across the chamber. Samples on the right hand side of
the chamber, closer to source C, have a higher dose rate than samples in the corresponding
positions on the left hand side of the chamber.
Following the extensive dosimetry of the source, a dose decay series is set up using
Microsoft Excel. This dose rate decay calculator is then validated monthly via single point
dosimetry to ensure the decay calculated dose rates are correct.
5.3 Calculation of Absorbed Dose using 60πͺπ Source
Now that a dose rate for each position has been calculated, it is important to determine the
absorbed dose by real samples irradiated under the same conditions. This is easily
calculated if the sample and dosimeter are both homogeneous and have the same density
and size, as the absorbed dose will be the same. This is true with aqueous solutions and the
Fricke dosimeter. If the samples differ from the dosimeter then extra calculations are
needed to determine the absorbed dose.
Chapter 5 Dosimetry 7131060
104
Equation 5.3 shows how absorbed dose, π·π·, is related to the radiochemical yield of product
formed by irradiation (in this case πΊ(πΉπ3+) for Fricke dosimeter). The absorbed dose in a
sample π·π is related to absorbed dose in the dosimeter by Equation 5.4:
πΊ(π)π = πΊ(πβ²)π· [π]π
[πβ²]π· ππ·
ππ π·π·
π·π Equation 5.4
where πΊ(πβ²)π· is the radiochemical yield of product πβ² formed in the dosimeter, [π]π and
[πβ²]π· are the measured yields of π and πβ² (moles per unit volume) in the sample and
dosimeter when exposed to the same radiation field, ππ· and ππ are the densities of the
sample and dosimeter and π·π·
π·π is the ratio of absorbed dose per unit mass in the sample and
dosimeter. The absorbed dose in the sample and dosimeter are related by the following
equation:
π·π = π·π· (
ππππ
)π
(πππ
π)
π·
Equation 5.5
where (πππ
π)
π and (
πππ
π)
π· are the mass energy absorption coefficients for the sample and
dosimeter respectively.
From the 60πΆπ decay scheme seen in Figure 3.2, the energies of photons emitted by the
source are 1.17 and 1.33 MeV and from Figure 1.8 (replicated in Figure 5.2) it is seen that
these energies lie in the region where Compton scattering is the dominant process of Ξ³ β ray
absorption.
(molecules 100 eV-1)
Chapter 5 Dosimetry 7131060
105
Figure 5.2: Ξ³-ray interaction processes and their dependence on photon energy and Z of medium (replicated from [13])
Therefore Equation 5.5 can be simplified to the following:
π·π = π·π· (π π΄β )π
(π π΄β )π· Equation 5.6
where π π΄β is the ratio of atomic number to atomic weight for an element.
This simplification is incorporated because Compton absorption is proportional to the
number of electrons in the medium and not to the way in which they are bound in the
atoms. As the number of electrons per unit mass of material is proportional to π π΄β , it does
not require knowledge of mass energy absorption coefficients.
5.3.1 Adsorbed Dose in Gaseous Systems
For a mixture such as the systems of interest in this research, a mean value (π π΄βΜ Μ Μ Μ Μ Μ ), is
calculated using Equation 5.7.
π π΄βΜ Μ Μ Μ Μ Μ = π΄ [π€π (π
π΄)
π] Equation 5.7
π€π is the weight fraction of element i in the medium. Equation 5.6 then becomes:
0
20
40
60
80
100
120
0.01 0.1 1 10 100
Z o
f m
ediu
m
hΞ½ / MeV
Photoelectric effect
Compton effect
Pair production
Chapter 5 Dosimetry 7131060
106
π·π = π·π· (π π΄βΜ Μ Μ Μ Μ Μ )
π
(π π΄βΜ Μ Μ Μ Μ Μ )π·
Equation 5.8
The Fricke dosimeter has the following weight percentages: 10.84% π»2, 87.91% π2 and
1.25% sulphur, therefore (π π΄β )Μ Μ Μ Μ Μ Μ Μ Μ π· is calculated thus:
(π π΄β )Μ Μ Μ Μ Μ Μ Μ Μ π· = [0.108 x (
2
2.016)] + [0.88 x (
16
31.998)] + [0.012 x (
16
32.06)]
= 0.5532
A gas mixture with partial pressures of 5:5:90 π»2: π2: π΄π has the following weight
percentages (in a 10 cm3 reaction vessel at 1 bar absolute), 0.27% π»2, 4.25% π2 and 95.48%
π΄π, therefore (π π΄β )Μ Μ Μ Μ Μ Μ Μ Μ π is calculated thus:
(π π΄β )Μ Μ Μ Μ Μ Μ Μ Μ π = [0.0027 x (
2
2.016)] + [0.0425 x (
16
31.998)] + [0.9548 x (
18
39.948)]
= 0.4541
Equation 5.8 then becomes:
π·π = π·π· 0.8209 Equation 5.9
Assuming that both sample and dosimeter are of the same size (volume), exposed to the
same irradiation field and irradiated in the same vessels, then a gaseous mix of 5:5:90
π»2: π2: π΄π will receive 82% of the equivalent absorbed dose of the Fricke dosimeter.
For samples that contain an oxide powder, only the dose absorbed by the gas is considered.
This is because the species formed/reacted that are of interest are gaseous species that
originate from the gas phase. The presence of an oxide powder may lead to catalytic or
Chapter 5 Dosimetry 7131060
107
steric effects but it is unknown whether it plays a part in the radiation chemistry reaction
mechanism.
5.3.2 Literature Review of Heterogeneous System Dosimetry
There are several different approaches when dealing with the dosimetry of heterogeneous
systems in the literature. In a paper by Nilsson and Jonsson, investigating the Ξ³ β ray induced
dissolution of ππ2 pellets in 10 mM hydrogen carbonate (π»πΆπ3β) solutions, the dose rate is
just that determined by Fricke dosimetry without any subsequent correction [53].
Experiments carried out by Petrik et al. [25] which investigated the gamma radiolysis of
water on the surface of a variety of metal oxide surfaces, stated that the absorbed dose rate
is determined by the Fricke dosimeter only, without subsequent correction. In a paper by
Stone [54] investigating the radiolysis of cyclohexane in a xenon matrix, Fricke dosimetry
was used to determine the dose rate of the gamma source, however, for the higher Z
materials of interest, an ion chamber with walls composed of graphite was used to
determine the energy absorbed by the cyclohexane and the results extrapolated to
ascertain a weighting factor for the dose absorbed by the xenon. The same approach was
used by Sagert and Robinson [55] when investigating nitrous oxide (π2π), adsorbed to silica
gel and πππ2. The dose rate of the source was determined by Fricke dosimetry and an ion
chamber with walls composed of πππ2 was utilised to investigate the equivalent dose
absorbed by the πππ2. There was no reference made to how the energy absorbed by π2π
was calculated, however it was found that πππ2 absorbs 10% more energy than the Fricke
solution when exposed to the same radiation field. This value has been used in subsequent
papers by LaVerne and Tandon [29, 56] which investigated the hydrogen formation from
radiolysis of adsorbed water on several metal oxide powders. The energy absorbed by the
Chapter 5 Dosimetry 7131060
108
adsorbed water was calculated directly from Fricke measurements. A 10% weighting factor
was added to this energy to determine the energy absorbed by the metal oxides. They
plotted their results as a function of dose absorbed by the water alone and also as a
function of total energy absorbed by the entire system (oxide and water).
From these various references it is clear that there is not a clearly outlined methodology for
determining the absorbed dose in a heterogeneous system. In most cases, the dose
absorbed by the phase of interest (usually an adsorbed organic species) is calculated as that
absorbed by the equivalent Fricke measurement whilst dose absorbed by the solid metal
oxide phase is neglected. In other references however, a weighting factor is added to the
absorbed dose calculated by the Fricke dosimeter for higher Z materials.
In this research, only the energy absorbed by the gas phase will be utilised to determine G-
values for the systems of interest. The dose rate from the gamma irradiation source will be
determined by Fricke dosimetry and these values corrected for the difference in sample
density, using Equation 5.9 for the energy absorbed by π»2: π2: π΄π gas mixtures and
Equation 5.10 to estimate the dose absorbed by air.
π·π = π·π· 0.9022 Equation 5.10
assuming air has the following weight percentage, 75.56% π2, 23.15% π2 and 1.29% π΄π and
thus (π π΄β )Μ Μ Μ Μ Μ Μ Μ Μ π = 0.4992.
Chapter 5 Dosimetry 7131060
109
5.4 Disadvantages of Fricke Dosimetry with Metal Vessels
As stated previously, dosimetry using a Fricke solution is investigated by filling an
appropriate reaction vessel with an aliquot of the solution. In this research there are two
distinct reaction vessels. These are the glass headspace vials shown in Figure 3.5 pertaining
to the air radiolysis experiments and the metal sample cylinders seen in Figure 4.11 to
investigate the radiolysis of π»2 β π2 gas mixtures. Borosilicate glass is very chemically
resistant to dilute acidic solutions therefore no issues arise from irradiating Fricke solutions
in these reaction vessels. However, sulphuric acid does react with most metals to liberate
hydrogen gas and a salt of the metal, thus even at these low concentrations (0.4 M), there
may be an etching effect on the steel. It is important to quantify the affect the steel has on
attenuating the radiation field, therefore the dose rates attained from Fricke in glass vials
cannot be extrapolated for steel vessels. A different type of chemical dosimeter will
consequently be needed to investigate the dose absorbed by π»2 β π2 gas mixtures.
There are several other materials that are used for dosimetry in radiation chemistry.
Another commonly used chemical dosimeter is that of ceric sulphate which investigates the
reduction of ceric ions (πΆπ4+) to cerrous ions (πΆπ3+). This suffers the same problem as
Fricke dosimetry in that it is a 0.4 M acid solution. There are also solid state dosimeters such
as polymethylmethacrylate ( ππππ΄ ), which degrades under irradiation and forms
chromophores which can be measured spectrophotometrically. This will not react with the
steel vessels and is available from a commercial company which therefore increases
repeatability across several measurements. A disadvantage of this type of dosimeter is that
the 1 cm strips of ππππ΄ are ready made to be able to fit into a UV-Vis spectrophotometer.
These dimensions do not allow the strips to be placed in the sample cylinders without
Chapter 5 Dosimetry 7131060
110
cutting them down to an appropriate size. This reduces the repeatability of each strip as the
dimensions will change between samples and also the certified calibration for each batch
may not be fit for purpose. Another disadvantage is that the density between ππππ΄ and
gaseous samples is greater than that of gaseous samples and Fricke solutions, therefore
more corrections are needed to ascertain the absorbed dose by the gas phase.
5.5 Gas Phase Dosimetry
It was decided to use a gas phase dosimeter in order to negate the need for any density
corrections. The two most commonly used gas phase dosimeters are π2π and ethylene
(πΆ2π»4). Both systems are well investigated and understood and use gas chromatography to
measure the yield of π2 and π»2 respectively and determine the energy absorbed by the
system. The following section analyses the literature to review the work that has been
undertaken for these gaseous dosimeter systems.
5.5.1 Gas Phase Dosimetry Literature
As stated in Figure 5.2, the main energy deposition process for solid and liquid samples of
low Z numbers is Compton scattering where the energy absorbed can be calculated from a
secondary dosimeter. In gaseous samples however, there is very little direct absorption of
gamma radiation and most of the absorbed energy comes from secondary electrons
generated by the gamma radiation interacting with the vessel walls [57]. Therefore, the
sample vessel geometry and nature of the wall materials is of importance for gas phase
dosimetry.
Chapter 5 Dosimetry 7131060
111
Johnson [58] irradiated π2π with a 60πΆπ gamma source and calculated a G(π2) value of
12.8 Β± 0.4 molecules 100 eV-1. They used two parallel methods to determine the energy
absorbed in the system; these were ionisation current measurements and the Fricke
dosimeter. Corrections were applied to these measurements to determine the dose
absorbed by π2π, before determining the dose rate from ionisation current measurements
by applying the following equation (5.11):
π·π = π½ ππ2π Equation 5.11
where π½ is the number of ion pairs formed per minute and ππ2π is the mean energy
required to produce an ion pair in eV.
Determination of the energy absorbed by π2π as a function of the Fricke dosimetry has
been calculated using Equation 5.12.
π·π2π = π·π· ππ2πππ2π
ππ·ππ Equation 5.12
where π·π· is the dose absorbed by the Fricke dosimeter, ππ2π and ππ· are the number of
electrons cm-1 for π2π gas and the Fricke dosimeter respectively and ππ2π and ππ are the
stopping powers per electron in π2π and the vessel wall respectively. This equation has
several uncertainties however, and the author disregarded this calculation and relied solely
on ionisation current measurements.
McLaren [59] replicated part of this work and attained G(π2) values of 9.03 Β± 0.1 molecules
100 eV-1 by using ionisation measurements to determine dose rates. They attribute the
difference in yield determined by Johnson to leaks of air into the system during
experiments. These errors limit the accuracy of the dosimeter to 10%.
Chapter 5 Dosimetry 7131060
112
Jankovsky [60] compared the use of π2π and ethylene for gas phase dosimetry and found
that the yield of G(π2) from π2π value varied between 9.03 and 12.8 molecules 100 eV-1 of
energy absorbed using 60πΆπ as the radiation source. This data has a relative standard
deviation of 0.1. This scatter is attributed to leaks in the system and also to the unavoidable
difficulties in determining small π2 yields from irradiation cells with β€ 100 cm3 volume.
Studies using ethylene found yields of hydrogen varied between 1.2-1.36 molecules 100 eV-1
energy absorbed for 60πΆπ gamma rays. The relative standard deviation for this data is 0.04.
Therefore their conclusions are that ethylene is the better system to determine gas phase
dosimetry when small reaction volumes are utilised.
Ethylene gas has also been used in mixed radiation fields to determine absorbed dose [61,
62]. Ikezoe et al. determined the yield of π»2 from ethylene radiolysis to be 1.3 molecules
100 eV-1 for both 60πΆπ gamma rays and reactor radiation which was a mix of neutrons and
gamma rays [61]. A similar study by Srinivasan et al. determined the yield of π»2 to be 1.2
molecules 100 eV-1 in a reactor radiation field [62].
Summary
From this literature selection it is evident that ethylene is the more suitable option for a gas
phase dosimeter. This is due to the amount of scatter in the G(π2) yields which arises from
air ingress into the system and also the limits of detection required for low volumes of
sample analysis. As stated in Section 3.3.1, the current gas chromatogram configuration is
optimised for the detection of π»2 down to very low concentrations (~100 ppm) which
indicates that the configuration is more suited to detect the radiolysis products from
Chapter 5 Dosimetry 7131060
113
ethylene than that of π2π. Another factor is the vacuum pump employed in the GC analysis
system does not evacuate the sample loop to absolute vacuum, only to approximately 1% of
atmospheric pressure. This means it is almost impossible to remove π2 from the sample
loop entirely without further considerations, so that yields of π2 from π2π radiolysis could
not be determined accurately.
5.5.2 Ethylene Dosimetry Results
To ascertain the dose rate inside the steel cylinders, the cylinders are attached to the
manifold outlined in Section 3.4.1 and evacuated to a pressure of < 20 mTorr. The ethylene
calibration gas is fed into the cylinders until atmospheric pressure is achieved inside the
vessels before the samples are placed inside the test tube rack array and irradiated for
several hours. Once irradiated, the samples are analysed using the GC, following the same
procedure as outlined in Section 4.3.3. Following analysis, the vessels are washed with
methanol and baked at 250 Β°C for several hours in order to ensure any polymeric products
that may condense onto the vessel walls are removed before the vessels are used again.
Due to the steric constraints inside the irradiation chamber and the high doses required,
only the front row of the test tube rack has been tested (Figure 5.3). For the calculation of
the absorbed dose, the value of G(π»2) = 1.36 molecules 100 eV-1 was utilised [59] and a
value of 28.05 g mol-1 to represent the molecular weight of ethylene was used to calculate
the mass of ethylene irradiated.
Chapter 5 Dosimetry 7131060
114
Figure 5.3: Results of ethylene dosimetry (units β Gy min-1) (dose rates correct as of 17th February 2015)
These results in comparison to those attained with the Fricke dosimeter results will be
discussed further in Chapter Seven.
5.6 Ion Accelerator Dosimetry
As seen in Section 5.3, dosimetry of a heterogeneous system using a gamma source is a very
complex issue, one that still is not fully understood in the wider research community. In
contrast, dosimetry of an ion source is far simpler. The previous sections have dealt with
several secondary dosimeters, however, dosimetry of an ion source can be calculated using
absolute measurements. As seen in Figure 3.7, the ion beam passes through a titanium
window before entering the sample vessel. This configuration of windows acts as a Faraday
cup [50, 63] which allows for the collection of charged particles hitting the cup. The resulting
current can be measured and used to calculate the number of ions entering a sample.
Throughout this research, the beam consists of ions in a single charge state, therefore for a
Chapter 5 Dosimetry 7131060
115
continuous beam, Equation 5.13 can be used to determine the number of ions π
penetrating the sample.
π = πΌ.π‘
e Equation 5.13
where πΌ is the measured electric current (in amperes), π‘ is the irradiation time (in seconds)
and e is the elementary charge (in Coulombs). This value is used to calculate the absorbed
dose π·, in the sample using Equation 5.14:
π· = ππΈ
π Equation 5.14
where πΈ is the incident energy of each ion (in MeV) and π is the ion charge state. All
experiments using the ion accelerator utilise a beam of π»π2+ ions, therefore π is 2.
This method is the most commonly used for ion accelerator dosimetry [12, 64].
The electric current is measured by a pico-ammeter that is connected at several points
along the beam line.
Chapter 5 Dosimetry 7131060
116
Figure 5.4: Plot of current as a function of time for a 15 min irradiation using the ion accelerator showing the current measured on the ππ window
Figure 5.4 shows the resulting current profile of a 15 min irradiation using a current of
20 nA. The current put on the ππ window is very stable and only drops once during the
irradiation.
Summary
This chapter outlines the difficulties in calculating the absorbed dose in the systems of
interest to this research. In previous literature sources, there are many methods to
determine this dose, however, there is not a unified concept which is agreed upon. In this
research there are three systems of interest:
Ξ³-radiolysis of air in contact with a metal oxide powder;
Ξ³-radiolysis of π»2: π2: π΄π mixtures in contact with metal oxide powders; and
radiolysis of π»2: π2: π΄π mixtures using an accelerated ion beam
-5.0E-09
0.0E+00
5.0E-09
1.0E-08
1.5E-08
2.0E-08
2.5E-08
3 8 13 18 23
Ti w
ind
ow
cu
rren
t /
Am
ps
Time / min
Chapter 5 Dosimetry 7131060
117
Each system has different requirements with regards to how absorbed dose is calculated.
Dosimetry of the gamma source has been carried out with secondary chemical dosimeters,
due to their simplicity and adaptability. In the first system of interest, only the dose
absorbed by the air will be used to calculate G-values. This is achieved by the Fricke
dosimeter multiplied by a weighting factor (Equation 5.10) due to the difference in sample
density.
The dose absorbed by the π»2: π2: π΄π mixtures will solely be used to determine loss of
reactants in the second system. Due to the nature of the sample vessels, ethylene gas is
used as the chemical dosimeter. The dose rates utilised are shown in Figure 5.3 which are
corrected for decay of the 60πΆπ source.
Experiments that use an ion accelerator as the radiation source, absolute dosimetry from
currents measurements collected during each experiment will be used to calculate the dose
received by the sample.
Chapter 6 Oxide Powder Characterisation 7131060
118
6 Oxide Powder Characterisation
This chapter outlines the physical properties of the two oxide powders utilised in this
research. Each oxide is characterised as received and after undergoing the regeneration
process outlined in Section 3.4.3. Finally, a comparison is made between the properties of
πΆππ2 and πππ2. If the oxide powders have any catalytic effects on the gas phase chemistry,
then it is important to determine their physical properties.
6.1 Properties of πͺππΆπ
6.1.1 As Received
To ascertain the purity and morphology of the πΆππ2 (as received), SEM and EDS analysis
were undertaken.
Figure 6.1: Scanning electron micrograph of πΆππ2 (as received)
Figure 6.1 illustrates the powder morphology of πΆππ2 using an SEM. It is clear from this
image that there is not a dominant morphology within the powder. There are well defined
Chapter 6 Oxide Powder Characterisation 7131060
119
edges along with irregular shaped grains and the average particle has faces with surface
area of approximately 3 Β΅m2.
The EDS spectrum for the, as received πΆππ2 is shown in Figure 6.2. The carbon signal arises
from the carbon stub. Silicon is the largest impurity present, as stated in Section 3.1.2.
Figure 6.2: EDS spectrum of πΆππ2 (as received)
The BET adsorption-desorption isotherm is shown in Figure 6.3.
Figure 6.3: BET adsorption (solid trace) - desorption (dashed trace) of πΆππ2 (as received)
0.0
5.0
10.0
15.0
20.0
25.0
0 0.2 0.4 0.6 0.8 1
Qu
anti
ty a
dso
rbed
/ c
m3 g
-1
Relative pressure / (P/Po)
Chapter 6 Oxide Powder Characterisation 7131060
120
The isotherm in Figure 6.3 is a type three isotherm [65]. This indicates that adsorbate
molecules have a higher affinity for themselves rather than the surface of the sample [48].
When the relative pressure nears 1, the adsorbate molecules finally adhere to the surface in
large quantities. It is clear from the desorption isotherm (dashed trace) that there is
hysteresis in the isotherm, indicating the sample has a mesoporous nature [48].
The calculated BET surface area is 6.33 Β± 0.02 m2 g-1.
The DRIFT spectra of the πΆππ2 (as received) is highlighted in Figure 6.4.
Figure 6.4: DRIFT spectra of πΆππ2 (as received)
The broad band at approximately 3500 cm-1 is the stretching mode of π β π» and arises from
the adsorbed water on the oxide surface [66]. The water is present as water of
crystallisation or intra-molecular bound water. The sharp inverse band at 2300 cm-1 is due to
the asymmetrical stretching band of πΆπ2 present in the atmosphere and is used as a
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
2.0
2.2
5001000150020002500300035004000
Ref
lect
ance
/ %
Wavenumber / cm-1
Chapter 6 Oxide Powder Characterisation 7131060
121
reference to align the module [67]. The bands present between 1700-1300 cm-1 are a
mixture of πΆ β π and π β π vibrational modes. Nitrate and carbonate moieties exhibit
similar vibrational bands when adsorbed to metal oxides [68]. When πΆπ2 adsorbs to a
surface where water is present, it can have several forms; linear πΆπ2, carbonate (πΆπ32β),
bicarbonate (π»πΆπ3β) and carboxylate species (πΆπ2
β). These species have bands representing
asymmetrical stretching (1415 cm-1), π = πΆ = π bending (1700-1200 cm-1) and symmetrical
and asymmetrical π β π» bending bands (1655-1370 cm-1) from interaction with surface
hydroxyl groups [68]. ππ2 adsorbed onto metal oxides has three distinct bands in the
region, at 1680, 1400 and 1320 cm-1, representing asymmetrical ππ2 stretching, π β π»
bending and symmetrical ππ2 stretching respectively [69]. The broad signal present at 650
cm-1 is the stretching mode of πΆπ β π β πΆπ [66]. This is the dominant signal as it is the
dominant bond in the oxide powder.
It is evident from Figure 6.4 that there are several adsorbed species on πΆππ2 (as received)
surface in addition to water, namely πΆπ2and πππ₯. High temperatures are required to
remove water completely, however, this procedure may affect other properties of the
oxide. It is not known how strongly the other species are adsorbed to the surface and
whether they are removed when placed under vacuum on the manifold prior to
investigation of π»2 β π2 β π΄π experiments.
6.1.2 Regenerated πͺππΆπ Properties
Experiments investigating the radiolysis of air used regenerated oxide powders which had
been washed and baked according to Section 3.4.3. Therefore, it was of importance to
characterise the regenerated oxide and determine if this process had any effects on the
oxide properties.
Chapter 6 Oxide Powder Characterisation 7131060
122
Section 3.4.2 outlined the methodology employed to investigate the radiolysis of air over an
oxide surface. To determine the quantity of oxide powder needed to produce the 50% and
90% (by volume) oxide samples, the bulk density of the powder was required. This
parameter was determined by filling a known volume with oxide and recording its weight.
The bulk density of regenerated πΆππ2 was calculated as 1.424 Β± 0.005 g cm-3. This value is
much lower than the crystal density of πΆππ2 which is 7.215 g cm-3, arising from the inability
of the powder to pack as tightly as a single crystal.
Figure 6.5: SEM images of regenerated πΆππ2 illustrating the macrostructure of the powder (top) and a large particle (bottom)
Chapter 6 Oxide Powder Characterisation 7131060
123
Figure 6.5 illustrates two electron micrographs from the regenerated oxide. There is no
dominant morphology within the sample with well-defined edges and irregular shaped
grains being dominant.
Changes in the surface area of the powder are significant as this may affect the catalytic
properties (if any) of the oxide in determining the gas phase radiation chemistry. Figure 6.6
illustrates the adsorption-desorption isotherm for regenerated πΆππ2. The BET surface area
for the regenerated πΆππ2 is 7.42 Β± 0.02 m2 g-1.
Figure 6.6: BET adsorption (solid trace) β desorption (dashed trace) isotherm for regenerated πΆππ2
The isotherm in Figure 6.6 is identical in shape to the isotherm generated from πΆππ2 (as
received).
0.0
2.0
4.0
6.0
8.0
10.0
12.0
14.0
16.0
18.0
20.0
0 0.2 0.4 0.6 0.8 1
Qu
anti
ty a
dso
rbe
d /
cm
3 g
-1
Relative pressure / (P/Po)
Chapter 6 Oxide Powder Characterisation 7131060
124
Figure 6.7 illustrates the results from thermogravimetric analysis of regenerated πΆππ2
decomposed under static air and π2 up to 1000 Β°C:
Figure 6.7: Thermogram of regenerated πΆππ2 decomposed under π2 (blue) and static air (red). Heating rate 10 Β°C min-1
It is clear from this figure, that there are no impurities or vast quantity of adsorbed species
on regenerated πΆππ2, with the mass change being Β± 0.5% from the initial mass.
Figure 6.8 shows the DRIFT spectra measured for regenerated πΆππ2. It highlights the nature
of any adsorbed species on the oxide surface:
98.0
98.5
99.0
99.5
100.0
100.5
101.0
101.5
102.0
0 100 200 300 400 500 600 700 800 900 1000
Mas
s /
%
Temperature / oC
N2
Air
Chapter 6 Oxide Powder Characterisation 7131060
125
Figure 6.8: DRIFT spectrum of regenerated πΆππ2
All of the absorption bands present in Figure 6.8 have previously been assigned in Figure
6.4.
6.1.3 Comparison of βAs Receivedβ and Regenerated πͺππΆπ
It is noticeable when comparing SEM images in Figures 6.1 and 6.5 that larger agglomerated
particles are present in the regenerated πΆππ2 that were not observed in the oxide before
washing and baking. The surface area of the faces has increased from 3 to 300 Β΅m2. This
increase is likely to be an effect of heating the oxide and causing grains to combine and
agglomerate.
Although the particle size has increased in the regenerated oxide, the BET surface area
remained within 10% of the πΆππ2 (as received) after five subsequent regeneration cycles.
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
2.0
5001000150020002500300035004000
Re
fle
ctan
ce /
%
Wavenumber / cm-1
Chapter 6 Oxide Powder Characterisation 7131060
126
The bulk density of the regenerated oxide is within 1% of the πΆππ2 (as received),
highlighting that the regeneration process has little effect on the oxide properties.
There was very little difference between the DRIFT spectra of πΆππ2 (as received) and
regenerated πΆππ2 (Figures 6.4 and 6.8). Both spectra had identical absorption bands
indicating that the regeneration cycle outlined in Section 3.4.3 has no effect on the
concentration or identity of adsorbed species on πΆππ2. Figure 6.9 highlights DRIFT spectra
of an identical sample of πΆππ2 (as received) that has undergone five subsequent
regeneration cycles. A sample was taken after each cycle and anaylsed.
Figure 6.9: DRIFT spectra of πΆππ2 (as received) and regenerated πΆππ2 up to five subsequent regeneration cycles
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
2.0
5001000150020002500300035004000
Re
fle
ctan
ce /
%
Wavenumber / cm-1
As received Regen. 1
Regen. 2 Regen. 3
Regen. 4 Regen. 5
Chapter 6 Oxide Powder Characterisation 7131060
127
It is clear from Figure 6.9, that the regeneration process has no effect on the oxide powder
as no new bands are detected. Absorption bands present in πΆππ2 (as received) have not
diminished after consecutive washing and baking.
6.2 Properties of πππΆπ
6.2.1 As Received
To ascertain the purity and morphology of the as received πππ2, SEM and EDS analysis were
undertaken.
Figure 6.10: SEM image of πππ2 (as received)
An SEM image of βas receivedβ πππ2 is shown in Figure 6.10. The πππ2 particles have a
defined rod like structure, and range in size from 10 to 40 Β΅m in length.
Chapter 6 Oxide Powder Characterisation 7131060
128
The EDS spectrum of πππ2 is shown in Figure 6.11. It indicates that there are no major
impurities in the powder, with zirconium and oxygen being the only detectable elements in
the sample, apart from the carbon stub.
Figure 6.11: EDS spectrum of πππ2 (as received)
Figure 6.12 highlights the adsorption-desorption isotherm for πππ2 (as received). The
calculated BET surface area for this powder was 2.02 Β± 0.04 m2 g-1.
Figure 6.12: BET adsorption (solid trace) β desorption (dashed trace) isotherm of πππ2 (as received)
0.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
0 0.2 0.4 0.6 0.8 1
Qu
anti
ty a
dso
rbed
/ c
m3 g
-1
Relative pressure / (P/Po)
Chapter 6 Oxide Powder Characterisation 7131060
129
Like the adsorption isotherms highlighted for πΆππ2 (Figures 6.3 and 6.6), this isotherm is
also type three. The features of which, were discussed after Figure 6.3.
The DRIFT spectra of πππ2 (as received) is highlighted in Figure 6.13.
Figure 6.13: DRIFT spectrum of πππ2 (as received)
The broad band at approximately 3500 cm-1 is the stretching mode of π β π» and arises from
the adsorbed water on the oxide surface [66]. The water is present as water of
crystallisation or intra-molecular bound water. The band present between 1700-1400 cm-1 is
a mixture of πΆ β π and π β π vibrational modes. Nitrate and carbonate moieties exhibit
similar vibrational bands when adsorbed to metal oxides [68]. When πΆπ2 adsorbs to a
surface where water is present, it can have several forms; linear πΆπ2, carbonate (πΆπ32β),
0
0.2
0.4
0.6
0.8
1
1.2
5001000150020002500300035004000
Re
fle
ctan
ce /
%
Wavenumber / cm-1
Chapter 6 Oxide Powder Characterisation 7131060
130
bicarbonate (π»πΆπ3β) and carboxylate species (πΆπ2
β). These species have bands representing
asymmetrical stretching (1415 cm-1), π = πΆ = π bending (1700-1200 cm-1) and symmetrical
and asymmetrical π β π» bending bands (1655-1370 cm-1) from interaction with surface
hydroxyl groups [68]. ππ2 adsorbed onto metal oxides has three distinct bands in the
region, at 1680, 1400 and 1320 cm-1, representing asymmetrical ππ2 stretching, π β π»
bending and symmetrical ππ2 stretching respectively [69]. All of these bands are visible in
Figure 6.13, however, some are stronger than others.
6.2.2 Regenerated πππΆπ Properties
As with πΆππ2 , it is important to characterise the regenerated oxide powder and to
determine if the regeneration process changes any of the oxide properties. The bulk density
of regenerated πππ2 has been calculated as 2.059 Β± 0.007 g cm-3, which is approximately
35% of the crystal density (5.68 g cm-3) for the reasons explained in Section 6.1.2 for πΆππ2.
Figure 6.14 illustrates the morphologies of particles of regenerated πππ2:
Chapter 6 Oxide Powder Characterisation 7131060
131
Figure 6.14: SEM images of regenerated πππ2 illustrating large agglomerated particles
The dominant morphology of regenerated πππ2 is large agglomerated particles with well-
defined faces.
Chapter 6 Oxide Powder Characterisation 7131060
132
Figure 6.15: EDS spectrum of regenerated πππ2
Figure 6.15 shows the EDS spectrum of the regenerated πππ2. The most distinguishing
feature of Figure 6.15 is the presence of sodium in the regenerated πππ2. This impurity is
attributable to the regeneration process, where the oxide is washed with an aliquot of
5 mM ππππ» to remove any adsorbed organics from the surface. The powder is washed
with copious amounts of deionised water to remove any excess sodium, however, it is clear
that πππ2 has a large affinity for sodium cations which are likely to adsorb onto the oxide
surface.
The thermogravimetric analysis results of regenerated πππ2 decomposed under static air
and π2 are displayed in Figure 6.16:
Chapter 6 Oxide Powder Characterisation 7131060
133
Figure 6.16: Thermogram of regenerated πππ2 decomposed under π2 (blue) and static air (red). Heating rate 10 Β°C min-1
As seen in Figure 6.7, there are no large impurities or adsorbed species in samples of
regenerated πππ2. The mass difference is within Β± 0.5%.
Figure 6.17 is the adsorption-desorption isotherm for regenerated πππ2. The resulting BET
surface area was 2.24 Β± 0.02 m2 g-1.
99.0
99.2
99.4
99.6
99.8
100.0
100.2
100.4
100.6
100.8
101.0
0 200 400 600 800 1000
Mas
s /
%
Temperature / oC
N2
Air
Chapter 6 Oxide Powder Characterisation 7131060
134
Figure 6.17: BET adsorption (solid trace)-desorption (dashed trace) isotherm of regenerated πππ2
The isotherm depicted in Figure 6.17 is of type three. There is a hysteresis loop in the
isotherm, indicating the sample has a mesoporous nature.
The DRIFT spectra for regenerated πππ2 is depicted in Figure 6.18.
0.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
9.0
0 0.2 0.4 0.6 0.8 1
Qu
anti
ty a
dso
rbed
/ c
m3
g-1
Relative pressure / (P/Po)
Chapter 6 Oxide Powder Characterisation 7131060
135
Figure 6.18: DRIFT spectrum of regenerated πππ2
The absorption bands present in Figure 6.18 have all been identified and assigned in Figure
6.13 for πππ2 (as received).
6.2.3 Comparison of βAs Receivedβ and Regenerated πππΆπ
Comparing Figure 6.10 and Figure 6.14, the regenerated πππ2 has larger particle sizes than
the fresh oxide powder. The rod-like morphology is still present in regenerated πππ2,
however, larger agglomerated particles have been observed. These agglomerated particles
have faces with surface areas of at least 400 Β΅m2 which is an order of magnitude above the
particles observed in Figure 6.10. Although the particles of the regenerated oxide are an
order of magnitude larger than πππ2 (as received), they still have defined faces and appear
to be agglomerations of smaller particles.
0.0
0.2
0.4
0.6
0.8
1.0
1.2
5001000150020002500300035004000
Ref
lect
ance
/ %
Wavenumber / cm-1
Chapter 6 Oxide Powder Characterisation 7131060
136
The largest difference between the βas receivedβ and regenerated πππ2 is highlighted in the
EDS spectra (Figures 6.11 and 6.15). The regeneration process has led to sodium being
retained by the oxide.
The bulk density value for the regenerated oxide is within 1% of the πππ2 (as received).
The surface area of πππ2 has not been altered too greatly by the regeneration process.
πππ2 (as received) had a surface area of 2.02 Β± 0.04 m2 g-1, this had changed to 2.24 Β± 0.02
m2 g-1 after four regeneration cycles. There was no direct increase or decrease in surface
area after subsequent regeneration cycles indicating that the change in macro particle size
and the uptake of sodium onto the oxide surface has no effect on these properties.
There is very little difference between the DRIFT spectra of πππ2 (as received) and
regenerated πππ2 (Figures 6.13 and 6.18). To highlight the effect (if any) of the
regeneration cycle has on the adsorbed species on πππ2, Figure 6.19 highlights the DRIFT
spectra of a sample of πππ2 (as received) that has undergone four subsequent
regeneration cycles, with a sample taken after each cycle and analysed.
Chapter 6 Oxide Powder Characterisation 7131060
137
Figure 6.19: DRIFT spectra of πππ2 (as received) and regenerated πππ2 up to four subsequent regeneration cycles
This figure highlights that the regeneration process has no effect on the concentration or
identity of adsorbed species on πππ2.
6.3 Comparison of Regenerated πͺππΆπ and πππΆπ
The major effect of the regeneration process outlined in Section 3.4.3 is the formation of
large agglomerated particles. This occurs with both πΆππ2 and πππ2 and leads to particles
with well-defined faces of surface area 300 ΞΌm2 and 400 ΞΌm2, respectively. The
regeneration process also leads to sodium uptake in πππ2 but not in πΆππ2. This uptake does
0.0
0.2
0.4
0.6
0.8
1.0
1.2
5001000150020002500300035004000
Re
fle
ctan
ce /
%
Wavenumber / cm-1
As received
Regen. 1
Regen. 2
Regen. 3
Regen. 4
Chapter 6 Oxide Powder Characterisation 7131060
138
not affect the surface area of πππ2. The BET surface area is three times greater for πΆππ2
(7.42 m2 g-1) than πππ2 (2.24 m2 g-1) highlighted by the quantity of π2 adsorbed; 18 cm3 g-1
for πΆππ2 compared to 8 cm3 g-1 with πππ2. This reflects the larger surface area and more
porous nature of πΆππ2.
πππ2 has a slightly higher bulk density than πΆππ2 (2.06 g cm-3 compared to 1.42 g cm-3)
which means a larger mass of πππ2 is required for air radiolysis experiments containing 50
and 90% (by volume) of oxide.
The thermograms of both πΆππ2 and πππ2 highlighted that both oxides were of high purity
with little or no adsorbed organic species present.
The DRIFT spectra of regenerated πΆππ2 and πππ2 highlight that π»2π, πΆπ2 and πππ₯ are
present as adsorbed species on both oxides. These bands were also present in the βas
receivedβ powders, therefore are not due to regenerating the oxide powders. There are
more adsorption bands present in the regenerated πΆππ2 spectrum (Figure 6.8) than in the
regenerated πππ2 spectrum (Figure 6.18) highlighting the fact that the adsorption is more
dominant for πΆππ2 than πππ2.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
139
7 π―2 β πΆ2 Radiolysis Results and Discussion
The following chapter details the results of radiolysis of π»2-π2 gas mixtures in an argon
matrix in the presence or absence of an oxide surface. The initial focus of this chapter is
discussion of the radiolysis of ethylene results outlined in Chapter Five in comparison to
those results attained using the Fricke dosimeter. The chapter discusses the sources of error
in the experimental configuration and the mechanism of ethylene radiolysis. Finally the
chapter outlines preliminary trials of π»2 - π2 gas radiolysis using an ion accelerator as the
radiation source and discusses the use of ethylene as a chemical dosimeter compared to
absolute current measurements for accelerator dosimetry. The relevance of these results
are discussed and interpreted throughout the chapter with a final conclusion given at the
end.
7.1 Discussion of πͺππ―π Dosimetry in Comparison with Fricke
Dosimetry
Comparison of the ethylene dosimetry results in Figure 5.3 against those attained using the
Fricke dosimeter seen in Figure 5.1 (both reproduced in Figure 7.1) illustrates that there is a
good agreement between the calculated dose rates of the two dosimeters.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
140
i)
ii)
Figure 7.1: Comparison of dose rates obtained by different chemical dosimeters (units Gy min-1) i) Fricke dosimetry and ii) ethylene dosimetry (dose rates correct as of 17th February
2015)
It is clear from Figure 7.1 that there is very good agreement between the two dosimeter
systems utilised. The small difference in dose rate can be attributed to the different vessels
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
141
used in each measurement. As stated previously, in gaseous samples, the majority of the
absorbed dose comes from secondary electrons ejected by the vessel wall [57], therefore
the difference in density between the glass vials used for Fricke dosimetry and the steel
vessels used for ethylene dosimetry will have an effect on the secondary electron yield.
Another difference is the irradiated volume of the sample. In the Fricke dosimeter
experiments, only 3 ml of solution was irradiated in the 12 ml glass vials, however, for the
ethylene experiments, the entire gas volume is irradiated. As seen in Figure 7.1i, there is
lateral dependence on dose rate inside the chamber as well as depth dependence.
Therefore it is entirely plausible that there will be a vertical dependency on dose rate as
well.
The majority of the focus in Section 5.3 has been on determining the absorbed dose in a
sample. The dose rate is determined by dividing the absorbed dose by the irradiation time,
however, little attention has been given to errors associated with the time constituent. The
program that controls the 60πΆπ irradiator can set irradiations to last a certain time required
within a second of accuracy. The two source rods are raised into the chamber independently
of each other and rely on an air compressor to do so. The speed of which the rods raise is
dependent on the compressor pressure and can alter the speed by up to a second. Within
this second, the sources are still emitting Ξ³βrays which are being absorbed by the sample.
For short irradiations such as that employed by Fricke dosimetry where irradiations can last
up to a minute, this time error becomes more significant than the time error associated with
ethylene experiments, where irradiation times are at least one hour in length. The minimum
error associated with the time coefficient of Fricke measurements is 3%. This could explain
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
142
why the dose rates did not unilaterally increase or decrease between the dosimeters as the
source rods may have risen slower during one dosimeter experiment and not the other.
7.2 Source of Errors in Ethylene Dosimetry
After collating several results from ethylene radiolysis experiments, it became apparent that
there was disagreement in several samples across the multiple injections with respect to π»2
concentration in the GC sample loop. Figure 7.2 is a plot of the scatter in each sample
against the peak area of π»2 from the first injection of that sample for three different
irradiation times.
Figure 7.2: Plot of scatter in each sample of ethylene as a function of the peak area of π»2 in the first injection
From this figure, two observations can be made. Firstly, after the first injection of the
sample, if the π»2 peak area is less than 10 AU, there is a higher disagreement between the
pressure in the sample loop and the peak area of π»2 for subsequent injections. The scatter
0.0
2.0
4.0
6.0
8.0
10.0
12.0
14.0
0.00 10.00 20.00 30.00 40.00 50.00 60.00
RSD
of
resu
lts
fro
m r
un
/ %
H2 peak area from first injection / AU
540 min
3900 min
5760 min
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
143
varies between 1-13%. When the initial π»2 peak area is at least double this figure, the
scatter is always less than 2%. This trend could infer that the lower detection limit of the GC
detector is being reached as there is a larger error in smaller signals. Figure 7.3 is an overlay
of three chromatograms from three subsequent injections of a post irradiated ethylene
sample (irradiated for 540 min).
Figure 7.3: Gas chromatogram overlay of three subsequent injections of post irradiated ethylene highlighting the π»2 signal
With subsequent injections, the baseline becomes less stable as the signal to noise ratio
increases. This effect is highlighted further in Figure 7.4, which shows the chromatogram
profile of the π»2 signal for the first injection of two different samples:
-1000
-500
0
500
1000
1500
2000
2500
3000
3500
4000
20 25 30 35 40 45 50 55 60
Sign
al In
ten
sity
/ A
U
Retention time / s
1st injection
2nd injection
3rd injection
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
144
i)
ii)
Figure 7.4: Gas chromatogram of two separate ethylene samples irradiated for i) 540 min and ii) 5760 min
The red bands in Figure 7.4 are the bounding limits of the noise in the chromatogram. As
can be seen in Figure 7.4i, a larger percentage of the π»2 signal is within this noise limit
compared to the π»2 signal in 7.4ii. With subsequent injections, as the signal gets smaller, a
greater portion will lie within the noise limit. The sample represented by Figure 7.4i had
12.4% scatter across all three injections as the signal to noise ratio decreased. The sample
-500
0
500
1000
1500
2000
2500
3000
20 25 30 35 40 45 50 55 60
Sign
al In
ten
sity
/ A
U
Retention time / s
-1000
2000
5000
8000
11000
14000
17000
20 25 30 35 40 45 50 55 60
Sign
al In
ten
sity
/A
U
Retention time / s
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
145
represented by Figure 7.4ii had 0.7% scatter across all three injections as the signal
outweighed the noise limits of the instruments.
The second observation that can be made from Figure 7.2 is that longer irradiation times
lead to larger π»2 peak areas for the first injection. This is to be expected as the sample is in
the radiation field for longer therefore more of the ethylene will undergo radiolysis.
As there is no back reaction to reform ethylene, a steady state will not be reached in the
system.
To ascertain more accurate and reproducible results for the ethylene dosimeter, a larger
quantity of hydrogen needs to be measured to reduce the interference from the signal/
noise ratio of the GC. This can be attained by two methods. The first is to irradiate the
samples for longer periods of time to ensure a greater percentage of ethylene undergoes
radiolysis. This is not feasible however, due to scheduling conflicts with the irradiation
source and also the linear range of the dosimeter. As mentioned in Section 4.1, the Fricke
dosimeter has a linear oxidation rate between 0-400 Gy; the ethylene dosimeter has a linear
range of π»2 formation between 5-200 kGy [12]. For the central two positions in the rack,
any irradiation time over 11 h leads to the dosimeter being out of range and the value of
G(π»2) = 1.36 is obsolete. To circumvent the issue of shorter irradiation times to increase π»2
production a second method is employed. Previously, all samples have been irradiated at
atmospheric pressure (1 bar); therefore by increasing the pressure inside the sample vessel
there is a larger number of ethylene molecules that can undergo radiolysis. The results of
experiments at higher pressures are shown in Figure 7.5:
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
146
Figure 7.5: Results of ethylene dosimetry at increased pressure (units β Gy min-1) (dose rates correct as of 24th February 2015)
These dose rates are put into the same decay series spreadsheet as the Fricke results to
determine the dose rate on a given date. These dose rates are used to determine the
absorbed dose by a particular sample during the course of π»2 β π2 β π΄π radiolysis
experiments. This decay series is then validated once a month with single point dosimetry.
7.3 Mechanism of Ethylene (πͺππ―π) Radiolysis
It is important to understand the mechanism of ethylene radiolysis and what factors may
affect the yield of π»2 produced with it being used as dosimeter for π»2 - π2 radiolysis
experiments.
Work has been carried out to investigate the decomposition products in the radiolysis of
ethylene. It is understood that the primary products are π»2, acetylene (πΆ2π»2), and higher
molecular weight polymeric products [61]. It is widely agreed that π»2 is formed from direct
molecular elimination processes (Reaction 7.1 and 7.2):
πΆ2π»4 β πΆ2π»2 + π»2 Reaction 7.1
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
147
πΆ2π»4 β πΆπ»2πΆ + π»2 Reaction 7.2
The hydrogen atoms can be eliminated from separate carbon atoms (Reaction 7.1) or both
can come from a single carbon atom (Reaction 7.2) [13]. However, both hydrogen atoms are
eliminated from a single ethylene molecule. This has been investigated with isotopic
experiments where 50:50 mixtures of πΆ2π»4 and πΆ2π·4 have been irradiated [70]. Mass
spectroscopic data showed that 95% of the decomposition product was either π»2 or π·2
with only 5.2% being π»π·. The yield of πΆπ»πΆπ· was also very low, which suggested that the
methylene species (πΆπ»2 or πΆπ·2), was not involved in the production of acetylene. The
product in Reaction 7.2 (πΆπ»2πΆ) can rearrange to form acetylene πΆ2π»2 [71] which accounts
for roughly 10% of the ethylene reacted. The remaining 90% undergoes condensation
reactions to form higher molecular weight products [70]. The formation of π»2 by molecular
elimination has also been observed in the photolysis of ethylene gas using a xenon lamp
source [72].
Alongside Reactions 7.1 and 7.2, the radiolysis of ethylene can produce a primary excitation
process which leads to hydrogen atom formation (Reactions 7.3 and 7.4) [73]:
πΆ2π»4 β πΆ2π»4β β πΆ2π»2 + 2π»β Reaction 7.3
β πΆ2π»4β β πΆ2π»3
β + π»β Reaction 7.4
The hydrogen atom yield has been calculated as G(π»β) = 6.8. This atomic species reacts very
rapidly with ethylene to form the ethyl radical (πΆ2π»5. ), (Reaction 7.5) [62, 74, 75]:
π»β + πΆ2π»4 β πΆ2π»5β Reaction 7.5
The ethyl radical can undergo recombination and disproportionation reactions with other
radical species such as the vinyl (πΆ2π»3β ), and methyl (πΆπ»3
β ), to form the higher molecular
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
148
weight polymeric and unsaturated hydrocarbon products. It can also react with the
hydrogen atom to form ethane (Reaction 7.6):
π»β + πΆ2π»5β β πΆ2π»6 Reaction 7.6
This reaction (7.6) has been shown to occur via radical recombination by Yang et al. [75]
who added nitric oxide (ππ), to the system to act as a radical scavenger. Their results
showed firstly, that with addition of ππ, ethane was not formed and secondly, that the
yields of π»2 and πΆ2π»2 were not affected by the addition of ππ to the system. This suggests
that the recombination of hydrogen atoms to form π»2 does not occur.
Alongside excitation reactions, formation of fragmented ions can occur [74]:
πΆ2π»4 β πΆ2π»2+ + 2π»β + πβ Reaction 7.7
The ethyl cation can then react with ethylene as seen in Reaction 7.8.
πΆ2π»2+ + πΆ2π»4 β πΆ3π»5
+ + πΆπ»3β Reaction 7.8
These products can then go on to form higher molecular weight species.
From this reaction scheme it can be seen that ethylene radiolysis is well understood and the
majority of products are gaseous hydrocarbon species. Due to their size, these products will
not interfere with π»2 analysis as they will not get through the packed column of the GC.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
149
7.4 π―π Production from Adsorbed Water on Oxide Powders
Before experiments were undertaken investigating the radiation chemistry of π»2 β π2 β π΄π
gas mixtures in contact with an oxide surface, it was important to determine the quantity of
π»2 produced from adsorbed water radiolysis and whether this concentration affects the
measurements of π»2 initially added to the system.
The metal vessels in Figure 4.11 were filled with the relevant oxide to capacity using the
bulk density calculated in Chapter Six. The vessels were assembled and attached to the gas
mixing manifold (Figure 4.18). The samples were placed under vacuum to remove the
headspace and any physisorbed species on the oxide surface. After approximately 30 min
under vacuum, the vessels were filled with argon to atmospheric pressure (1 bar absolute)
and irradiated for different periods of time. Only the dose absorbed by the adsorbed water
was considered. To determine this value, the mass of water adsorbed onto the oxide
powder needed to be determined. It is assumed that 1 monolayer of water will be adsorbed
onto the oxide due to the relative humidity of the laboratory and the vacuum pump
removing any physisorbed species. Haschke and Ricketts have determined the mass of one
water monolayer as 0.21 mg m-2 adsorbed onto ππ’π2 powder [23]. Due to the similarities in
crystal structure, lattice parameters and surface area, this value is a good approximation for
the mass of one water monolayer adsorbed onto πΆππ2 and πππ2. Knowledge of the SSA and
mass of oxide powder in each sample allows for the mass of water in each sample to be
determined and therefore, the absorbed dose. The results of these experiments are shown
in Figure 7.6.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
150
Figure 7.6: Hydrogen production as a function of absorbed dose1 from water adsorbed to πππ2 (primary y-axis) and πΆππ2 (secondary y-axis)
There are two distinct features from the results shown in Figure 7.6. Firstly, the yield of π»2
from water adsorbed onto πΆππ2 is at least an order of magnitude below the yield from
πππ2 and has to be plotted on a second axis. One possible hypothesis is; there is more
water adsorbed onto πππ2 than πΆππ2, therefore more π»2 can be produced by radiolysis.
Using the value of Haschke and Ricketts of 0.21 mg m-2 for the mass of one monolayer [23]
and the surface area of each oxide determined in Chapter Six; the surface area present in
each sample is 90 and 45 m2 for πΆππ2 and πππ2, respectively. From these values, the mass
of water adsorbed can be determined and assuming π»2 formation from water radiolysis
occurs via Reaction 7.9; then the maximum number of π»2 molecules that could be formed is
6.3x1020 and 3.15x1020 molecules in samples containing πΆππ2 and πππ2, respectively.
2π»2ππππ β 2π»2 (π) + π2 (π) Reaction 7.9
1 Throughout this Chapter, in all plots of species production/depletion as a function of absorbed dose, the absorbed dose
axis has been plotted in units of 100 eV so that G-values for the species in question can be determined from the gradient of the trend line of the data.
0.0
5.0
10.0
15.0
20.0
25.0
30.0
35.0
40.0
45.0
50.0
0.0
500.0
1000.0
1500.0
2000.0
2500.0
0.0 10.0 20.0 30.0 40.0 50.0 60.0 70.0 80.0 90.0
H2 p
rod
uct
ion
/ (
x10
16)
mo
lec.
H2 p
rod
uct
ion
/ (
x10
16)
mo
lec.
Absorbed Dose / (x1016) 100 eV
ZrO2
CeO2
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
151
From these values it is clear that there is sufficient water in 1 monolayer to produce the
quantity of π»2 that has been measured with the reaction efficiency calculated as 0.03 and
6.35% for adsorbed water radiolysis on πΆππ2 and πππ2, respectively.
The explanation for greater π»2 production from πππ2 than πΆππ2 is due to an increase in
energy transfer from the oxide to the adsorbed species. This has been investigated by
LaVerne and Tandon [29] who found πππ2 produced five times more π»2 than πΆππ2 for the
same quantity of adsorbed water using 60πΆπ Ξ³-rays. Petrik et al. have attributed this
phenomena partly to the resonance between the band gap of πππ2 (5.0 eV) [76] and the
bond dissociation energy of water (π»π β π») (5.15 eV) [27]. The band of πΆππ2 is in the range
3.1-3.5 eV [77]. Therefore, not enough energy can be transferred from πΆππ2 to adsorbed
water to enhance the formation of π»2. However, LaVerne et al. [29] state that other metal
oxides with a band gap inside this range does not increase the yield of π»2. Chelnokov et al
[78] investigated the electron transfer at the interface between liquid water and several
metal oxides with band gaps ranging between 3.3-9.0 eV under the influence of ionising
radiation. They found that the interaction between the radiation field and the oxide
nanoparticles produces secondary electrons with enough energy to transfer across to the
water independent of oxide band gap. This electron transfer led to increased yields of
solvated electrons (πππβ ), across all oxides normalised to that of pure water. Other
explanations such as exciton formation and water adsorption form have also been given. It
is widely agreed that an energy transfer mechanism is responsible for these results,
however, no conclusions as to the nature of this mechanism has received widespread
acceptance.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
152
The second feature of Figure 7.6 is the scattered nature of π»2 yields from water adsorbed to
πππ2. There appears to be a positive correlation between absorbed dose and production of
π»2 from πππ2, however, there is a large variance in the quantity of π»2. It is possible that
there are differing quantities of π»2π adsorbed across all the samples. The oxides were not
treated beforehand, therefore, removal of adsorbed water was reliant solely on the vacuum
pump. This parameter may become important, however, for this research it is important to
qualify the amount of π»2 that can be produced from adsorbed water radiolysis.
It is important to note that π2 is not detected (or below the limits of detection of the gas
chromatograph) in samples of either πΆππ2 or πππ2. This effect has been highlighted by
other researchers investigating radiolysis of adsorbed water on metal oxide surfaces
[25, 29]. This has led to debate as to the location of π2. One hypothesis is that π2 oxidises
the metal oxide, leading to the formation of the super-stoichiometric ππ2+π₯ product [79]. A
second hypothesis is the formation of interstitial hydroxyl groups leading to a product with
chemical formula ππ2(ππ») [80]. This has not been studied further as the primary concern
is π»2 formation.
7.5 Radiolysis of Ethylene in Contact with Oxides
To help elucidate a better understanding of dosimetry in heterogeneous systems, and the
dose received by the overlying gas phase in contact with an oxide powder, ethylene gas was
added to sample vessels which contained either πΆππ2 or πππ2. The vessels were filled to
capacity with the relevant oxide and sealed for the duration of experiments investigating
ethylene radiolysis. The mass of each oxide was noted to determine the volume occupied by
oxide. The volume of ethylene was calculated by subtracting the volume of oxide (using the
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
153
crystal density) from the reaction vessel volume. The corrected volume of ethylene was
used to determine the mass of ethylene and the absorbed dose.
Figure 7.7 shows the resulting chromatograms for a sample containing pure ethylene
(πΆ2π»4), a vessel containing πΆππ2 in an argon atmosphere and a vessel containing πΆππ2 in an
πΆ2π»4 atmosphere. The vessel volume was identical in all three samples and the mass of
πΆππ2 in the two heterogeneous systems was the same. All three samples were irradiated at
the same pressure for an identical time period in the same position in the test tube array.
Figure 7.7: Gas chromatograms showing a comparison of the π»2 signal of irradiated ethylene (πΆ2π»4) (blue trace), πΆππ2 in π΄π atmosphere (green trace) and πΆππ2 in ethylene
(πΆ2π»4) (red trace) irradiated for 9 h in identical radiation fields
In the figure above, the chromatograms are taken from the first injection of each sample,
where the quantity of π»2 is at its greatest. Each chromatogram has been normalised to the
same sample loop pressure (that of ethylene (blue trace)) so that the variables between
samples remains at a minimum.
Section 7.4 highlighted the presence of adsorbed water on πΆππ2 which can lead to small
quantities of π»2 being produced. The efficiency of the reaction is not great and only a small
0.0
5.0
10.0
15.0
20.0
25.0
30 35 40 45 50
Sign
al In
ten
sity
/ A
U
Retention time / seconds
CeO2 - C2H4
CeO2 - Ar
C2H4
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
154
proportion of the adsorbed water is radiolysed. This is evident from Figure 7.7 where the
yield of π»2 from adsorbed water is approximately half the yield of π»2 from pure ethylene
radiolysis. Figure 7.7 also highlights that the π»2 generated from ethylene radiolysed in
contact with πΆππ2 (red trace) is greater than the sum of π»2 generated from pure ethylene
radiolysis and adsorbed water radiolysis.
Figure 7.8 is the parallel study using πππ2 as the oxide surface.
Figure 7.8: Gas chromatograms showing a comparison of the π»2 signal of irradiated ethylene (πΆ2π»4) (blue trace β secondary y-axis), πππ2 in π΄π atmosphere (green trace β
secondary y-axis) and πππ2 in ethylene (πΆ2π»4) (red trace β primary y-axis) irradiated for 9 h in identical radiation fields
The chromatograms in Figure 7.8 have been normalised to the same sample loop pressure
(that of ethylene (blue trace)) for the reason mentioned previously.
In Figures 7.7 and 7.8, the chromatogram from ethylene (blue trace) is the same sample.
This allows a comparison to be made between πΆππ2 and πππ2 samples under identical
conditions. As seen in Section 7.4, the yield of π»2 from adsorbed water on πππ2 is at least
0.0
5.0
10.0
15.0
20.0
25.0
30.0
35.0
40.0
45.0
50.0
0.0
400.0
800.0
1,200.0
1,600.0
2,000.0
2,400.0
30 35 40 45 50 55Si
gnal
Inte
nsi
ty /
AU
Sign
al In
ten
sity
/ A
U
Retention time / seconds
ZrO2 - C2H4
ZrO2 - Ar
C2H4
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
155
five times greater than a parallel πΆππ2 sample in Figure 7.7. The stand-out feature of Figure
7.8, is the chromatogram of πππ2 β πΆ2π»4 (red trace), which is plotted on the primary
vertical axis whereas the chromatograms of irradiated πππ2 in an argon atmosphere and
πΆ2π»4 gas only are plotted on the secondary vertical axis. From the scale of these axes, it is
noted that the yield of π»2 from ethylene is almost 450 times greater in the presence of
πππ2 than with no oxide present. In concurrence with πΆππ2 results, this yield is greater than
the sum of ethylene radiolysis and adsorbed water radiolysis.
The increase in π»2 production from adsorbed water on πππ2 in comparison to πΆππ2 is partly
attributed to the resonance between the band gap of πππ2 and the bond dissociation of
water as discussed earlier. The bond dissociation energy of ethylene (πΆπ»2πΆπ» β π») is
4.81 eV [27]. This value is below the band gap of πππ2, therefore energy transfer is likely to
occur. The bond dissociation energy of ethylene is greater than the band gap of πΆππ2,
therefore there may be another mechanism occurring alongside energy transfer which leads
to the increase in ethylene decomposition in the presence of an oxide surface. This other
mechanism may occur in adsorbed water radiolysis discussed previously [25, 29]; however,
there is no chemical change to the inert gas phase that is measureable.
It is evident from Figure 7.6 that the oxide powders have water adsorbed onto the surface,
however, it is not clear as to the extent of water coverage and also the extent of
physisorbed vs. chemisorbed water. Any interaction between ethylene and the oxide
surface is likely to be through physisorption (Figure 7.9).
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
156
Figure 7.9: Postulated schematic of ethylene interaction with an oxide surface
This enhancement of ethylene decomposition may be due to a catalytic mechanism rather
than radiolytic. Studies have shown that doped metal oxides (in particular πΆππ2 and πππ2)
are useful in many hydrocarbon reactions [81] including ethylene dimerisation (Reaction
7.10):
2 πΆ2π»4 β πΆ4π»6 + π»2 Reaction 7.10
This reaction may lead to enhanced π»2 yields that are falsely attributed to radiolysis. This
hypothesis was tested by filling several sample vessels with either πΆππ2 or πππ2, evacuating
the gas phase and replacing with ethylene gas. The samples were then left in a water bath at
50 Β°C for 10 h in order to simulate conditions inside the 60πΆπ irradiator. After this period, the
samples were analysed using the GC. The resulting chromatograms had no π»2 present, with
any quantities, below the limits of detection. Pressure measurements of the samples in the
water bath showed no change in pressure other than to be expected for temperature
fluctuation. This indicates that there is no significant adsorption of ethylene onto the oxide
surface or catalytic reactions occurring (which would lead to a pressure decrease) and the
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
157
gas chromatography results confirm there is no π»2 being produced. Therefore the effect
seen in Figures 7.7 and 7.8 is a radiation driven process.
As the oxide is in powder form, there will be cavities inside the powder which the ethylene
will occupy. This may lead to cavity ionisation. This is a theory postulated by Gray [82],
where the ionisation in a gas cavity inside a medium is related to the energy absorbed by
the surrounding medium. The Bragg-Gray cavity theory is expressed quantitatively in
Equation 7.1:
πΈπ = π½π ππ Equation 7.1
where πΈπ is the energy absorbed by the medium, π½π is the ionisation produced in the cavity,
π is the average energy lost by secondary electrons per ion pair formed in the gas and π is
the ratio of the stopping powers of the medium and the gas. This theory neglects the
existence of high energy secondary electrons which has led to discrepancies in experimental
results of ionisation measurements taken in air filled cavities from that predicted by
Equation 7.1 [83, 84]. These studies also found that the discrepancy increased with
increasing wall Z number. From this, it would be expected that the dose received by the gas
inside a cavity within πΆππ2 to be higher than the dose received by the same gas in a πππ2
cavity. The results, however, do not support this claim as the yield of π»2 is greater from
πππ2 samples than πΆππ2 samples.
It is evident in heterogeneous systems that there is energy transfer between the oxide
powder and the gas phase, however, a definitive mechanism is not forthcoming and there is
no definitive value of how much the oxide surface contributes to the absorbed dose by the
gas phase.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
158
Figure 7.10 highlights the DRIFT spectra of regenerated πΆππ2 before and after irradiation
under an ethylene atmosphere.
Figure 7.10: DRIFT spectra of regenerated πΆππ2 pre-irradiation (blue) and post-irradiation (red) in an ethylene atmosphere
The main difference in the spectra highlighted in Figure 7.10 is the emergence of a group of
bands between 3000-3800 cm-1. These bands have been assigned as πΆ β π» stretches [66].
The emergence of these absorption bands indicates adsorption of ethylene radiolysis
products onto the oxide surface.
Figure 7.11 is the comparative spectra for πππ2.
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
2.0
2.2
5001000150020002500300035004000
Re
fle
ctan
ce /
%
Wavenumber / cm-1
Pre-irradiationPost-irradiation
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
159
Figure 7.11: DRIFT spectra of regenerated πππ2 pre-irradiation (blue) and post-irradiation (red) in an ethylene atmosphere
As seen in Figure 7.10, absorption bands associated with πΆ β π» stretches are present in the post
irradiated sample indicating adsorption of ethylene radiolysis products.
At the conclusion of these experiments, the oxide powders were baked in a furnace at
400 Β°C under static air for 12 h. This temperature ensured the removal of any organic
contaminants on the surface of each oxide without changing the physical properties of the
oxide outlined in Chapter Six. Figures 7.12 and 7.13 depict DRIFT spectra up to 400 Β°C for
the post irradiated πΆππ2 and πππ2, respectively.
0.0
0.2
0.4
0.6
0.8
1.0
1.2
5001000150020002500300035004000
Re
fle
ctan
ce /
%
Wavenumber /cm-1
Pre-irradiation
Post-irradiation
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
160
Figure 7.12: DRIFT spectra of irradiated πΆππ2 in an ethylene atmosphere analysed between 20 β 400 Β°C
0.0
2.0
4.0
6.0
8.0
10.0
12.0
14.0
16.0
18.0
5001000150020002500300035004000
Re
fle
ctan
ce /
%
Wavenumber / cm-1
20 degC
60 degC
120 degC
250 degC
400 degC
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
161
Figure 7.13: DRIFT spectra of irradiated πππ2 in an ethylene atmosphere analysed between 20 β 400 Β°C
It is clear from the previous two figures (7.12 and 7.13), that the temperature employed is
high enough to decompose and remove any organic species that are adsorbed onto the
oxide surfaces. This is seen by the diminishing adsorption band between 3000-2800 cm-1. At
higher temperatures, adsorbed water is driven off the surface as well; however, this will be
re-adsorbed as the temperature decreases as the baking of the oxides is carried out under
static air conditions. At 400 Β°C, the adsorption band identified as πΆπ2 increases, this is more
prominent for πππ2 samples. This is due to hydrocarbon species decomposing in air to form
πΆπ2 and water vapour.
0.0
5.0
10.0
15.0
20.0
25.0
5001000150020002500300035004000
Re
fle
ctan
ce /
%
Wavenumber / cm-1
20 degC
60 degC
120 degC
250 degC
400 degC
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
162
After the oxides have been baked, the πΆπ2 band is reduced to atmospheric levels. Before
the oxides are re-used in further experiments, they are evacuated under vacuum on the
manifold system, which will remove any physisorbed species.
7.6 Gamma Radiolysis of π―π β πΆπ β π¨π Gas Mixtures
The following section outlines the results from pure gas phase radiolysis of five different
mixtures of π»2 β π2 β π΄π , irradiated using 60πΆπ Ξ³-rays. In all of the samples, argon
constitutes at least 90% (by volume) of the sample. The five ratios utilised in this project
were:
π»2 rich atmospheres (stoichiometry 10 : 1 : 89 π»2 β π2 β π΄π (by volume));
π2 rich atmospheres (stoichiometry 1 : 10 : 89 π»2 β π2 β π΄π (by volume));
Equal volumes of π»2 and π2 (stoichiometry 5 : 5 : 90 π»2 β π2 β π΄π (by
volume));
Water stoichiometry of π»2 and π2 (stoichiometry 5 : 2.5 : 92.5 π»2 β π2 β
π΄π (by volume)); and
π2 excess atmospheres (stoichiometry 2.5 : 5 : 92.5 π»2 β π2 β π΄π (by
volume))
Throughout this chapter each ratio has an assigned colour, which is maintained throughout
the figures.
Figure 7.14 shows the results of π»2 depletion as a function of dose for the five systems
outlined above.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
163
Figure 7.14: Results of gamma radiolysis of different ratios of π»2 β π2 β π΄π2 illustrating π»2 depletion as a function of absorbed dose (n.b. trend line for 01:10 data set obscured by
2.5:5 trend line)
The green data points circled in red are anomalous results due to complete depletion of π»2
from the gas phase. This most likely occurred at a lower dose, which would bring the points
closer to the entire data set. These points have been omitted from the G(-π»2) calculations.
Table 7-1 outlines the G(-π»2) values calculated from each trend line of the relevant data set.
Error calculations are within one standard deviation.
2 For clarity, only the π»2 : π2 ratio is shown in the legend of each figure
0.0
10.0
20.0
30.0
40.0
50.0
60.0
70.0
80.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0 180.0
H2 d
eple
tio
n /
(x1
01
7)
mo
lec.
Absorbed Dose / (x1016) 100 eV
10:01
05:02.5
05:05
2.5:5
01:10
H2: O2 (%)
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
164
System (π―π β πΆπ β π¨π (by volume))
G(-π―π) / molecules 100 eV
-1 Error (ππππππ)
10 : 1 : 89 3.56 Β± 0.67
5 : 2.5 : 92.5 4.66 Β± 0.37
5 : 5 : 90 4.68 Β± 0.13
2.5 : 5 : 92.5 3.81 Β± 0.12
1 : 10 : 89 3.60 Β± 1.58
Table 7-1: Calculated G(-π»2) values for several different ratios of π»2 β π2 β π΄π gas using gamma radiation
The system that contains 10: 1: 89 π»2 β π2 β π΄π is the only system where complete
depletion of π»2 cannot occur due to lack of available π2 to form water. The other four
systems can be compared. The G(-π»2) values in Table 7-1 increase with increasing π»2
concentration from 3.60 to 4.66 molecules 100 eV-1 which suggests a first order relationship.
However, this statement is difficult to clarify as the concentration of π2 changes in the
system as well. Also the associated error with samples containing 1: 10: 89 π»2 β π2 β π΄π is
large in comparison to the other errors in Table 7-1. Another hypothesis is that the system is
zero order with π»2 depletion being independent of starting π»2 concentration.
The order of the rate of recombination of π»2 β π2 is still debated in literature sources, with
both zero and first order kinetics highlighted and discussed [40, 41].
Figure 7.15 is a plot of the G(-π»2) value for each individual point in Figure 7.14.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
165
Figure 7.15: Plot of G(-π»2) as a function of absorbed dose for several different ratios of π»2 β π2 β π΄π gas using gamma radiation using the data in Figure 7.14
At low absorbed doses, the G(-π»2) scatter is much larger due to the formula used to
calculate G-values (molecules lost or formed per 100 eV of energy absorbed). At low doses,
this calculation is the division of two numbers of similar magnitudes; if the rate of
formation/ consumption is constant, then at higher doses, the denominator becomes a
much larger number than the number of molecules formed/ consumed.
From Figure 7.15, it is clear that the G(-π»2) values for all five gaseous systems lies in the
range of 2-6 molecules of π»2 consumed per 100 eV of energy absorbed. This range is in
good agreement with Dautzenbergβs earlier work [41].
The corresponding π2 depletion data is plotted in Figures 7.16 and 7.17. The G(-π2) values
for each system is tabulated in Table 7-2. As highlighted in Chapter Four, the GC
0.0
2.0
4.0
6.0
8.0
10.0
12.0
14.0
16.0
18.0
20.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0 180.0
G(-
H2 )
Absorbed Dose / (x1016) 100 eV
10:01
05:02.5
05:05
2.5:5
01:10
H2: O2 (%)
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
166
configuration utilised in this research is less sensitive to π2 than π»2, however, in the
concentration range used, this effect should be nullified.
System (π―π β πΆπ β π¨π (by volume))
G(-πΆπ) / molecules 100 eV
-1 Error (ππππππ)
10 : 1 : 89 2.44 Β± 0.19
5 : 2.5 : 92.5 3.89 Β± 0.28
5 : 5 : 90 4.27 Β± 0.65
2.5 : 5 : 92.5 1.87 Β± 0.28
1 : 10 : 89 2.55 Β± 0.09
Table 7-2: Calculated G(-π2) values for several different ratios of π»2 β π2 β π΄π gas using gamma radiation
Figure 7.16: π2 depletion as a function of absorbed dose using gamma radiation of different ratios of π»2 β π2 β π΄π gas mixtures
-40.0
-20.0
0.0
20.0
40.0
60.0
80.0
100.0
120.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0 180.0
O2 d
eple
tio
n /
(x1
01
7)
mo
lec.
Absorbed Dose / (x1016) 100 eV
10:01
05:02.5
05:05
2.5:5
01:10
H2: O2 (%)
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
167
Although π2 is present in percent concentrations, there is a lot more scatter in these results
compared to the corresponding π»2 data in Figure 7.14 which in turn leads to larger
associated errors. This is likely to be as a result of the dead volume inside the gas
chromatograph and the inability of the vacuum pump to achieve a high vacuum. Despite
this, π2 consumption appears to be zero order with respect to initial π2 concentration.
Figure 7.17: Plot of G(-π2) as a function of absorbed dose for several different ratios of π»2 β π2 β π΄π gas using gamma radiation using the data in Figure 7.16
Assuming that π»2 and π2 recombines to form water via Reaction 7.11, then it would be
expected that the G(-π»2) values would be twice the order of G(-π2) values. The average
ratio between G(-π»2) values in Table 7-1 and the G(-π2) values in Table 7-2 is 1.44. As this
value is greater than 1, it can be assumed that hydrogen peroxide (π»2π2) is not the final
stable product. Therefore, it is likely that there are other stable products that can be formed
during irradiation alongside water.
0.0
2.0
4.0
6.0
8.0
10.0
12.0
14.0
16.0
18.0
20.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0 180.0
G(-
O2 )
Absorbed Dose / (x1016) 100 eV
10:01
05:02.5
05:05
2.5:5
01:10
H2: O2 (%)
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
168
2π»2 + π2 β 2π»2π Reaction 7.11
7.6.1 Discussion
To understand the reaction order of the results, a mechanistic understanding of the system
is needed.
The initial step of this system is the ionisation and excitation of each component (Reactions
7.12-14).
π΄π β π΄π+ + πβ β π΄πβ Reaction 7.12
π»2 β π»2+ + πβ β π»2
β Reaction 7.13
π2 β π2+ + πβ β π2
β Reaction 7.14
Charge transfer between the initial ionised species is important to determine the
concentration of radical species. Table 7-3 gives the ionisation energies of each ground-
state gas molecule [85].
Gas Molecule Ionisation Energy / eV
π΄π 15.76
π»2 15.43
π2 12.07
Table 7-3: Ionisation energy of the three gas molecules in the initial system
From this table it is clear that π΄π can ionise both π»2 and π2 (Reactions 7.15 and 7.16), and
π»2 can ionise π2 (Reaction 7.17).
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
169
π΄π+ + π»2 β π΄π + π»2+ Ο = 1.13x10-15 cm2 [86] Reaction 7.15
π΄π+ + π2 β π΄π + π2+ Ο = 8.0x10-15 cm2 [87] Reaction 7.16
π»2+ + π2 β π»2 + π2
+ Ο = 3.43x10-16 cm2 [88] Reaction 7.17
The reaction cross-sections of Reactions 7.15 - 7.17 are highlighted above. This leads to π2+
being the dominant species after initial ionisation. The ionised states of π»2 and π2 will
undergo geminate recombination and dissociation (Reactions 7.18 and 7.19), π»2β will
dissociate into π» atoms and π2β dissociates primarily into a singlet (1D) and a triplet (3P) state
π atoms [89] which have different reaction rates with different species.
π»2β β 2π» Reaction 7.18
π2β β π(1D) + π(3P) Reaction 7.19
The atomic species produced in Reactions 7.18 and 7.19 then react further and lead to
consumption of π»2 and π2. As π(1D) and π(3P) are the dominant products of the initial
ionisation, their reaction rates with π»2 and π2 will be important to understanding the
mechanism occurring in the gas phase. These reaction rates3 have been determined and are
outlined in the following reactions:
π(1D)+ π»2 β ππ» + π» k= 2.87x10-10 cm3 molecule-1 sec-1 [90] Reaction 7.20
π(3P)+π»2 β ππ» + π» k= 9.08x10-18 cm3 molecule-1 sec-1 [91] Reaction 7.21
π + π2 + π β π3 + π k= 5.8x10-34 cm6 molecule-2 sec-1 [92] Reaction 7.22
Reactions 7.20 and 7.21 highlight the different reaction rates of the singlet and triplet states
of π and Reaction 7.22 highlights the competing reaction with π2 requires a third body
3 Throughout this chapter, reaction rate coefficients are given at 300K
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
170
(π=π2/π2/π΄π/π»π). If π΄π is assumed to be the third body, the concentration is 2.188x1019
molecules cm-3 (assuming 0.9 bar partial pressure and ambient temperature). This
concentration can be used to turn the third order rate constant into a pseudo-second order
rate constant with a value of k= 1.27x10-14 cm3 molecule-1 sec-1. Reaction 7.22 is faster in
comparison to Reaction 7.21, but not as fast as the singlet oxygen reaction with π»2
(Reaction 7.20).
Hydrogen atoms formed in Reaction 7.18 will also react with π»2 and π2 in competition with
Reactions 7.20-22:
π» + π2 β π + ππ» k= 4.25x10-13 cm3 molecule-1 sec-1 [93] Reaction 7.23
π» + π»2 β π»2 + π» k= 1.96x10-32 cm3 molecule-1 sec-1 [94] Reaction 7.24
Recombination of π and π» atoms to form π2 and π»2 molecules both require a third body.
The reaction rates are 4.82x10-33 cm6 molecule-2 sec-1 and 1.3x10-32 cm6 molecule-2 sec-1
[95, 96] respectively. The pseudo-second order reaction rates are k= 1.05x10-13
cm3 molecule-1 sec-1 and k= 2.84x10-13 cm3 molecule-1 sec-1, respectively.
The ππ» formed in Reactions 7.20, 7.21 and 7.23 will then react with molecular and atomic
species as outlined below:
ππ» + π»2 β π»2π + π» k= 6.96x10-15 cm3 molecule-1 sec-1 [97] Reaction 7.25
ππ» + π(3P)β π2 + π» k= 2.92x10-11 cm3 molecule-1 sec-1 [98] Reaction 7.26
Reactions of ππ» with π2 and π» require high temperatures to occur.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
171
Reaction 7.23 can also form π»π2 but requires a third body. The rate constant for this
reaction is 2.2x10-32 cm6 molecule-2 sec-1 [99]. The pseudo-second order rate constant is very
fast however, with a value of k= 4.81x10-13 cm3 molecule-1 sec-1.
π»π2 is a very stable species and can undergo recombination to form hydrogen peroxide
(Reaction 7.27). Hydrogen peroxide can then react with ππ» to form water (Reaction 7.28).
2π»π2 β π»2π2 + π2 k= 6.89x10-13 cm3 molecule-1 sec-1 [100] Reaction 7.27
π»2π2 + ππ» β π»2π + π»π2 k= 1.91x10-12 cm3 molecule-1 sec-1 [101] Reaction 7.28
The reaction mechanism outlined above leads to the formation of water, which is fairly
unreactive to other species, as high temperatures are needed for reactions to occur with
atomic hydrogen and oxygen, and reaction with ππ» leads to hydrogen exchange (Reaction
7.29). Water will however, undergo radiolysis leading to ππ» and π» formation. These species
can then feed back into the mechanism outlined above.
ππ» + π»2π β π»2π + ππ» k= 2.2x10-16 cm3 molecule-1 sec-1 [102] Reaction 7.29
The fastest reaction outlined above is the singlet oxygen atom with π»2 (Reaction 7.20),
therefore in systems where π2 is in excess, consumption of π»2 should be at its greatest. This
is not the case however, suggesting that other reactions may dominate. There are very few
reactions that lead to π»2 being reformed, as π» atom recombination requires a third body,
therefore the probability of the reaction taking place is lower. It is possible that in excess π2
conditions, Reaction 7.22 is increased, as the concentration of π will be at its greatest.
The mechanism outlined above is only at a primitive stage, ionic reactions have not been
included and will play a role in the overall radiation chemistry of the system. Further
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
172
fundamental experiments are required to elucidate a better understanding of the
mechanism.
It should also be noted, that in Figure 7.14, in the absorbed dose range investigated, π»2
continues to be consumed. There are no plateaus in any of the data sets which would lead
to the suggestion of a steady state being reached between recombination and radiolysis
(Reaction 7.30). Therefore, in the system studied in this research, the rate of π»2 and π2
recombination is greater than the rate of water vapour radiolysis.
2π»2 + π2 β 2π»2π Reaction 7.30
7.7 Gamma Radiolysis of π―π β πΆπ β π¨π in the Presence of an Oxide
Surface
The following section outlines results of π»2 β π2 β π΄π radiolysis in the presence of πΆππ2
and πππ2. In all experiments detailed herein, the metal reaction vessels are filled to capacity
with the relevant oxide material. The mass and bulk density of the relevant oxide is used to
determine the remaining gas volume and therefore, the starting concentrations of each
gaseous component. Only the dose absorbed by the gas volume is used to calculate G(-π»2)
values.
Figure 7.18 highlights the consumption of π»2 in the five gaseous mixtures of interest in
contact with πΆππ2.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
173
Figure 7.18: π»2 consumption as a function of absorbed dose for various π»2 β π2 β π΄π gas mixtures in contact with πΆππ2
At low doses, Figure 7.18 highlights that there is more π»2 in the gas phase than was added
initially. It is presumed that this βexcessβ π»2 is from adsorbed water radiolysis as highlighted
in Figure 7.6. The maximum yield of π»2 produced from radiolysis of adsorbed water on
πΆππ2 measured in Figure 7.6 was 0.33 Β΅mol. This yield was attained after 7.0x1019 eV had
been absorbed by the water. In Figure 7.18, the maximum yield measured was 88.0 nmol
after 1.21x1018 eV had been absorbed. These two values are approximately proportional
with dose. However, as the absorbed dose increases, π»2 is not produced in any significant
quantities, it is only consumed.
After initial excitation, any energy transfer from the oxide must interact with adsorbed
species before gaseous species. Therefore the rate of water radiolysis is initially faster than
the rate of recombination. As the adsorbed water is radiolysed, it increases the
-10.0
0.0
10.0
20.0
30.0
40.0
50.0
60.0
70.0
80.0
90.0
100.0
0.0 5.0 10.0 15.0 20.0 25.0 30.0
H2 d
eple
tio
n /
(x1
01
7)
mo
lec.
Absorbed Dose / (x1016) 100 eV
10:0105:02.505:052.5:501:10
H2 : O2 (%)
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
174
concentrations of ππ» and π», therefore, the rates of Reactions 7.23, 7.35 and 7.26 will
increase, leading to π»2 and π2 consumption.
The comparative plot of G(-π»2) values for the data presented in Figure 7.18 is shown in
Figure 7.19.
Figure 7.19: Plot of G(-π»2) as a function of absorbed dose for several different ratios of π»2 β π2 β π΄π gas in contact with πΆππ2
It is clear from this figure that the increased rate of π»2 consumption leads to much larger
G(-π»2) values in this system than in pure gas phase radiolysis (Figure 7.15). However, like
gas phase data presented in Figure 7.15, there is greater variation at lower absorbed doses.
Due to the scatter present in the π2 consumption data in Figure 7.16 from pure gas-phase
experiments, the corresponding data for samples containing πΆππ2 are not shown in this
thesis.
-50.0
0.0
50.0
100.0
150.0
200.0
250.0
300.0
0.0 5.0 10.0 15.0 20.0 25.0 30.0
G (
-H2)
Absorbed Dose / (x1016) 100 eV
10:01
05:02.5
05:05
2.5:5
01:10
H2 : O2 (%)
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
175
Figure 7.20 illustrates the consumption of π»2 as a function of absorbed dose to the five
gaseous systems of interest in contact with πππ2.
Figure 7.20: Plot of π»2 consumption as a function of absorbed dose for the five gaseous systems of relevance in contact with πππ2
As highlighted previously in Figure 7.18, at low absorbed doses, the concentration of π»2
initially increases in Figure 7.20, due to the radiolysis of adsorbed water on the oxide
powder. The maximum yield of π»2 measured in Figure 7.20 is 2.0 Β΅mol at 2.0x1018 eV
absorbed dose. This yield is an order of magnitude above the corresponding yield measured
for the same absorbed dose in Figure 7.6 (0.58 Β΅mol). This may not be a βrealβ effect, as
these are two separate samples, with slight differences in πππ2 mass. This will lead to
differences in calculation of the dose absorbed by each sample.
-20.0
-10.0
0.0
10.0
20.0
30.0
40.0
50.0
60.0
70.0
80.0
90.0
100.0
0.0 2.0 4.0 6.0 8.0 10.0 12.0 14.0 16.0 18.0 20.0
H2 d
eple
tio
n /
(x1
01
7)
mo
lec.
Absorbed dose / (x1016) 100 eV
10:01
05:02.5
05:05
2.5:5
01:10
H2 : O2 (%)
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
176
The βexcessβ π»2 measured in Figure 7.20, is over an order of magnitude greater than the
βexcessβ π»2 measured in Figure 7.18. This further highlights the increase in energy transfer
from πππ2 to adsorbed water than is seen in the corresponding πΆππ2 system.
After the initial increase in π»2, at higher absorbed doses, π»2 is then consumed in all five
gaseous systems of interest.
Figure 7.21 highlights the G(-π»2) yield for the five gaseous systems in contact with πππ2.
Figure 7.21: G(-π»2) as a function of absorbed dose for five gaseous mixtures of π»2 β π2 βπ΄π irradiated in contact with πππ2
The G(-π»2) values are two orders of magnitude greater than measured in the gaseous
system. This wide range of G(-π»2) values is unlikely to be an effect of the scatter that was
highlighted in Figure 7.15, but is hypothesised to be evidence of a chain reaction.
-100.0
0.0
100.0
200.0
300.0
400.0
500.0
0.0 5.0 10.0 15.0 20.0
G (
-H2)
Absorbed dose / (x1016) 100 eV
10:01
05:02.5
05:05
2.5:5
01:10
H2 : O2 (%)
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
177
7.8 Comparison of Homogeneous and Heterogeneous Radiolysis
In comparing the scale of the x-axes in Figures 7.14, 7.18 and 7.20, it is evident that, the rate
of consumption of π»2 is vastly increased in the presence of an oxide surface. More data has
been collected on systems containing the following π»2 β π2 β π΄π concentrations: 5: 5: 90,
5: 2.5: 92.5 and 2.5: 5: 92.5. Therefore, these systems will be compared.
Figure 7.22 compares the consumption of π»2 for systems containing equal concentration of
π»2 and π2 in pure gas and in contact with πππ2 and πΆππ2.
Figure 7.22: π»2 consumption as a function of absorbed dose in samples of 5: 5: 90 π»2 β π2 β π΄π concentration in contact with πΆππ2 and πππ2 and in pure gas system only
The calculated G(-π»2) values from this graph with associated errors are tabulated in Table
7-4:
0.0
10.0
20.0
30.0
40.0
50.0
60.0
70.0
80.0
90.0
100.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0 180.0
H2 d
ep
leti
on
/ (
x10
17)
mo
lec.
Absorbed Dose / (x1016) 100 eV
Gas only
CeO2
ZrO2
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
178
System G(-π―π) / molecules 100 eV
-1 Error (ππππππ)
Gas Only 4.68 Β± 0.13
πΆππ2 35.07 Β± 2.18
πππ2 48.27 Β± 6.48
Table 7-4: Calculated G(-π»2) in samples containing 5: 5: 90 π»2 β π2 β π΄π (by volume) in the presence of πΆππ2, πππ2 and in pure gas phase
The G(-π»2) values in Table 7-4, emphasise the effect the presence of an oxide powder on
the recombination of π»2 and π2.
A possible hypothesis is that radiolysis of adsorbed water on the oxide surface leads to an
increase in π»2 in the gas phase and increases the ratio of π»2 to π2 closer to the favourable
water stoichiometry (2:1). This stoichiometry leads to the favourable formation of water in
the system (Reaction 7.31). Radiolysis of adsorbed water on πππ2 contributes more π»2 than
adsorbed water on πΆππ2, therefore, the rate of consumption of π»2 is greatly increased.
π»2 + π2 + π₯π»2 β (1 + π₯)π»2π (π₯ β€ 1) Reaction 7.31
Figure 7.23 illustrates the rate of π»2 consumption in samples containing 5: 2.5: 92.5
π»2 β π2 β π΄π (by volume) in contact with πΆππ2, πππ2 and in pure gas.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
179
Figure 7.23: π»2 consumption as a function of absorbed dose in samples of 5: 2.5: 92.5 π»2 β π2 β π΄π concentration in contact with πΆππ2 and πππ2 and in pure gas
This figure further highlights how the presence of an oxide surface increases the rate of
consumption of π»2. It is evident from this figure, that in both systems containing an oxide,
π»2 is produced at low doses. This was not evident in Figure 7.22. Investigation of the gas
stoichiometries may lead to an explanation. The initial gas concentration is set at water
stoichiometry (2:1), therefore βexcessβ π»2 from adsorbed water radiolysis, will lead to excess
π»2 in the gas phase (Reaction 7.32), which is measured at low doses.
2π»2 + π2 + π₯π»2 β 2π»2π + π₯π»2 Reaction 7.32
At higher doses, the βexcessβ π»2 may adsorb to the oxide surface (more likely as π» than π»2)
and react with hydroxyl groups on the surface, leading to adsorbed water formation.
-20.0
-10.0
0.0
10.0
20.0
30.0
40.0
50.0
60.0
70.0
80.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0
H2 d
eple
tio
n /
(x1
01
7)
mo
lec.
Absorbed Dose / (x1016) 100 eV
Gas only
CeO2
ZrO2
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
180
The compiled results for π»2 depletion from samples with 2.5: 5: 92.5 π»2 β π2 β π΄π gas
compositions are shown in Figure 7.24.
Figure 7.24: π»2 consumption as a function of absorbed dose in samples of 2.5: 5: 92.5 π»2 β π2 β π΄π concentration in contact with πΆππ2 and πππ2 and in pure gas
In this figure, βexcessβ π»2 is only measured in samples that contains πππ2. The maximum
yield of π»2 is approximately 0.8 Β΅mol, in comparison to 2.1 Β΅mol measured in the
corresponding sample in Figure 7.23. In this system, π2 is initially in excess, therefore any
π»2 formed from adsorbed water radiolysis, will enhance the rate of recombination. This is
highlighted by the fact that, βexcessβ π»2 is not measured in samples containing πΆππ2 and the
yield measured from πππ2 containing samples is an order of magnitude below what is
expected. The overall reaction in this system is shown in Reaction 7.33.
π»2 + 2π2 + π₯π»2 β (1 + π₯)π»2π (π₯ β€ 3) Reaction 7.33
-10.0
0.0
10.0
20.0
30.0
40.0
50.0
60.0
70.0
80.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0
H2 d
eple
tio
n /
(x1
01
7)
mo
lec.
Absorbed Dose / (x1016) 100 eV
Gas only
CeO2
ZrO2
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
181
Summary
From the figures presented in Section 7.8, it is clear that the presence of an oxide powder,
greatly increases the rate of π»2 consumption in mixtures of π»2 β π2 β π΄π gas, in
comparison to homogeneous studies. It is not yet clear however, if this is due to a catalytic
effect from the oxide powder, whether the presence of adsorbed water enhances the gas
phase radiation chemistry or whether other physical properties of the oxides have an effect.
7.9 Discussion of Pelletron Dosimetry
Section 5.6 outlined the methodology used to determine the dose absorbed by a sample
using an accelerated ion source. To enhance the validity of the absolute current
measurements, several experiments were carried out irradiating a chemical dosimeter in
order to make direct comparison between the two systems utilised. The chemical
dosimeters discussed in Sections 5.2 and 5.5 have been investigated using ion accelerators
[64, 103]. Due to the geometry of the reaction vessel and the nature of the radiation field,
the Fricke dosimeter is an unsuitable candidate. The solution is not agitated during
irradiation and the ion beam will only penetrate a few tens of ΞΌm, which will lead to
significant errors in determining the dose by the entire solution. Only mixtures of
π»2 β π2 β π΄π gas will be studied using the ion accelerator therefore ethylene gas was
chosen as the appropriate choice for a chemical dosimeter. The benefits of using ethylene
gas instead of π2π have been discussed previously for use with gamma radiation. Another
disadvantage of using π2π with accelerated ions is the potential to form activated nitrogen
isotopes. The formation of 13π, which is a Ξ² emitter with half-life of ten minutes may lead to
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
182
errors in analysis due to the elapsed time in post irradiation analysis whilst this isotope
decays to safe background levels.
Ethylene radiolysis using a beam of accelerated ions was carried out following the method
outlined in Section 3.4.4. The GC has been adapted to accept glass vessels instead of the
steel sample vessels utilised in Ξ³ radiation studies. The glass vessels have a larger volume
than the corresponding metal cylinders which leads to a smaller change in pressure during
subsequent injections on the GC; this ensures the fragile mica window is not subjected to
large pressure differences.
The results of the ethylene trials are shown in Figure 7.25.
Figure 7.25: Plot of π»2 production as a function of absorbed dose for ethylene experiments using an ion accelerator
In Figure 7.25, the absorbed dose has been calculated by integrating the current profile of
each experiment. The calculated G-value for π»2 formation is 1.39 Β± 0.02 molecules 100 eV-1.
0.0
10.0
20.0
30.0
40.0
50.0
60.0
0.0 5.0 10.0 15.0 20.0 25.0 30.0 35.0 40.0
H2 p
rod
uct
ion
/ (
x10
17)
mo
lec.
Absorbed Dose / (x1017) 100 eV
G(H2)= 1.39 Β± 0.02
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
183
This value is within five percent of the value quoted in several literature sources
(G(π»2)=1.36) [12, 59]. Possible deviations of these values are discussed with respect to
errors associated with ethylene analysis and current measurements.
7.9.1 Source of Errors in Ethylene Analysis
With respect to ethylene, the errors discussed in Section 7.3 are still valid; however, due to
the fragility of the mica window assembly, irradiation at higher pressures is not possible.
Another source of error may be due to a leak in the system. The presence of π»2 in the post
irradiated chromatogram is evidence of a major leak not being present.
Figure 7.26 is a plot of the sample pressure during irradiation of a sample of ethylene.
Figure 7.26: Plot of pressure as a function of time for a sample of ethylene irradiated using 5.5 MeV π»π2+ ions. Irradiation time 30 min, 10 nA current on sample
940
945
950
955
960
965
970
975
0 500 1000 1500 2000 2500 3000 3500
Pre
ssu
re /
mb
ar
Time / s
Irradiation Time
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
184
This figure shows pressure increases inside the sample vessel as the ion beam was
accelerated into the sample. The pressure decreases by the same quantity when the beam
was stopped. The pressure decreased at a rate of 0.93 mbar min-1 during the fifteen minutes
the beam was irradiating the sample. This 2.89% decrease was attributed to radiolysis of the
ethylene. Higher molecular weight polymeric products will condense onto the vessel walls
leading to a decrease in the pressure as will the reaction of ethylene molecules. The stability
of the sample pressure outside of the window of irradiation suggests there is not a leak in
the vessel.
Anderson and Best [103] have studied the ethylene dosimeter using a cyclotron accelerator.
They irradiated samples at approximately 530 mbar and utilised substantially higher dose
rates than in this research. They found the yield of π»2 produced was linear up to absorbed
doses of 3x1020 eV with varying dose rates, ion energy and type.
7.9.2 Source of Errors in Current Measurements
A possible source of error in the current measurements is due to βcrosstalkβ. A small
percentage of ions, when hitting the mica window may be rebounded back onto the ππ
window which leads to some ions being counted more than once. This phenomenon is a
larger problem when more dense materials are placed after the ππ window assembly. It has
been shown that the current on the ππ window is greater when a steel slide is placed after
the window compared to a quartz slide. Mica is less dense than these materials and is
placed further away from the ππ window due to the glass collar. As the ions will have a
lower energy after rebounding off the mica window and traversing across to the ππ window,
the dose enhancement will be negligible.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
185
It is possible that electrons can be ejected from the mica window when the ion beam
traverses the window. Any electrons that are ejected from the window towards the ππ
window will cancel the charge of the positive ions. The probability of this happening is very
small as the majority of electrons will be ejected in the direction of the beam and into the
sample.
Summary
Experiments utilising ethylene as a secondary dosimeter show there is excellent agreement
between the absorbed dose calculated using ethylene dosimetry and absolute current
measurements, with the calculated G-value being within 5% of the literature value. This has
validated the use of the absolute current measurements to determine the absorbed dose in
samples of π»2 β π2 β π΄π gas.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
186
7.10 π―π β πΆπ β π¨π Radiolysis using an Ion Accelerator
Due to operational and time constraints, a revised experiment set was investigated using
accelerated ions. As a result of the complexity of the source and the system of interest, only
gaseous samples were irradiated and only three different compositions. These were:
Equal volumes of π»2 and π2 (stoichiometry 5 : 5 : 90 π»2 β π2 β π΄π (by
volume));
Water stoichiometry of π»2 and π2 (stoichiometry 5 : 2.5 : 92.5 π»2 β π2 β
π΄π (by volume)); and
π2 excess atmospheres (stoichiometry 2.5 : 5 : 92.5 π»2 β π2 β π΄π (by
volume))
The results of these experiments are outlined in Figure 7.27 and Table 7-5.
Figure 7.27: π»2 depletion as a function of absorbed dose for three different mixtures of π»2 β π2 β π΄π utilising 5.5 MeV π»π2+ accelerated ions
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
0.0 1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0
H2 d
eple
tio
n /
(x1
01
9)
mo
lec.
Absorbed Dose / (x1018) 100 eV
05:2.5
05:05
2.5:5
H2 : O2 (%)
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
187
System (π―π β πΆπ β π¨π (by volume))
G(-π―π) / molecules 100 eV
-1 Error (ππππππ)
5 : 2.5 : 92.5 5.04 Β± 0.72
5 : 5 : 90 4.76 Β± 0.61
2.5 : 5 : 92.5 5.38 Β± 0.46
Table 7-5: Calculated G(-π»2) values from experiments utilising 5.5 MeV π»π2+ accelerated ions
The errors associated with this data are larger than the corresponding errors for data
collected with the 60πΆπ source. This is due to a smaller sample set.
In Figure 7.27, π»2 is being depleted linearly with absorbed dose. The G-values calculated for
these data sets indicate the depletion of π»2 is independent of initial π»2 concentration.
7.11 Comparison of Ξ³ and π―ππ+ Irradiation of Gaseous π―π β πΆπ β π¨π
Samples
It is possible to compare the results of π»2 β π2 β π΄π radiolysis using both 60πΆπ gamma rays
and π»π2+ accelerated ions, as there should be no linear energy transfer (LET) effect in
gaseous samples, due to the low density of the systems.
Figure 7.28 combines the results of π»2 depletion as a function of absorbed dose using
gamma rays (Figure 7.14) and accelerated π»π2+ ions (Figure 7.27) for the three gaseous
mixtures investigated using both sources and the calculated G-values are shown in Table
7-6.
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
188
Figure 7.28: π»2 depletion as a function of absorbed dose for three various mixtures of π»2 β π2 β π΄π utilising 60πΆπ Ξ³-rays and 5.5 MeV π»π2+ accelerated ions
System
(π―π β πΆπ β π¨π
(by volume))
60πͺπ Ξ³-rays 5.5MeV π―ππ+ accelerated Ions
G(-π―π) / molecules 100 eV
-1 Error (ππππππ) G(-π―π) /
molecules 100 eV-1
Error (ππππππ)
5 : 2.5 : 92.5 4.66 Β± 0.37 5.04 Β± 0.72
5 : 5 : 90 4.68 Β± 0.13 4.76 Β± 0.61
2.5 : 5 : 92.5 3.81 Β± 0.12 5.38 Β± 0.46
Table 7-6: Calculated G(-π»2) values and associated errors for three different mixtures of π»2 β π2 β π΄π utilising 60πΆπ Ξ³-rays and 5.5 MeV π»π2+ accelerated ions
0.0
50.0
100.0
150.0
200.0
250.0
300.0
350.0
400.0
450.0
0.0 100.0 200.0 300.0 400.0 500.0 600.0 700.0 800.0
H2 d
eple
tio
n /
(x1
01
7)
mo
lec.
Absorbed Dose / (x1016) 100 eV
5:2.5 gamma 5:2.5 He2+
5:5 gamma 5:5 He2+
2.5:5 gamma 2.5:5 He2+
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
189
The G-values in Table 7-6, are very close, however, the error associated with the accelerated
ion data is significantly higher. Sections 7.3 and 7.9 discussed the potential sources of errors
with the dosimetry systems used in each set of measurements and Chapter Four dealt with
the errors associated with GC analysis.
This data confirms there is no radiation type effect and therefore no LET effect as to be
expected in gaseous systems.
The primary radiation sources utilised (60πΆπ Ξ³-rays and 5.5 MeV π»π2+ accelerated ions)
leads to different radiation fields in the samples. Inside the 60πΆπ source, the entire sample is
within the radiation field, however, only part of the sample is in the primary radiation field
when accelerated ions are used. This effect is negated by the secondary electron radiation
field. In gaseous systems the majority of the absorbed dose is from interactions of the
secondary electrons with the gas, not the primary radiation [57]. These secondary electrons
can have ranges in the order of metres, therefore all of the sample can still be irradiated.
Conclusions
60πͺπ Studies
The use of ethylene (πΆ2π»4), as a gas-phase dosimeter for 60πΆπ Ξ³-rays provides results in
good agreement with the more commonly used Fricke dosimeter. This allows for a good
approximation of the dose absorbed by the gas phase studied in this chapter. The detection
limits of the GC leads to higher irradiation pressures being required to attain repeatable
results.
Adsorbed water on both πΆππ2 and πππ2 leads to π»2 formation during irradiations. The
quantity of π»2 produced is five times greater in the presence of πππ2 than πΆππ2, in good
agreement with literature [25, 29], an explanation of this, is the resonance of the oxide
Chapter 7 π»2 - π2 Radiolysis Results and Discussion 7131060
190
band gap with the bond dissociation energy of water. The approximation of one monolayer
of adsorbed water is valid, with the quantities of π»2 measured.
A similar effect is seen with radiolysis of ethylene in contact with an oxide surface. The yield
of π»2 is greater than the sum of radiolysis of ethylene alone and π»2 produced from
adsorbed water radiolysis. The bond dissociation energy of ethylene is 4.81 eV, which is low
enough for energy transfer from πππ2 to enhance decomposition.
The gamma radiolysis of π»2 β π2 β π΄π gas mixtures follows zero order kinetics with regards
to π»2 depletion. This is in agreement with literature data [41], however, a complete
explanation is not forthcoming. The presence of an oxide surface greatly enhances depletion
of π»2 from the gas phase. At low doses, there is an βexcessβ of π»2 due to the radiolysis of
adsorbed water having a faster rate than recombination of π»2 and π2, at higher doses,
however, recombination dominates. A steady state between the two processes is not
reached.
π―ππ+ Studies
The use of ethylene gas as a dosimeter for ion accelerator experiments provides good
validation of the absolute current measurements. The G(π»2) value of 1.39 is within 5% of
literature values.
Experiments utilising accelerated π»π2+ ions confirm there is no LET effect in samples of
π»2 β π2 β π΄π. These experiments also highlight that no steady state is reached between
the recombination of π»2 β π2 and the radiolysis of water vapour at higher absorbed doses
than achieved with 60πΆπ Ξ³-rays.
Chapter 8 Air Radiolysis Results and Discussion 7131060
191
8 Air Radiolysis Results and Discussion
The following chapter details the results from radiolysis of air experiments in the
presence/absence of a particular oxide surface. The experimental details were outlined in
Chapter Three (all experiments undertaken in 12.0 cm3 glass vials, with the temperature
inside the 60πΆπ irradiator being approximately 35 Β°C). The results are interpreted and their
relevance discussed throughout.
This chapter details the results from radiolysis of air measurements and their significance.
This is followed by initial results with samples containing an oxide surface. During these
results, an interference from another species was identified and resolved. New data from air
radiolysis experiments in the presence of an oxide surface are presented and discussed
followed by results and discussion of the interfering species. A final conclusion of the results
presented in this chapter is given at the end.
8.1 Ion Chromatogram Calibration
During the course of air radiolysis experiments, the primary product ion of interest is the
nitrate anion (ππ3β). To determine the detection limit of the ion chromatograph and its
linearity, calibration solutions of sodium nitrate (ππππ3) with known concentrations were
injected into the ion chromatograph. Two injections of each standard were taken to ensure
there were no instrument anomalies. The calibration results are shown in Figure 8.1:
Chapter 8 Air Radiolysis Results and Discussion 7131060
192
Figure 8.1: Calibration plot of ππ3β peak area as a function of ππππ3 concentration using
ion chromatography
The ion chromatograph has a linear response to ππ3β in the range of 0.05-1 mmol L-1. The
standard deviation of the slope (Ο) is 0.99. To validate the performance of the detector,
fortnightly calibrations using fresh ππππ3 solutions were carried out.
y = 49.279x RΒ² = 0.9968
0.0
10.0
20.0
30.0
40.0
50.0
60.0
0 0.2 0.4 0.6 0.8 1 1.2
Pea
k ar
ea /
AU
[NaNO3] / mM
Chapter 8 Air Radiolysis Results and Discussion 7131060
193
8.2 Air Radiolysis
To determine the baseline yield of nitrate without an oxide present, the glass vials shown in
Figure 3.5 were sealed and irradiated. The results are shown in Figure 8.2:
Figure 8.2: Effect of Ξ³ radiation dose4 on nitrate production from laboratory air Volume of sample = 12.0 cm3 at 35 Β°C
Initially there is a linear relationship between the dose absorbed by the gas and the
production of ππ3β. This initial production has been plotted on the graph (black dashed line)
and gives an initial yield, G(ππ3β), value of 1.39 Β± 0.04 ions 100 eV-1. As seen in Chapter Two,
this yield is within the value quoted in the literature [45, 46]. Above an absorbed dose of
6x1019 eV, the measured production of ππ3β drops off from the initial rate of formation and
starts to plateau with increasing dose. This decreased production suggests that a steady
state has been reached for this system, in which the amount of ππ3β is 1 Β΅mol.
4 Throughout this Chapter, in all plots of species production as a function of absorbed dose, the absorbed dose
axis has been plotted in units of 100 eV so that G-values for the species in question can be determined from the gradient of the trend line of the data.
0.0
20.0
40.0
60.0
80.0
100.0
120.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0
Nit
rate
pro
du
ctio
n /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV 1
G(NO3-)=1.39
Chapter 8 Air Radiolysis Results and Discussion 7131060
194
A plausible explanation for the levelling of the ππ3β production is the depletion of a reactant
that leads to the formation of nitric acid. This reactant is likely to be water vapour as
outlined by Jones [46]. To assess this hypothesis, 100 Β΅l of liquid water was added to the
vials and irradiations were performed under the same conditions. Figure 8.3 shows the
results:
Figure 8.3: Effect of Ξ³ radiation dose on the production of nitrate in water saturated and unsaturated laboratory air. Volume of air = 11.9-12.0 cm3 at 35 Β°C
When water is added to the system, the initial rate of ππ3β formation seen in Figure 8.2 is
extended to higher doses and shows no sign of levelling off. The G-value for ππ3β formation
in the water saturated system is 1.17 Β± 0.06 ions 100 eV-1.
If the concentration of water is the factor limiting the production of nitric acid in air
radiolysis, it is important to quantify the amount of water vapour present in the initial
system. The relative humidity in the laboratory where the samples are prepared is
approximately 40% with an average temperature of 25 Β°C. These conditions give a saturated
0.0
20.0
40.0
60.0
80.0
100.0
120.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0
Nit
rate
yie
ld /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV
Lab. Air
Air (H2O added)
G(NO3-) = 1.17
Chapter 8 Air Radiolysis Results and Discussion 7131060
195
vapour density of 23 g m-3 of water. Using Equation 8.1, the actual vapour density in the
room is calculated as 9.2 g m-3:
π . π». = πππ‘π’ππ π£ππππ’π ππππ ππ‘π¦
π ππ‘π’πππ‘ππ π£ππππ’π ππππ ππ‘π¦ x 100% Equation 8.1
The glass vials in Figure 3.5 have a crimped volume of 12 cm3. Therefore the quantity of
water in the initial vial is 3.69x1018 molecules. Assuming that each water molecule can react
with π2 and π2 to form 2 molecules of nitric acid (π»ππ3) (Reaction 8.1), the maximum yield
of nitrate theoretically attainable is 12.26 Β΅mol.
2π»2π + π2 + 2π2 β 4π»ππ3 Reaction 8.1
This value exceeds the maximum yield achieved in Figure 8.2 (1 Β΅mol) by approximately
90%, suggesting that there is another mechanism occurring that leads to the removal of
water vapour from the system. Chapter Seven discussed this topic in more detail with the
likely mechanism being water vapour radiolysis, forming π»2 and π2 gas.
In the subsequent data plots, the water saturated air results will be plotted to represent the
system in the absence of an oxide. This is to show the trend of nitrate formation assuming
an excess of water vapour was present.
8.3 Air Radiolysis in the Presence of an Oxide Surface
In the following section, results are given for the systems containing an oxide powder.
Dosimetry of this system was detailed in Section 5.3, with a weighting factor applied to
Fricke dosimeter results to correct for the difference in density of the dosimeter solution
and air. The volume of gas irradiated is calculated by subtracting the volume of oxide (using
Chapter 8 Air Radiolysis Results and Discussion 7131060
196
the crystal density and the mass) from the total volume. The actual volume of gas inside the
vial is used to determine the dose absorbed of the gas.
Figure 8.4 shows the results of the system containing 1 g of an oxide powder. In this system,
the majority of the volume is still occupied by the gas phase (~95%) therefore the surface
should not have a profound effect on the nitrate yield.
Figure 8.4: Nitrate production as a function of dose for systems containing 1 g of either πΆππ2 or πππ2 powder and water saturated air (no oxide)
The G-values of nitrate formation calculated from the gradient of each data set is given in
the following table:
System G(π΅πΆπβ) /
molecules 100 eV-1 Error (ππππππ)5
No oxide 1.17 Β± 0.06
1 g πΆππ2 1.96 Β± 0.03
1 g πππ2 2.10 Β± 0.04
Table 8-1: Calculated G(ππ3β) values and standard deviation of the gradient for 1 g oxide
systems and water saturated air (no oxide)
5 Throughout this Chapter, errors are calculated within one standard deviation.
0.0
20.0
40.0
60.0
80.0
100.0
120.0
140.0
160.0
0.0 10.0 20.0 30.0 40.0 50.0 60.0 70.0 80.0 90.0
Nit
rate
pro
du
ctio
n /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV
No Oxide
CeO2
ZrO2
Chapter 8 Air Radiolysis Results and Discussion 7131060
197
From this table, it is clear that in the presence of an oxide surface, the yield of nitrate
formation increases by 60 and 80% with πΆππ2 and πππ2, respectively. Furthermore, this
increased rate of formation remains constant up to absorbed doses of 7x1019 eV. This trend
suggests that there is more water in the irradiated system in the presence of an oxide than
is present in laboratory air alone. The water is most likely to be adsorbed to the oxide
surface.
Table 8-2 highlights the water available in the system, either in the headspace or adsorbed
onto the oxide powder. Several assumptions have been made in these calculations. Firstly,
only one monolayer of water is adsorbed onto the oxide. The mass of this monolayer has
been calculated as 0.21 mg m-2 for ππ’π2 [23], this value should not differ greatly for πΆππ2
or πππ2. Secondly, the vapour density of the air is 9.2 g m-3 with 40% relative humidity. The
surface area of each oxide was determined in Chapter Six.
System Surface Area / m2
Oxide Volume6 /
cm3
Mass of water on oxide /
mg
Mass of water in
headspace / Β΅g
Total mass of water in
system / mg
Water Saturated air
(no oxide)
- - - (0.1 mg of
liquid water)
110.40 0.18
1 g πΆππ2 7.42 0.14 1.56 109.11 1.67
1 g πππ2 2.24 0.18 0.47 108.74 0.58
Table 8-2: Calculated mass of water in systems containing 1 g πΆππ2, 1 g πππ2 and water saturated air (no oxide)
Clearly the mass of water adsorbed on the oxide surface far outweighs the mass of water in
the gas phase, and it is unlikely that water depletion will occur in experiments on samples
containing the oxide powder.
6 Using crystal density values of: 7.215 and 5.68 g cm
-3 for πΆππ2and πππ2, respectively
Chapter 8 Air Radiolysis Results and Discussion 7131060
198
The following paragraph details the results from experiments on a system with 50% oxide
(by volume). As explained in Section 3.4.2 and determined in Chapter Six, the bulk density of
each oxide was used to calculate the mass needed to fill the glass vials to approximately half
the volume. The mass of oxide required was 6 and 11 g for πΆππ2 and πππ2, respectively.
Table 8-3 highlights the calculated water available in the system for both oxides.
System Surface Area / m2
Oxide Volume /
cm3
Mass of water on oxide /
mg
Mass of water in
headspace / Β΅g
Total mass of water in
system / mg
Water Saturated air
(no oxide)
- - - (0.1 mg of
liquid water)
110.40 0.18
50% πΆππ2 (by volume)
(~6 g)
44.5 0.83 9.35 102.76 9.45
50% πππ2 (by volume)
(~11 g)
24.6 1.94 5.17 92.55 5.26
Table 8-3: Calculated mass of water in systems containing 50% πΆππ2 and 50% πππ2 (by volume) and water saturated air (no oxide)
The results are shown in Figure 8.5 and Table 8-4:
Chapter 8 Air Radiolysis Results and Discussion 7131060
199
Figure 8.5: Nitrate production as a function of absorbed dose for systems containing 50% oxide (by volume) and for water saturated air (no oxide)
System G(π΅πΆπβ) /
molecules 100 eV-1 Error (ππππππ)
No oxide 1.17 Β± 0.06
50% πΆππ2 (~6 g) 2.96 Β± 0.09
50% πππ2 (~11 g) 3.55 Β± 0.11
50% πππ2 (2) (~11 g) 4.77 Β± 1.30
Table 8-4: Calculated G(ππ3β) values and standard deviation of the gradient for experiment
with 50% oxide (by volume) and with water saturated air (no oxide)
The most prominent feature of Figure 8.5 is that at low absorbed doses (< 1x1019 eV) there
is a discrepancy in the πππ2 system which leads to some samples (orange data) producing
almost double the yield of nitrate. The orange data set represents a separate experiment
run in comparison to the green data set. The data represented by the orange markers has a
higher degree of scatter and standard deviation. The explanation for this will be discussed in
the following section.
0.0
50.0
100.0
150.0
200.0
250.0
300.0
350.0
400.0
450.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0
Nit
rate
yie
ld /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV
No Oxide
CeO2 (~6 g)
ZrO2 (~11 g)
ZrO2 (2) (~11 g)
Chapter 8 Air Radiolysis Results and Discussion 7131060
200
As seen in the 1 g data set, the presence of an oxide surface greatly enhances the formation
of nitric acid. The yield of ππ3β is two and a half times greater with 50% πΆππ2 present and
three times greater with πππ2 present. The yield is greater with πππ2 present than πΆππ2, as
seen with the 1 g data set. This difference is not simply due to an increase in surface area
and a possible increase in catalytic sites on the powder, as there is three times more surface
area in the πΆππ2 system than in the πππ2 system.
The oxide masses used in experiments with 90% oxide (by volume) are 12 g of πΆππ2 and 20
g of πππ2. Table 8-5 highlights the calculated water available in each system.
System Surface Area / m2
Oxide Volume /
cm3
Mass of water on oxide /
mg
Mass of water in
headspace / Β΅g
Total mass of water in
system / mg
Water Saturated air
(no oxide)
- - - (0.1 mg of
liquid water)
110.40 0.18
90% πΆππ2 (by volume)
(~12 g)
89.0 1.66 18.7 95.13 18.80
90% πππ2 (by volume)
(~20 g)
44.8 3.52 9.41 78.02 9.49
Table 8-5: Calculated mass of water in systems containing 90% πΆππ2 and 90% πππ2 (by volume) and water saturated air (no oxide)
Figure 8.6 and Table 8-6 show the results from experiments with 90% oxide present (by
volume).
Chapter 8 Air Radiolysis Results and Discussion 7131060
201
Figure 8.6: Nitrate production as a function of dose for systems containing 90% oxide (by volume) and for water saturated air (no oxide)
System G(π΅πΆπβ) / molecules 100 eV-1
Error (ππππππ)
No oxide 1.17 Β± 0.06
90% πΆππ2 (~12 g) 4.54 Β± 0.72
90% πππ2 (~20 g) -20.55 Β± 11.54
90% πππ2 (~20 g) manipulated (orange line)
19.78 Β± 3.57
Table 8-6: Calculated G(ππ3β) values and standard deviation of the gradient for systems with
90% oxide (by volume) and for water saturated air (no oxide)
At low absorbed doses, there is a large amount of scatter in the πππ2 system. This scatter
was also apparent in the 50% system (Figure 8.5). The size of the possible error in the yields
obtained for the πΆππ2 system has also increased from the 50% system. This increase will be
discussed in the next section. The presence of the two πππ2 data points with yields of
nitrate above 1.8x1016 molecules (3 Β΅mol) (highlighted in red circles) complicates the data
analysis and leads to apparently negative yield of nitrate calculated. By removing these
points, the G(ππ3β) yield is 19.78 molecules 100 eV-1 and the standard deviation of the slope
0.0
50.0
100.0
150.0
200.0
250.0
300.0
0.0 10.0 20.0 30.0 40.0 50.0 60.0 70.0 80.0
Nit
rate
yie
ld /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV
No Oxide
CeO2 (~12 g)
ZrO2 (~20 g)
Chapter 8 Air Radiolysis Results and Discussion 7131060
202
is 3.57. This slope is highlighted in orange in Figure 8.6. This data manipulation greatly
reduces the scatter in the results; however, the G-value calculated is much larger than that
measured in the previous πππ2 data sets. The large increase was not seen between the 1 g
and 50% sample systems, therefore this may not be a real effect.
8.3.1 Comparison of πͺππΆπ Data
Figure 8.7 and Table 8-7 compares Ξ³-radiation results for the πΆππ2 system and displays how
nitrate formation is affected by the presence of πΆππ2.
Figure 8.7: Nitrate production as a function of absorbed dose for 1 g, 50% and 90% (by
volume) πΆππ2 systems and for water saturated air (no oxide)
System G(π΅πΆπβ) /
molecules 100 eV-1 Error (ππππππ) Surface Area /
m2
No oxide 1.17 Β± 0.06 N/A
1 g πΆππ2 1.96 Β± 0.03 7.42
50% πΆππ2 (~6 g) 2.96 Β± 0.09 44.5
90% πΆππ2 (~12 g) 4.54 Β± 0.72 89.0
Table 8-7: Calculated G(ππ3β) values for the πΆππ2 containing systems and for water
saturated air (no oxide)
0.0
50.0
100.0
150.0
200.0
250.0
300.0
350.0
400.0
450.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0
Nit
rate
yie
ld /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV
No Oxide
1 g
50% (~6 g)
90% (~12 g)
Increasing oxide
surface area
Chapter 8 Air Radiolysis Results and Discussion 7131060
203
It is clear from this table that the yield of nitrate is affected by the presence of πΆππ2 in the
system. The yield rises with increasing quantity of oxide, however, the rate of increase, does
not correspond to the increase in volume or surface area. In the systems containing 50% (by
volume) πΆππ2, there is a six fold increase in mass and surface area compared to samples
containing 1 g πΆππ2, yet the yield of nitrate only increases by 50%; this trend is seen in
systems with 50% and 90% (by volume) πΆππ2 where the mass and surface area are doubled
but the nitrate yield only increases by 50%. This trend will be discussed later in the chapter.
8.3.2 Discussion
An interesting feature of Figure 8.7 is that none of the trend lines for the yield of nitrate
appear to go through zero. At low absorbed doses (< 1x1019 eV), there is an initial off-set
between the yield of nitrate and the mass of oxide present. This is shown more clearly in
Figure 8.8:
Figure 8.8: Nitrate production as a function of absorbed dose for 1 g, 50% and 90% (by volume) πΆππ2 systems and for water saturated air (no oxide) up to an absorbed dose of
2.0x1019 eV
0.0
10.0
20.0
30.0
40.0
50.0
60.0
70.0
80.0
90.0
100.0
0.0 2.0 4.0 6.0 8.0 10.0 12.0 14.0 16.0 18.0 20.0
Nit
rate
yie
ld /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV
No Oxide
1 g
50% (~6 g)
90% (~12 g)
Chapter 8 Air Radiolysis Results and Discussion 7131060
204
Extrapolation of the trend lines to zero absorbed dose generates the following nitrate yields
(Table 8-8):
System Inferred Quantity of Nitrate at zero absorbed dose /
Β΅mol
No oxide 0.17 Β± 0.04
1 g πΆππ2 0.14 Β± 0.01
50% πΆππ2 (~6 g) 0.50 Β± 0.06
90% πΆππ2 (~12 g) 0.35 Β± 0.23
Table 8-8: Initial yield of nitrate pre-irradiation
It is evident from the above data that there appears to be significantly more nitrate present
in the higher loading systems than in the 1 g and the water saturated air system. This initial
yield could be due to a fast reaction of some description that leads to the oxide surface
becoming saturated with nitrate or another species. Once the surface is covered with a layer
of nitrate, the rate of the reaction decreases and leads to the yields calculated in Table 8-8.
Another explanation is the presence of a contaminant, either in the oxide powder or the
ππππ» solution used in the analysis of samples.
Cerium and zirconium dioxide both have fluorite crystal structures which are built around a
face centred cube unit cell (Figure 8.9i) with πΆπ4+/ππ4+ located at the octahedrally
coordinated lattice points and π2β located at the tetragonal interstitials.
Chapter 8 Air Radiolysis Results and Discussion 7131060
205
i) ii)
Figure 8.9: i) Face-centred cubic crystal structure unit cell7, and ii) atomic structure of each face in the unit cell [104]
The unit cell contains four atoms with each face having one atom. From the lattice
parameter, the area of each surface atom can be determined (Figure 8.9ii). This allows for
the determination of the total number of surface atoms in the solid which can act as
adsorption sites for gas phase molecules. The lattice parameter of πΆππ2 is 5.4 Γ [105] and
the lattice parameter of πππ2 is 5.27 Γ [106]. Using this lattice parameter, the cross-
sectional area of each atom is 1.14x10-19 m2. Assuming one gas phase molecule can adsorb
to each surface atom, the surface coverage of one monolayer will be 8.78x1018 molecules
m-2. This value is reasonable as the corresponding value for πππ2 is 5.2x1018 molecules m-2
[107].
As the surface area of each oxide is known, the number of molecules that can adsorb to the
surface and form one monolayer will be approximately 1.61x1019 molecules g-1 for πΆππ2 and
5.0x1018 molecules g-1 for πππ2. If the gas phase molecule in question requires two surface
atoms to adsorb to the surface (bridging mode), the calculated number of adsorbed
molecules will be reduced by a factor of two.
7 Tetragonal interstitials not included for clarity
Chapter 8 Air Radiolysis Results and Discussion 7131060
206
From Figure 8.8 and Table 8-8, it is clear that the initial yield of nitrate in the 50% (by
volume) system is 0.5 Β΅mol. This is equal to 3.0x1017 molecules, which is two orders of
magnitude below the calculated value for the number of molecules needed to form one
monolayer on πΆππ2, assuming one nitrate molecule can adsorb to one surface atom.
Therefore, allowing for differences in the lattice parameter and the number of surface sites
needed for a nitrate molecule to adsorb to, the off-set seen in Figure 8.8 is not due to
surface saturation.
An alternative explanation is that a quantity of nitrate is already adsorbed onto the πΆππ2
surface before experiments begin. As explained in Section 3.4.3, the oxide powders are
regenerated after analysis by washing with water and baking for several hours. It is possible
that these conditions do not fully remove adsorbed nitrate from the surface before further
experiments are undertaken. DRIFT spectra of the regenerated oxides were shown in
Chapter Six, the spectra of both πΆππ2 and πππ2 highlighted the presence of πππ₯ moieties
on the oxide surface which could potentially oxidise and enhance the yield of nitrate. This
will be discussed in more detail in the following section.
8.3.3 Comparison of πππΆπ Data
Figure 8.10 and Table 8-9 highlights the corresponding compiled data for πππ2.
Chapter 8 Air Radiolysis Results and Discussion 7131060
207
Figure 8.10: Nitrate production as a function of absorbed dose for 1 g, 50% and 90% (by volume) πππ2 systems and for water saturated air (no oxide)
System G(π΅πΆπβ) /
molecules 100 eV-1 Error (ππππππ) Surface Area /
m2
No oxide 1.17 Β± 0.06 N/A
1 g πππ2 2.10 Β± 0.04 2.24
50% πππ2 (~11 g) (green data)
3.55 Β± 0.11 24.6
50% πππ2 (2) (~11 g) (orange data)
4.77 Β± 1.30 24.6
90% πππ2 (~20 g) (manipulated)
19.78 Β± 3.57 44.8
Table 8-9: Calculated G(ππ3β) values for the system containing πππ2 and for water
saturated air (no oxide)
As seen with the πΆππ2 data, the production of nitrate increases with increasing mass of
πππ2. For qualitative interpretation, the increase in scatter at higher loadings of oxide is a
concern and therefore only limited conclusions can be drawn from the data set given in
Table 8-9.
0.0
20.0
40.0
60.0
80.0
100.0
120.0
140.0
0.0 10.0 20.0 30.0 40.0 50.0 60.0 70.0 80.0 90.0
Nit
rate
yie
ld /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV
No Oxide1 g50% (~11 g)50% (2) (~11 g)90% (~20 g)
Chapter 8 Air Radiolysis Results and Discussion 7131060
208
8.4 Explanation of Scatter in 50% and 90% (by volume) πππΆπ Results
The concentration of nitrate is determined by the integrated peak area of the ion
chromatogram signal relative to the calibration plot. Ascertaining the true peak area for the
nitrate signal for the samples containing 50 and 90% (by volume) of πππ2 proved
challenging. Figure 8.11 shows typical chromatograms measured with post irradiated
analysis of samples containing various loadings of πππ2:
Chapter 8 Air Radiolysis Results and Discussion 7131060
209
i)
ii)
iii)
Figure 8.11: Three ion chromatograms of samples containing: i) 1 g, ii) 50% and iii) 90% πππ2 (by volume) illustrating the emergence of a second signal at 6.6 min
0.0
10.0
20.0
30.0
40.0
50.0
60.0
70.0
3 4 5 6 7 8 9
Co
nd
uct
ivit
y /
Β΅S
Retention time / min
Nitrate
-1.0
1.0
3.0
5.0
7.0
9.0
11.0
13.0
3 4 5 6 7 8 9
Co
nd
uct
ivit
y /
Β΅S
Retention time / min
Nitrate
-2.0
3.0
8.0
13.0
18.0
23.0
28.0
3 4 5 6 7 8 9
Co
nd
uct
ivit
y /
Β΅S
Retention time / min
Nitrate
1 g
50%
90%
Chapter 8 Air Radiolysis Results and Discussion 7131060
210
In the chromatograms shown in Figure 8.11, the signal representing nitrate has been
labelled. It has a retention time of approximately 7 min. The four signals present in the
chromatograms that have retention less than 6 min have been assigned and tabulated in
Table 8-10.
Anion Retention Time / min
Carbonate (πΆπ32β) 3.55
Chloride (πΆπβ) 4.45
Bicarbonate (π»πΆπ3β) 5.10
Sulphate (ππ42β) 5.95
Table 8-10: Anions and corresponding retention times (in minutes) present in deionised water
These anions are present in the deionised water used to prepare the 5 mM ππππ» solution.
Due to the basic nature of the solution, carbon dioxide (πΆπ2) from the atmosphere dissolves
in the solution and hydrolyses to form both carbonate and bicarbonate anions. These two
anions are indistinguishable using the current instrument configuration, therefore the
signals with retention times of 3.55 and 5.10 min can be labelled as carbonate or
bicarbonate. The concentration of these anions does not increase with absorbed dose in the
system, therefore they are not a product of radiolysis. The chloride signal does increase,
however, with increasing mass of oxide. Therefore it is likely that chloride is present as a
contaminant counter ion in the oxide lattice and will not significantly affect the chemistry of
the system.
In the chromatogram shown in Figure 8.11i, the signal produced by nitrate has an
asymmetric non-Gaussian profile. The asymmetry could be due to the response of the
Chapter 8 Air Radiolysis Results and Discussion 7131060
211
detector or interference from another signal. Figure 8.11ii shows the emergence of a
second signal at 6.6 min. The profile of the nitrate signal is now more symmetrical, however,
the second signal appears as a βshoulderβ on the nitrate peak. In the final chromatogram
(Figure 8.11iii), the second signal has a much larger concentration and has started to split
from the nitrate signal, however, the two signals are not fully resolved and still overlap. The
close proximity of the two peaks makes integration of a single peak difficult and
assumptions of true peak profiles will lead to errors in the subsequent nitrate yield
calculation. Both of the signals discussed here, with retention between 6.5 and 7 min do not
appear in unirradiated blanks, therefore both anions are formed from radiolytic processes.
The second πππ2 data set plotted in Figure 8.5 (orange data points) all had chromatogram
profiles similar to that shown in Figure 8.11ii. The integrated peak area used in the
subsequent nitrate calculation was the sum of the nitrate signal and the shoulder. The
instrument software is unable to differentiate the presence of two signals. The consequence
is an increased area which leads to overestimation of the nitrate concentration in the
solution and the radiolytic yield of nitrate formation.
It is of importance to separate and identify this second signal to ensure that a true nitrate
yield can be calculated. Several inorganic anions such as phosphate (ππ43β) and simple
organic anions based around carbon, nitrogen and oxygen moieties including nitrite (ππ2β)
and cyanate (πΆππβ) have been analysed to determine the identity of this second signal.
After intensive investigation, the second signal was identified as oxalate (πΆ2π42β). Figure
8.12 shows the ion chromatogram peak profile of 50 ΞΌM oxalic acid (π»2πΆ2π4), 0.1 mM
sodium nitrate and a mixed solution of both compounds.
Chapter 8 Air Radiolysis Results and Discussion 7131060
212
Figure 8.12: Ion chromatogram of 50 ΞΌM oxalic acid, 0.1 mM sodium nitrate and a mixed solution of both
The signal profile of the sample containing both oxalate and nitrate anions is identical to the
signal profile seen in Figure 8.11iii. It is clear from this figure that, with the current
instrument configuration, the retention of oxalate and nitrate are very similar and lead to
interference between the two signals.
To separate these anions, several of the instrument conditions were changed, including flow
rate, column temperature and eluent concentration. Altering the flow rate and column
temperature led to longer elution times, however, the peaks were still poorly separated.
Lowering the eluent concentration was found to have the desired effect of separating the
oxalate and nitrate peaks whilst increasing the elution time of both. Figure 8.13 illustrates
the chromatogram of the mixed solution containing both compounds seen in Figure 8.12,
however, the πΎππ» eluent concentration has been lowered from 23 mM to 14 mM.
0.0
5.0
10.0
15.0
20.0
25.0
30.0
5.5 5.7 5.9 6.1 6.3 6.5 6.7 6.9 7.1 7.3 7.5
Co
nd
uct
ivit
y /
Β΅S
Retention time / min
0.1 mM NaNO3
0.05 mM H2C2O4
0.1 mM NaNO3 / 0.05 mM H2C2O4
Chapter 8 Air Radiolysis Results and Discussion 7131060
213
Figure 8.13: Chromatogram of 0.1 mM ππππ3 and 50 ΞΌM oxalic acid mixed solution using eluent concentration of 14 mM πΎππ»
The nitrate anion now elutes at approximately 8.9 min and oxalate elutes at 11.5 min. If the
eluent concentration is decreased below 14 mM then the signal from sulphate starts to
interfere with nitrate. The signal from sulphate can be seen in Figure 8.13 at a retention
time of 7.95 min.
0.0
5.0
10.0
15.0
20.0
25.0
6 7 8 9 10 11 12 13 14
Co
nd
uct
ivit
y /
Β΅S
Retention Time / min
0.1 mM NaNO3 / 0.05 mM H2C2O4
Nitrate
Oxalate
Sulphate
Chapter 8 Air Radiolysis Results and Discussion 7131060
214
8.5 Refinement of Experimental Data in the Presence of an Oxide
Surface
The following section details new nitrate production data that has been collected after the
identification of the oxalate interference had been resolved.
Figure 8.14 and Table 8-11 detail the refined data for the system containing 1 g of oxide:
Figure 8.14: Nitrate production as a function of dose for samples containing 1 g of oxide powder and for water saturated air (no oxide)
System G(π΅πΆπβ) /
molecules 100 eV-1 Error (ππππππ)
No oxide 1.17 Β± 0.06
1 g πΆππ2 2.07 Β± 0.07
1 g πππ2 1.48 Β± 0.04
Table 8-11: Calculated G(ππ3β) values and standard deviation of the gradient for systems
with 1 g oxide and water saturated air (no oxide)
Figure 8.14 illustrates that the presence of the oxide still has an effect on the formation of
nitrate in the radiolysis of air. The yield of nitrate in the system containing πΆππ2 is almost
double the yield from radiolysis of air alone, whilst the yield in the πππ2 system is 25%
greater than in humid air.
0.0
50.0
100.0
150.0
200.0
250.0
300.0
0.0 50.0 100.0 150.0 200.0
Nit
rate
pro
du
ctio
n /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV
No OxideCeO2ZrO2
Chapter 8 Air Radiolysis Results and Discussion 7131060
215
Figure 8.15 and Table 8-12 outline the results of nitrate formation yields for the systems
containing 50% oxide (by volume). The masses and surface areas are the same as outlined in
Table 8-3.
Figure 8.15: Nitrate production as a function of dose for samples containing 50% (by volume) πΆππ2 and πππ2 and from water saturated air (no oxide)
System G(π΅πΆπβ) /
molecules 100 eV-1
Error (ππππππ)
No oxide 1.17 Β± 0.06
50% πΆππ2 (~6 g) 2.48 Β± 0.02
50% πππ2 (~11 g) 2.13 Β± 0.11
Table 8-12: Calculated G(ππ3β) values and standard deviation of the gradient for systems
with 50% oxide (by volume) and water saturated air (no oxide)
It is clear from Table 8-12 that the yields of nitrate in the presence of an oxide surface are
greater than when no oxide is present. Now that the interference from oxalate has been
removed, the nitrate yields are considerably reduced from the original apparent values
shown in Table 8-4. This reduction is greater in πππ2 systems, with the yield decreasing by
40% compared to less than 20% for samples containing πΆππ2 from the original value,
0.0
50.0
100.0
150.0
200.0
250.0
0.0 20.0 40.0 60.0 80.0 100.0
Nit
rate
pro
du
ctio
n /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV
No Oxide
CeO2
ZrO2
Chapter 8 Air Radiolysis Results and Discussion 7131060
216
suggesting that the interference from oxalate was far greater in πππ2 containing samples
than in πΆππ2 samples.
Figure 8.16 and Table 8-13 are the new refined data sets for systems containing 90% (by
volume) of oxide. The respective masses and surface areas are identical to values outlined in
Table 8-5.
Figure 8.16: Nitrate production as a function of dose for samples containing 90% (by volume) πΆππ2 and πππ2 and from water saturated air (no oxide)
System G(π΅πΆπβ) /
molecules 100 eV-1
Error (ππππππ)
No oxide 1.17 Β± 0.06
90% πΆππ2 (~12 g) 3.19 Β± 0.09
90% πππ2 (~20 g) 6.50 Β± 0.19
Table 8-13: Calculated G(ππ3β) values and standard deviation of the gradient for systems
with 90% oxide (by volume) and water saturated air (no oxide)
When the oxide volume is significantly larger than the volume of the gas phase, the yield of
nitrate produced is vastly increased. The G(ππ3β) values calculated are greater than the
0.0
50.0
100.0
150.0
200.0
250.0
300.0
350.0
400.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0
Nit
rate
pro
du
ctio
n /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV
No Oxide
CeO2
ZrO2
Chapter 8 Air Radiolysis Results and Discussion 7131060
217
values calculated for the 50% oxide (by volume) system. In the 90% πππ2 system, the nitrate
yield is six times greater than that measured for air radiolysis and is greater than the yield
calculated for the corresponding πΆππ2 system.
8.5.1 Compiled Data
To illustrate the yield of nitrate produced as a function of absorbed dose for the differing
oxide quantities present in the samples, Figure 8.17 is the compiled data set for samples
containing πΆππ2 and water saturated air. Table 8-14 lists the calculated G(ππ3β) yields and
the standard deviation of each set of data points.
Figure 8.17: Nitrate production as a function of absorbed dose for 1 g, 50% and 90% (by volume) πΆππ2 systems and for water saturated air (no oxide)
0.0
50.0
100.0
150.0
200.0
250.0
300.0
350.0
400.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0
Nit
rate
yie
ld /
(x1
01
6)
mo
lec.
Dose to Air / (x1016) 100 eV
No Oxide
1 g
50% (~6 g)
90% (~12 g)
Increasing oxide
surface area
Chapter 8 Air Radiolysis Results and Discussion 7131060
218
System G(π΅πΆπβ) /
molecules 100 eV-1 Error
(ππππππ) Surface Area /
m2
No oxide 1.17 Β± 0.06 N/A
1 g πΆππ2 2.07 Β± 0.07 7.42
50% πΆππ2 (~6 g) 2.48 Β± 0.02 44.5
90% πΆππ2 (~12 g) 3.19 Β± 0.09 89.0
Table 8-14: Calculated G(ππ3β) values and standard deviation of the gradient for systems
with 1 g, 50% and 90% (by volume) πΆππ2 and water saturated air (no oxide)
It is clear from Figure 8.17 that the initial βoff-stepβ in ππ3β concentration seen in Figure 8.8
has now been removed as a result of the oxalate interference being separated. It is also
evident that the presence of an oxide surface increases the yield of ππ3β. The largest
difference is seen with 1 g πΆππ2 in comparison with saturated air results where the yield of
ππ3β has almost doubled with the oxide present. This increase in nitrate production is due
to the presence of the oxide, however, it is not simply a surface area effect as this increase
in ππ3β yield is not linear with the higher loading of oxide data sets.
Figure 8.18 illustrates the compiled data for samples containing πππ2 and water saturated
air. The calculated G(ππ3β) yields are detailed in Table 8-15.
Chapter 8 Air Radiolysis Results and Discussion 7131060
219
Figure 8.18: Nitrate production as a function of absorbed dose for 1 g, 50% and 90% (by volume) πππ2 systems and water saturated air (no oxide)
System G(π΅πΆπβ) /
molecules 100 eV-1
Error (ππππππ)
No oxide 1.17 Β± 0.06
1 g πππ2 1.48 Β± 0.04
50% πππ2 (~11 g) 2.13 Β± 0.11
90% πππ2 (~20 g) 6.50 Β± 0.19
Table 8-15: Calculated G(ππ3β) values and standard deviation of the gradient for systems
with 1 g, 50% and 90% (by volume) πππ2 and water saturated air (no oxide)
It is clear from Figure 8.18 and Table 8-15 that the scatter seen in previous data (Figure
8.10) has now been removed. It is also evident that the presence of πππ2 (especially 90%
(by volume)) has a large effect on the yield of ππ3β produced. This increase is not linear with
mass or surface area as there is an order of magnitude difference in the mass of πππ2 in 1 g
and 50% (by volume) samples, however, the yield of ππ3β increases by 50%. Samples that
0.0
50.0
100.0
150.0
200.0
250.0
300.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0 180.0 200.0
Nit
rate
yie
ld /
(x1
01
6)
mo
lec.
Dose to Air / (x1016) 100 eV
No Oxide
1 g
50% (~11 g)
90% (~20 g)
Increasing oxide
surface area
Chapter 8 Air Radiolysis Results and Discussion 7131060
220
contain 1 g and 50% (by volume) of πππ2 have a lower yield of ππ3β than the corresponding
πΆππ2 samples.
8.5.2 Discussion
Section 2.7 outlined the mechanism for radiolysis of dry air and water saturated air. These
systems are well understood, with the stable products of dry air radiolysis being ozone (π3),
nitrous oxide (π2π) and nitrogen dioxide (ππ2) [108]. In the presence of water, the major
stable product is nitric acid (π»ππ3). Nitric acid is formed from ππ2 reacting with water
radiolysis products such as hydroxyl radicals (Reaction 8.2) and oxygen atoms (Reaction 8.3)
as well as with water itself (Reaction 8.4) [109, 110].
ππ2 + π»π. β π»ππ3 Reaction 8.2
ππ2 + π + π β ππ3. + π Reaction 8.3
2ππ2 + π»2π β π»ππ2 + π»ππ3 Reaction 8.4
In Reaction 8.4, nitrous acid (π»ππ2) is also produced which will be discussed later. The
nitrate radical formed in Reaction 8.3 can react with ππ2 to form dinitrogen pentoxide
(π2π5) (Reaction 8.5) [111] which can further react to form nitric acid (Reaction 8.6):
ππ3. + ππ2 β π2π5 Reaction 8.5
π2π5 + π»2π β 2π»ππ3 Reaction 8.6
The mechanism outlined above leads to the nitrate yield of 1.17 molecules 100 eV-1 of
absorbed dose seen in the saturated air samples. In the presence of an oxide powder
(independent of quantity) this yield is much higher and is closer to the limiting yield of G(π)
[42] which has a value of approximately 6 atoms 100 eV-1. The lower yield in saturated
Chapter 8 Air Radiolysis Results and Discussion 7131060
221
laboratory air radiolysis is due to the fast reaction of nitrogen atoms with ππ2 and ππ
(Reactions 8.7 and 8.8), which lead to the reformation of π2:
π + ππ2 β 2ππ Reaction 8.7
π + ππ β π + π2 Reaction 8.8
These reactions have rate constants of 5.9x10-12 cm3 molecule-1 s-1 and 2.2x10-11 cm3
molecule-1 s-1 respectively.
When an oxide is present, Reaction 8.7 is inhibited, allowing higher yields of nitrate to be
produced. The most plausible explanation is that ππ2 is adsorbed to the oxide surface and
undergoes reactions including Reactions 8.2-8.4 to produce nitric acid.
The oxidation of ππ2 on an oxide surface has been investigated by Rodriguez et al. [112]
who investigated the reaction of ππ2 with stoichiometric πΆππ2 and with partially reduced
ceria ( πΆππ2βπ₯ ) from an environmental catalysis perspective. At room temperature,
adsorbed nitrate was the only major product found on pure πΆππ2 with a mixture of π, ππ
and ππ3 co-existing on the surface of partially reduced ceria.
The phenomenon is also known to occur with other oxide materials. Nanayakkara et al. have
studied the reactivity of several atmospheric gases with πππ2 and found that 96% of ππ2
reacts with surface hydroxyl groups to form bridged, mono and bidentate nitrate [113]. The
overall reaction is given in Reaction 8.9 and the bridging modes are illustrated in Figure
8.19. This is confirmed in other work by Hadjiivanov et al. [114].
3ππ2 (π) + 2ππ»β β 2ππ3 (πππ )β + ππ(π) + π»2π(πππ ) Reaction 8.9
Chapter 8 Air Radiolysis Results and Discussion 7131060
222
Figure 8.19: Pictorial representation of ππ3β bonding modes with metal centres depicting
(l-r) monodentate, bidentate and bridging adsorption modes
Haubrich et al. have proposed an alternative mechanism for ππ3β formation on a rutile
(πππ2) surface, which involves the disproportionation of adsorbed ππ2 (Reaction 8.10)
[115]:
2ππ2 (πππ ) β ππ3 (πππ )β + ππ(πππ ) Reaction 8.10
The ππ species will initially be adsorbed to the surface but will quickly desorb to the gas
phase due to the weak adsorption [116].
Chromia (πΆπ2π3) is another oxide where ππ2 adsorption leads to the formation of ππ3β on
the surface [117].
All of these systems mentioned above used ultra-high vacuum (UHV) conditions and studied
the adsorption and oxidation of ππ2 using infra-red spectroscopy. Radiation, in any form
was not utilised as part of the research.
Harteck and Dondes studied the decomposition of ππ and ππ2 using fission fragments
from uranium-235 [43]. They postulated that π2, π2π and π2 were the stable species,
however, analysis was carried out by pressure measurements alone. Nitrogen dioxide
decomposition was an order of magnitude slower than ππ decomposition and they did not
see any surface effects. The main reason for this negative result is the small quantity of
oxide powder utilised in the research (5 mg).
Chapter 8 Air Radiolysis Results and Discussion 7131060
223
Another possible explanation for the increased yields of ππ3β in the presence of an oxide
powder is that of energy transfer from the oxide to the gas phase. This phenomenon was
discussed in detail in Section 2.3 with respect to water radiolysis on an oxide surface. One
explanation for the enhancement of π»2 yield from adsorbed water radiolysis was due to the
similarities in the band gap of certain metal oxides and the bond dissociation energy of
water (5.15 eV) [25]. The band gaps of πππ2 and πΆππ2 are 5.0 eV [76] and 3.1-3.5 eV
[77, 118], respectively. The ionisation potentials of π2 and π2 are 15.58 and 12.07 eV,
respectively [85]. The bond dissociation energies of π β‘ π and π = π are 9.79 and 5.15 eV,
respectively [27]. Therefore there is not enough βexcitation energyβ available to be
transferred from either metal oxide utilised in this research to directly ionise or dissociate
π2. It is also unlikely that π2 will adsorb to the oxide surface.
From the explanation outlined above, initial ionisation of π2 and π2 occurs in the gas phase.
The surface will only have an effect on subsequently formed species, which will be
molecular, radical or ionic in character.
In all of the experiments investigated in this chapter, nitrite (ππ2β) is not present in any of
the post-irradiated chromatograms. Reaction 8.4 outlined the formation of nitrous acid
(π»ππ2) in the reaction mechanism, however, this isnβt present in the final system. Work by
Saliba et al. have found that adsorbed nitrous acid undergoes decomposition on silica
surfaces [119], as shown in Reaction 8.11:
2π»ππ2 (πππ ) β ππ + ππ2 + π»2π(πππ ) Reaction 8.11
Nitrite can also be oxidised on the surface by ππ». to form nitric acid.
Chapter 8 Air Radiolysis Results and Discussion 7131060
224
8.6 Oxalate
It is clear from Section 8.4 that oxalate (πΆ2π42β) is present in the post irradiated samples that
contain πππ2. It is important to quantify the yield of oxalate and to determine whether it is
a contaminant or a radiolytically produced species. Now that the oxalate signal has been
identified and separated from the nitrate signal, it is possible to detect the yield of both
anions in parallel for each sample. It is necessary to calibrate the response of the ion
chromatograph detector to oxalate in order to determine an accurate yield. To achieve this,
oxalic acid (π»2πΆ2π4) was used as a source of oxalate anions and several solutions over a
range of concentration similar to the concentrations used in calibrating the ion
chromatograph with nitrate (Section 8.1) were utilised. The resulting calibration plot is
shown in Figure 8.20:
Figure 8.20: Calibration plot of πΆ2π42β peak area as a function of π»2πΆ2π4 concentration
using ion chromatography
From this figure, it can be seen that the detector has a linear response to oxalate
concentration in the range of 0.05-1 mM. In comparison with Figure 8.1, the sensitivity for
both anions is very similar, with almost identical peak areas for the same concentration of
anions.
y = 61.886x RΒ² = 0.9986
0.0
10.0
20.0
30.0
40.0
50.0
60.0
70.0
0.0 0.2 0.4 0.6 0.8 1.0 1.2
Pe
ak a
rea
/ A
.U.
[H2C2O4] / mM
Chapter 8 Air Radiolysis Results and Discussion 7131060
225
Figure 8.21 is the compiled data set for oxalate yields in the system containing πΆππ2:
Figure 8.21: Plot of oxalate production as a function of absorbed dose for samples containing 1 g, 50% and 90% (by volume) of πΆππ2 and from water saturated air (no oxide)
From this plot, there appears to be a lot of scatter in the sample sets containing 50% and
90% πΆππ2 when compared to samples of water saturated air and 1 g πΆππ2. However, the
maximum yield of oxalate detected is 66.4 nmol in the system containing 90% πΆππ2; this
yield is an order of magnitude below the yield of nitrate for the corresponding system.
Therefore the scatter in Figure 8.21 is an effect of the detection limits of the ion
chromatograph. Samples without πΆππ2 appear to have the least scatter. The G-value for this
data set has been calculated as G(πΆ2π42β) = 0.03 molecules 100 eV-1.
Figure 8.22 shows the calculated oxalate yields in samples containing πππ2 and pure air:
0.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
9.0
10.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0
Oxa
late
yie
ld /
(x1
01
6)
mo
lec.
Dose to Air / (x1016) 100 eV
No Oxide
1 g
50% (~6 g)
90% (~12 g)
Chapter 8 Air Radiolysis Results and Discussion 7131060
226
Figure 8.22: Plot of oxalate production as a function of absorbed dose for samples containing 1 g, 50% and 90% (by volume) of πππ2 and from water saturated air (no oxide)
It is clear from comparing Figures 8.21 and 8.22 that the yield of oxalate is much higher in
samples containing πππ2 than in the corresponding πΆππ2 samples. The yield is up to five
times greater in 90% πππ2 (0.41 Β΅mol) than in 90% πΆππ2 (66.4 nmol). This large yield of
oxalate led to the large scatter seen in πππ2 samples at low doses (Figure 8.10).
0.0
5.0
10.0
15.0
20.0
25.0
30.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0 180.0 200.0
Oxa
late
yie
ld /
(x1
01
6)
mo
lec.
Dose to Air / (x1016) 100 eV
No Oxide
1 g
50% (~11 g)
90% (~20 g)
Chapter 8 Air Radiolysis Results and Discussion 7131060
227
8.6.1 Oxalate Discussion
It is of importance to understand the source of the oxalate, whether it is an impurity from
the oxide or from the gas phase. Once the source has been identified, the mechanism of its
formation can be discussed.
Both πππ2 and πΆππ2 are produced commercially by calcination of zirconium and cerium
containing compounds. One such compound is the oxalate. This is also true of ππ’π2, as
outlined in Chapter One. To determine whether oxalate is present in the starting oxide,
thermogravimetric analysis of cerium oxalate (πΆπ2πΌπΌπΌ(πΆ2π4)3. π₯π»2π) was investigated to
determine the thermal stability of the oxalate group. Figure 8.23 shows the thermograms of
πΆπ2πΌπΌπΌ(πΆ2π4)3. π₯π»2π decomposed under both air and π2:
Figure 8.23: Thermogravimetric analysis of cerium oxalate under π2 (blue) and static air (red) atmospheres. Heating rate 2 Β°C min-1
This figure highlights that there are three distinct mass changing events as the oxalate is
heated. The first step occurs between 35-130 Β°C, with this initial step being due to the water
of crystallisation being driven off. This step occurs at the same temperature, independent of
45.0
50.0
55.0
60.0
65.0
70.0
75.0
80.0
85.0
90.0
95.0
100.0
0.0 100.0 200.0 300.0 400.0 500.0 600.0
Mas
s /
%
Temperature / oC
N2
Air
Step 1
Step 2
Step 3
Chapter 8 Air Radiolysis Results and Discussion 7131060
228
flow gas, thus showing that this dehydration step is thermally driven rather than reaction
with the gas. This mass difference is approximately 15% therefore the number of water
molecules bound to the compound can be calculated as 5.4. The second step occurs
between 130-180 Β°C in both atmospheres and represents a mass change of approximately
3%. Due to the nature of the mass change, this step is assumed to be further dehydration of
the solid with loss of strongly bound water. The final mass change event is dependent on
flow gas used. In an air flow, this step occurs at 220 Β°C and at 350 Β°C under an π2 flow. This
step corresponds to the decomposition of the oxalate group.
During the decomposition of cerium oxalate into cerium oxide, cerium is oxidised from πΆππΌπΌπΌ
to πΆππΌπ; in an inert atmosphere there is nothing to oxidise the oxalate until it becomes
unstable and undergoes self-decomposition, whereas in oxidising atmospheres such as π2
or air, this oxidation occurs much quicker. This can be seen by the difference in the
temperature onset of the final step. The oxygen in the air starts to decompose the oxalate
130 Β°C below the temperature at which this starts to occur under π2. The steps outlined
above (dehydration followed by decomposition) have been investigated and confirmed by
other groups [120, 121]. The decomposition of cerium oxalate occurs in two distinct steps in
an air atmosphere, independent of heating rate employed [121, 122] suggesting that this
step is thermodynamically controlled. However, in a recent paper, De Almeida et al.
discovered under an argon flow, that an intermediate decomposition step occurred which
led to an oxy-carbonate intermediate with the chemical formula πΆπ2π2πΆπ3 [120]. This step
is not present however, in Figure 8.23 or at least not resolved.
After the heating program was completed, the sample decomposed in an air atmosphere
had 50% of the initial mass. Under π2, this value was 55.4%. The difference in final mass is
Chapter 8 Air Radiolysis Results and Discussion 7131060
229
due to the incomplete decomposition of the oxalate group and residual carbon in the
sample decomposed under π2.
In Section 3.4.3, the regeneration of the oxide powders between subsequent experiments
was outlined. The powders are baked at 400 Β°C for six hours under a static air atmosphere.
From Figure 8.23 it is clear that this temperature is sufficient to ensure complete
decomposition of any oxalate impurity. Therefore the source of the oxalate discovered in
the ion chromatograms is not an impurity from the solid.
The only other source of carbon during the experiments is carbon dioxide (πΆπ2) in the air.
The DRIFT spectra in Chapter Six of the regenerated oxides (Figures 6.8 and 6.18) identified
the presence of πΆπ2 compounds adsorbed onto the surfaces of both oxide materials. These
figures only gave qualitative information, therefore the concentrations of πΆπ2 present in the
pre-irradiated samples is unknown, however, a maximum concentration can be calculated in
the gas phase. The concentration of πΆπ2 in the atmosphere is approximately 400 ppm. In
the 12 ml sample vials used in this experiment, that is equal to 0.11 mmol of πΆπ2. Assuming
that two πΆπ2 molecules will dimerise to form one oxalate molecule, the maximum
theoretical yield of oxalate is 54.5 Β΅mol in pure air. Samples that contain 90% (by volume) of
oxide could generate a maximum yield of 47.0 Β΅mol for πΆππ2 containing samples and 10.8
Β΅mol for πππ2 containing samples. These maximum yields are far greater than the
measured yields of oxalate in Figures 8.21 and 8.22. The efficiency of the reaction assuming
simple dimerisation is 0.14% in the presence of πΆππ2 and 3.84% in the presence of πππ2.
These figures are based on the gas phase concentration of πΆπ2 and do not include any πΆπ2
adsorbed onto the oxide surface.
Chapter 8 Air Radiolysis Results and Discussion 7131060
230
Carbon dioxide is very radiation stable with less than 0.1% undergoing decomposition in gas
phase studies alone. Initially, it was postulated by Hirschfelder and Taylor that this was due
to the back reaction with ozone [123] (Reaction 8.12)
πΆπ + π3 β πΆπ2 + π2 Reaction 8.12
This reaction is exothermic, however, it has a rate coefficient of k β€ 4x10-25 cm3 molecule-1
sec-1 at ambient temperature [124], therefore would be very slow. Work by Harteck and
Dondes [125] outlined the following reaction mechanism for πΆπ2 radiolysis:
Initial ionisation πΆπ2 β πΆπ + π Reaction 8.13
β πΆ + 2π Reaction 8.14
Reaction 8.13 has a G-value of 8 molecule 100 eV-1 and is the more favoured primary
reaction of πΆπ2 irradiation. The reaction continues thus:
πΆπ + πΆ + π β πΆ2π + π Reaction 8.15
πΆ2π + πΆπ + π β πΆ3π2 + π Reaction 8.16
π + π2 + π β π3 + π Reaction 8.17
πΆ3π2 + π (or π3) β πΆ2π + πΆπ2(+π2) Reaction 8.18
πΆπ + π + π β πΆπ2 + π Reaction 8.19
The π2 in Reaction 8.17 is formed by the recombination of oxygen atoms from Reaction
8.14. Dicarbon monoxide (πΆ2π), acts as a catalyst in Reaction 8.19 before eventually
diffusing to the walls with carbon suboxide (πΆ3π2), and forming polymerised products.
Chapter 8 Air Radiolysis Results and Discussion 7131060
231
As πΆπ2 is the only source of carbon in the experimental configuration, another mechanism
must be occurring to hinder the reformation of πΆπ2, as the yields of oxalate are greater than
from 0.1% πΆπ2 decomposition.
An explanation is given by Harteck and Dondes [125] where they found that a small quantity
of ππ2 prevented the reformation of πΆπ2 by reaction with radicals. As outlined in Section
8.5.1, ππ2 will be present in the system due to radiolysis of π2 and π2. The reactions of ππ2
in the system are shown below:
π + ππ2 β ππ + π2 Reaction 8.20
πΆ + ππ2 β ππ + πΆπ Reaction 8.21
2ππ + π2 β 2ππ2 Reaction 8.22
Reaction with oxygen atoms (8.20) inhibits both Reactions 8.18 and 8.19, both of which lead
to the reformation of πΆπ2, and reaction with carbon atoms (8.21) leads to a lower yield of
πΆ2π which is the catalyst in Reaction 8.19. With ππ2 present, G(βπΆπ2) = 8 molecules
100 eV-1.
The mechanism outlined above will be occurring in the saturated air experiments. The G-
value for oxalate formation in this system is G(πΆ2π42β) = 0.03 molecules 100 eV-1 based on
dose absorbed by the air. It is clear from Figures 8.21 and 8.22 that the yield of oxalate in
samples with an oxide present are much greater, therefore a mechanism involving the
surface that inhibits the reformation of πΆπ2 must be occurring. It is postulated that πΆπ2
adsorbs onto the oxide prior to irradiation and then is reduced on the oxide surface during
irradiation forming πΆπ2β. If there are two reduced molecules in close proximity, these will
undergo dimerisation to form the oxalate (Reaction 8.23).
Chapter 8 Air Radiolysis Results and Discussion 7131060
232
2πΆπ2β + π β πΆ2π4
2β + π Reaction 8.23
Carbon dioxide adsorption onto metal oxide surfaces has been investigated by
Baltrusaitis et al. for several nanoparticle surfaces [68]. They studied πΆπ2 adsorption to iron
(III) oxide (πΉπ2π3), aluminium oxide (π΄π2π3) and titanium dioxide (πππ2) in the presence and
absence of water vapour. They found that πΆπ2 readily reacts with surface hydroxyls to form
bicarbonate species (π»πΆπ3β). Carbon dioxide will also react to form monodentate and
bidentate carbonate species (πΆπ32β). Carboxylate (πΆπ2
β) is also present on the surface of
πππ2. All of these species were formed under dry conditions. When co-adsorbed water was
present, they found that the carbonate species became solvated and the surface hydroxyl
groups became protonated. This occurs when no radiation is present, therefore in the
presence of ionising radiation, reduction of πΆπ2 is likely to be increased, leading to a higher
concentration of πΆπ2β on the oxide surface and therefore a higher concentration of oxalate
formation.
8.7 Synthetic Air
In an effort to remove πΆπ2 from the system, a series of samples were out-gassed with
synthetic air. Synthetic air is produced by mixing 20% π2 with 80% π2, the impurities are
certified as < 1 vppm πΆπ2, < 2 vppm π»2π and < 1 vppm πππ₯. This was achieved by inserting
a needle through the septa of the vial and flowing gas through the sample for several
minutes. Figure 8.24 highlights the nitrate yield results of pure synthetic air radiolysis
compared to laboratory air and water saturated lab air:
Chapter 8 Air Radiolysis Results and Discussion 7131060
233
Figure 8.24: Plot of nitrate production as a function of absorbed dose for synthetic air, laboratory air and water saturated laboratory air. Volume of air =11.9 - 12.0 cm3 at 35 Β°C
In theory, there should be no nitrate produced in the radiolysis of synthetic air, because as
previously discussed in Section 2.7, radiolysis of dry air, results in the steady state
concentrations of ozone (π3), nitrous oxide (π2π) and nitrogen dioxide (ππ2) [108]. Figure
8.24 clearly shows that nitrate is produced and in the same yields as normal lab air,
therefore it can be hypothesised that water is present in the system, either as water vapour
that hasnβt been fully removed or as silanol groups on the glass surface of the vials.
As seen in previous results, there is a large quantity of water present in the systems
containing an oxide powder as adsorbed water. Therefore, the yield of nitrate did not
change when samples containing an oxide were irradiated in a synthetic air atmosphere.
The oxalate yield in samples containing πΆππ2 that were irradiated in synthetic air did not
differ from the yields seen in Figure 8.21. This yield was very small in laboratory air,
therefore it is likely that a small quantity of πΆπ2 remains adsorbed to the oxide surface even
after out-gassing with synthetic air, which can be irradiated to form the oxalate species. It is
0.00
20.00
40.00
60.00
80.00
100.00
120.00
0.00 20.00 40.00 60.00 80.00 100.00 120.00 140.00
Nit
rate
pro
du
ctio
n /
(x1
01
6)
mo
lec.
Dose to air / (x1016) 100 eV
Lab. AirAir (H2O added)Synthetic air
Chapter 8 Air Radiolysis Results and Discussion 7131060
234
likely that the out gassing method used was not adequate enough to displace adsorbed
species on the oxide.
Samples containing πππ2 that were irradiated in synthetic air had a markedly reduced yield
of oxalate after subsequent analysis. The yields were similar to comparative samples of
πΆππ2. The explanation of this is likely to be inadequate removal of adsorbed species.
8.8 Sintered πͺππΆπ
In all previous experiments, the same batch of πΆππ2 and πππ2 has been used. These oxides
have a disparity in surface area of approximately three. To investigate the effect of surface
area on the radiolysis of air, a sample of πΆππ2 was sintered at 950 Β°C under static air for two
hours using a heating rate of 10 Β°C min-1. The following section outlines the sintered oxide
properties and subsequent experimental results.
8.8.1 Oxide Properties
Figure 8.25 represents the BET adsorption isotherm for the sintered oxide product. The
surface area was calculated as 2.20 m2 g-1. This is a decrease of 70% and is approximately
the same surface area as the πππ2 samples used in previous experiments.
Chapter 8 Air Radiolysis Results and Discussion 7131060
235
Figure 8.25: BET adsorption (solid trace) β desorption (dashed trace) isotherm of πΆππ2 sintered at 950 Β°C for 2 h
As seen in Figures 6.3 and 6.6, the adsorption-desorption isotherm for sintered πΆππ2 is of
type three [65]. The isotherm also has hysteresis, indicating that the oxide still has a porous
structure, however, the size of this loop has decreased indicating the loss of porosity. The
quantity of nitrogen adsorbed has reduced by 60% indicating the decrease in the BET
surface area.
After sintering, the bulk density has increased from 1.44 to 2.23 g cm-3. This is an increase of
approximately 55% and is to be expected as the porous structure becomes annealed at
higher temperatures. The increase in bulk density leads to increase masses of oxide needed
for 50% and 90% (by volume) samples. The mass of sintered πΆππ2 required is 13.5 g for 50%
volume samples and 24 g for 90% volume samples.
SEM and EDS data for sintered πΆππ2 are shown in Figure 8.26:
0.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
0 0.2 0.4 0.6 0.8 1
Qu
anti
ty a
dso
rbed
/ c
m3
g-1
Relative pressure / (P/Po)
Chapter 8 Air Radiolysis Results and Discussion 7131060
236
i)
ii)
Figure 8.26: i) Scanning electron micrograph and ii) EDS spectra for sintered πΆππ2
From the SEM image, it is clear that there is no dominant crystal morphology, this was
evident in the un-sintered πΆππ2 (Figure 6.1). The average particle size has not changed
drastically in Figure 8.26i, with an average area of 5 Β΅m2. The EDS data shows that there is
no change in the elemental make-up of the oxide, with cerium and oxygen, the major
constituents, and silicon and carbon present as an impurity and from the carbon stub
respectively.
Chapter 8 Air Radiolysis Results and Discussion 7131060
237
8.8.2 Nitrate Production over Sintered πͺππΆπ
Figure 8.27 and Table 8-16 outlines the compiled results for nitrate yield as a function of
absorbed dose for the sintered πΆππ2 system.
Figure 8.27: Nitrate production as a function of absorbed dose for samples containing 1 g, 50% and 90% (by volume) sintered πΆππ2 and from water saturated air (no oxide)
System G(π΅πΆπβ) /
molecules 100 eV-1 Error (ππππππ)
No oxide 1.17 Β± 0.06
1 g sintered πΆππ2 1.21 Β± 0.07
50% sintered πΆππ2
(~13.5 g)
2.35 Β± 0.17
90% sintered πΆππ2
(~24 g)
2.59 Β± 0.22
Table 8-16: Calculated G(ππ3β) values and standard deviation of the gradient for systems
containing 1 g, 50% and 90% (by volume) sintered πΆππ2 and water saturated air (no oxide)
0.0
20.0
40.0
60.0
80.0
100.0
120.0
0.0 10.0 20.0 30.0 40.0 50.0 60.0 70.0 80.0 90.0
Nit
rate
yie
ld /
(x1
01
6)
mo
lec
Dose to Air / (x1016) 100 eV
No Oxide
1 g
50% (~13.5 g)
90% (~24 g)
Chapter 8 Air Radiolysis Results and Discussion 7131060
238
It is clear from Table 8-16 that the yield of nitrate increases with growing mass of sintered
πΆππ2 which is in agreement with un-sintered πΆππ2 (Table 8-14). However, this increase is
not directly related to the mass of πΆππ2 present in the sample. The mass of πΆππ2 in the 50%
and 90% samples is over double the quantity of πΆππ2 present in the un-sintered samples,
however, the yield has not doubled. This suggests that the formation of nitrate is not purely
a mass driven process.
8.8.3 Comparison with Un-sintered πͺππΆπ Results
Figure 8.28 outlines the comparative results for samples containing either regenerated or
sintered πΆππ2 and Table 8-17 details the respective masses, surface areas and nitrate yields
for the regenerated and sintered πΆππ2 samples.
Figure 8.28: Compiled data plot of nitrate production as a function of dose for systems containing 1 g, 50% and 90% (by volume) regenerated πΆππ2, 1 g, 50% and 90% (by volume)
sintered πΆππ2 and from water saturated air (no oxide)
0.0
50.0
100.0
150.0
200.0
250.0
300.0
350.0
400.0
0.0 20.0 40.0 60.0 80.0 100.0 120.0
Nit
rate
yie
ld /
(x1
01
6)
mo
lec
Dose to Air / (x1016) 100 eV
1 g 1 g sin
50% (~6 g) 50% sin (~13.5 g)
90% (~12 g) 90% sin (~24 g)
No Oxide
Chapter 8 Air Radiolysis Results and Discussion 7131060
239
Regenerated πͺππΆπ Sintered πͺππΆπ
System Mass
/ g
Surface
Area / m2
G(π΅πΆπβ) /
molecules
100 eV-1
Error
(ππππππ)
Mass
/ g
Surface
Area / m2
G(π΅πΆπβ) /
molecules
100 eV-1
Error
(ππππππ)
No
Oxide
- - 1.17 Β± 0.06 - - 1.17 Β± 0.06
1 g 1 7.42 2.07 Β± 0.07 1 2.2 1.21 Β± 0.07
50% ~6 44.5 2.48 Β± 0.02 ~13.5 29.7 2.35 Β± 0.17
90% ~12 89.0 3.19 Β± 0.09 ~24 52.8 2.59 Β± 0.22
Table 8-17: Comparison between calculated G(ππ3β) for samples containing either
regenerated πΆππ2 or sintered πΆππ2 and water saturated air (no oxide)
An initial observation is that the yield of nitrate is greater in samples containing regenerated
πΆππ2 than the corresponding sintered πΆππ2 samples, however, this observation does not
account for the difference in surface area available in the system.
8.8.4 Discussion
As discussed in Section 8.5.2, the higher yields of nitrate observed in oxide containing
systems is hypothesised to be due to the adsorption of ππ2 which inhibits the back reaction
with nitrogen atoms (Reactions 8.7 and 8.8). To determine whether a decrease in the area
of surface available for ππ2 to adsorb to, reduces the yield of nitrate produced, Figure 8.29
is a plot of G(ππ3β) as a function of surface area for the three types of oxide used in this
research:
Chapter 8 Air Radiolysis Results and Discussion 7131060
240
Figure 8.29: Plot of G(ππ3β) as a function of surface area for the three oxide systems utilised
in this research and for reference, the water saturated air (no oxide) yield
It is clear from this figure that the difference in G(ππ3β) values seen in Table 8-17 correlates
with an increase in surface area present in the system. Figure 8.29 highlights that there is a
linear relationship between surface area and yield of nitrate formed in samples containing
πΆππ2 of differing surface areas. When there is little surface available for adsorption of ππ2,
as in 1 g samples of low SSA oxides, the yield of nitrate is comparable to that of water
saturated air. In these systems, the oxide equates to less than 5% of the total volume.
Therefore, the majority of the chemistry will occur in the gas phase and the surface will only
play a role when reactive species in the gas phase have diffused to the surface.
The mean free path can be used as an approximation for the distance travelled by a species
before interacting with another species. Equation 8.2 can be used to determine this value:
πΏ = (ππ)β1 Equation 8.2
0.00
1.00
2.00
3.00
4.00
5.00
6.00
7.00
0.0 20.0 40.0 60.0 80.0 100.0
G(N
O3
- )
Surface area / m2
H2O sat. air
Regenerated CeO2
Sintered CeO2
ZrO2
Chapter 8 Air Radiolysis Results and Discussion 7131060
241
where πΏ is the mean free path (in metres), π is the collision cross-section (in m2) and π is the
number of molecules (per m3).
The mean free path of an π2 molecule is approximately 6.6x10-8 m in air at 1 atmosphere of
pressure and 20 Β°C [126]. The collisional cross section value is very similar for π2 therefore
the mean free path will not differ dramatically. In the samples containing 1 g of oxide, there
is approximately 2.5 cm of headspace above the powder; from this mean free path, it is
evident that the majority of species generated in the gas phase will have reacted before
reaching the surface. Species within this distance from the surface will adsorb to the surface
and inhibit the back reaction with other gas phase species. This is why the G(ππ3β) for 1 g
systems are slightly above the value for saturated air samples. In samples with higher
loading of oxides, the distance needed to travel by a gas phase species before encountering
a surface is greatly reduced, therefore adsorption of ππ2 will be greater, leading to the
higher yields of nitrate reported throughout this chapter.
πππ2 initially follows the trend in Figure 8.29, however, samples containing 90% oxide have
a much higher yield than would be expected. As explained in Section 8.5.2, the band gap of
πππ2 is too low to directly ionise π2 or π2, however, it will greatly increase the radiolysis of
adsorbed water and the species generated from this (as seen in Chapter Seven). This higher
concentration of water radiolysis species (namely ππ». and π» atoms) will increase the yield
of nitrate produced (Reaction 8.2).
Chapter 8 Air Radiolysis Results and Discussion 7131060
242
Conclusions
The radiolysis of pure air reaches a maximum nitrate yield of 83 ΞΌmol L-1 due to the
exhaustion of water vapour in the system. The G-value for nitrate formation is 1.39
molecules 100 eV-1 absorbed energy.
In the presence of an oxide powder, the yield of nitrate greatly increases due to the surface
acting as a sink for ππ2 which inhibits the back reaction with π atoms to reform π2. The
yield of nitrate increases proportionally to the quantity of surface area available in the
sample. However, this trend is not followed by samples containing 90% (by volume) of
πππ2, which produces significantly higher yields of nitrate with a G(ππ3β) = 6.5 molecules
100 eV-1. This value is close to the limiting yield of G(π) = 6 atoms 100 eV-1. This large
increase in nitrate formation is due to the higher concentration of ππ»β from the radiolysis of
adsorbed water on the πππ2 surface. This species enhances nitrate formation in the
following reaction:
ππ2 + π»π. β π»ππ3 Reaction 8.2
Reducing the surface area of πΆππ2 from 7.42 to 2.2 m2 g-1 in turn reduces the yield of nitrate
formed due to the relationship between nitrate formation and the surface area present in
the system.
Carbon dioxide (πΆπ2) in the atmosphere gets reduced on the oxide surface and undergoes
dimerisation to form oxalate (πΆ2π42β). The yields are far greater in the presence of πππ2
than corresponding πΆππ2 samples. The yield of oxalate, however, is an order of magnitude
below the yield of nitrate formation in corresponding samples. There is very little oxalate
formed in pure air samples due to the reaction outlined below:
Chapter 8 Air Radiolysis Results and Discussion 7131060
243
πΆπ + π + π β πΆπ2 + π Reaction 8.19
Irradiating samples in synthetic air atmospheres removes a large quantity of πΆπ2 from the
gas phase and the yields of oxalate in πππ2 samples are reduced to the level of πΆππ2
samples. Due to πΆπ2 adsorbed to the oxide surface prior to irradiation, there is still oxalate
present in the post-irradiated samples.
Irradiating in synthetic air atmospheres had no effect on the nitrate yield as the water
adsorbed onto the oxide powder far outweighs the quantity of water vapour in the
headspace (Tables 8-2, 8-3 and 8-5) and, in pure air samples, the silanol (ππ β π β π»)
groups on the glass vials lead to nitric acid formation.
In all the systems investigated in this chapter, nitrite (ππ2β) is absent from the post-
irradiated chromatogram. This is due to the decomposition of nitrous acid on the surface as
outlined below:
2π»ππ2 (πππ ) β ππ + ππ2 + π»2π(πππ ) Reaction 8.11
Chapter 9 Final Conclusions 7131060
244
9 Final Conclusions
This chapter pulls together the conclusions drawn from π»2 β π2 β π΄π radiolysis studies in
the presence or absence of an oxide surface using Ξ³-rays and π»π2+ accelerated ions that
were discussed in Chapter Seven and the results of air radiolysis in the presence or absence
of an oxide surface using Ξ³-rays discussed in Chapter Eight.
9.1 π―π β πΆπ System
The development of a suitable reaction vessel to investigate the radiation chemistry of
π»2 β π2 β π΄π gas mixtures has been achieved, after several iterations of design. With these
iterations, development of the analysis technique was needed.
60πͺπ Studies
In homogeneous systems, the recombination of π»2 β π2 appears to be independent of
concentration of either gas. The G(-π»2) values in the range of 3.5-4.7 molecules 100 eV-1
were calculated, which is in good agreement with literature. The corresponding G(-π2)
values are within the range of 1.8-4.2 molecules 100 eV-1. The average ratio of G(-π»2) to
G(-π2) is 1.44. As this value is greater than one, it suggests that hydrogen peroxide (π»2π2) is
not the stable product in this system.
Addition of an oxide surface greatly increased the rate of recombination. At low doses, π»2
from radiolysis of adsorbed water is detected, however, this is soon depleted. It is not
known at this time whether, the effect of the oxide surface is catalytic, radiolytic or simply
as a surface for species to be adsorbed onto.
Chapter 9 Final Conclusions 7131060
245
In all of these systems, a steady state is not reached, therefore the rate of recombination is
greater than the rate of water vapour radiolysis.
π―ππ+Studies
Development of an adequate reaction vessel to investigate the recombination of π»2 β π2
using accelerated ions as a radiation source has been completed and preliminary
experiments have been undertaken.
Ethylene gas has been utilised as a secondary dosimeter to validate the absolute current
measurements. The results are within 5% of literature values, instilling confidence in the
absorbed dose calculations for this system.
In the results attained so far irradiating mixtures of π»2 β π2 β π΄π gas, π»2 continues to be
depleted with absorbed dose and no steady state is reached between π»2 β π2
recombination and radiolysis of water vapour. The G(-π»2) values calculated for this data lie
in the range of 4.7-5.4 molecules 100 eV-1, in good agreement with 60πΆπ Ξ³-ray studies.
Preliminary results highlight the absence of a linear energy transfer (LET) effect between
60πΆπ Ξ³-rays and accelerated π»π2+ ions, as is to be expected with gaseous systems.
9.2 Air Radiolysis System
The presence of an oxide surface, greatly increases the yield of nitric acid in the radiolysis of
air system. G(π»ππ3) values increase from 1.17 molecules 100 eV-1 in moist air, to
3.19 molecules 100 eV-1 in the presence of πΆππ2 and 6.5 molecules 100 eV-1 in the
presence of πππ2. It is hypothesised, that this increase is due to the surface acting as a sink
for ππ2 and thus preventing the back reaction to π2 (Reactions 8.7 and 8.8).
Chapter 9 Final Conclusions 7131060
246
The presence of an oxide surface also leads to the formation of oxalate (πΆ2π42β), from the
dimerisation of πΆπ2 in the air.
Decreasing the surface area of πΆππ2 leads to a reduction of nitric acid formation in
proportion to higher surface area πΆππ2.
Conclusion
In canisters of ππ’π2, it is likely that both of these systems may be occurring simultaneously.
It is not known what effect, one system may have on the other. The presence of the ππ’π2
leads to a very complex system with redox chemistry occurring on the surface, as well as
energy transfer from the solid to adsorbed species and gaseous species.
Hopefully this research has added to the knowledge gap that was outlined in Chapter Two,
however, more work is needed to achieve a complete understanding of the mechanism
occurring inside ππ’π2 storage canisters.
Chapter 10 Future Work 7131060
247
10 Future work
While the research chapters of this thesis have gone some way in exploring the radiation
chemistry of gaseous systems in contact with an oxide surface, there are still many areas in
which this research could be developed further. These are discussed below in the context of
specific experiments and general research directions.
10.1 π―π β πΆπ β π¨π System
To further elucidate the reaction mechanism of π»2 β π2 recombination, a kinetic model of
elementary reactions could be developed. Foy and Joyce have tried to model the chemistry
occurring inside ππ’π2 canisters, however, this work is very preliminary and is not extensive
[127]. Modelling of a compiled reaction scheme taken from the extensive photochemistry
literature may help to explain the zero order nature of the gas phase radiolysis results
presented in Section 7.6. Once good agreement has been reached with this gas phase
chemistry model, a surface can then be added to incorporate the chemistry occurring at an
oxide surface such as in ππ’π2 canisters. Development of this model would require
significant effort as rate constants for many of the important three-body reactions are yet to
be determined.
Section 8.8 detailed results of air radiolysis experiments using sintered πΆππ2. This study was
performed to determine the effect of SSA on the radiation chemistry of moist air. A similar
experiment was not performed to investigate π»2 β π2 recombination, and it is therefore,
not clear if the difference in results for πΆππ2 and πππ2, presented in Section 7.7, is due to
SSA effects or chemical differences. Experiments with particles of the same oxides of
Chapter 10 Future Work 7131060
248
differing surface areas should be investigated to determine the effect of SSA on π»2 β π2
recombination.
10.2 Air Radiolysis System
Figure 8.29 highlighted an increase in the radiolytic production of ππ3β, with an increase of
surface area. In this research the surface area of the two oxides of interest were in the
range of 2-8 m2 g-1, this surface area is analogous to ππ’π2 currently in storage. To
determine the extent of this trend, πΆππ2 and πππ2 with higher surface areas (100βs m2 g-1)
such as nano-particles should be investigated.
10.3 πͺππ―π System
By chance, it has been shown in this research, that decomposition of ethylene is enhanced
in the presence of an oxide surface with a 450 fold increase in π»2 production in the
presence of πππ2 than in pure ethylene. Further research is required to elucidate a
mechanism for this phenomenon and to what extent SSA, oxide band gap and quantity of
adsorbed water may have on this system.
This experiment was initially performed to help determine the dose adsorbed by the gas
phase in contact with an oxide surface, however, it has suggested another topic of research
interest.
Chapter One outlined the packaging criteria for ππ’π2 from the two product streams at the
Sellafield site. Magnox ππ’π2 product is packaged in an aluminium can and placed inside a
polyethylene ( ππΈ ) bag. During long term storage these bags have thermally and
Chapter 10 Future Work 7131060
249
radiolytically degraded, leading to the formation of π»2, small gaseous hydrocarbons and
unsaturated polymeric hydrocarbons. Other gaseous hydrocarbons, for example, ethane
and butene should be investigated to assess the decomposition of hydrocarbons in the
presence of an oxide surface and how this may contribute to π»2 concentration in the ullage
space.
Alongside gaseous hydrocarbons, powdered ππΈ could be mixed in various ratios with an
oxide powder and irradiated. This experiment would help to determine if the physical form
of the hydrocarbon has an effect on decomposition.
10.4 Generic Recommendations
The following recommendations are not specific for either of the gaseous system
investigated in this project.
In this research, surrogates of ππ’π2 have been used to investigate the gas phase radiation
chemistry occurring in the presence of an oxide surface. Although πΆππ2 and πππ2 have
been used extensively as ππ’π2 surrogates, there may be better alternatives. Thorium
dioxide (πβπ2) and uranium dioxide (ππ2) both have the same fluorite structure as ππ’π2
and as actinide oxides may bear a closer resemblance to ππ’π2 than either πΆππ2 or πππ2.
Both of these oxides are radioactive and like ππ’π2 are Ξ±-emitters. This would simulate
ππ’π2 canisters better as they are internal radiation sources with alpha decay energies
similar to plutonium (4-4.6 MeV for thorium and uranium isotopes in comparison to 5.2-5.6
MeV for plutonium isotopes).
Chapter 10 Future Work 7131060
250
The final stage of this research programme would be to undertake studies with ππ’π2. Using
surrogate oxides gives a good knowledge basis for potential reaction mechanisms inside the
storage canisters, but this approach will never be able to fully simulate the real system. It is
possible to replicate the physical properties of ππ’π2 (SSA, crystal structure, adsorbed
species); however, it is impossible to simulate the damage (and impurities) induced by
radioactive decay. ππ’π2 may have a large quantity of defects in the crystal lattice which
may affect the gas phase chemistry which cannot be replicated in a facile way.
The use of the three actinide oxides detailed above requires specialist facilities with regards
to handling and safeguards. All this work could not be undertaken at the DCF due to
environmental licensing and current infrastructure. Some of this work would have to be
undertaken at NNLβs Central Laboratory located at the Sellafield site.
Throughout this research, the effects of adsorbed species (in particular water) have been
highlighted as having an effect on the gas phase radiation chemistry. To determine the full
extent of this effect it is necessary to investigate a βcleanβ surface where the identity and
quantity of adsorbates is known. This may be achieved by utilising a single crystal or thin
film of the relevant oxide. UHV conditions would be needed to undertake this research to
maintain the surface properties of the oxide. Similar work has been undertaken with, for
instance, titanium dioxide thin films [128] using low energy electrons as the radiation
source. Experiments utilising energetic electrons and accelerated ions as the radiation
sources are also feasible. In addition, it would also be possible to use an internal radiation
source such as the actinide dioxides described above.
Chapter 10 Future Work 7131060
251
10.5 Future Work with Accelerated Ions
Section 7.9 outlined experiments utilising ethylene gas as a validation method for the
absolute current measurements. Good agreement was achieved with both systems for a
range of currents and absorbed doses. The low density of ethylene should allow for several
ion types to be investigated with reasonable penetration into the sample. This will help to
determine if π»2 production from ethylene radiolysis is dependent on ion type.
As described in Section 7.10, investigations with the ion accelerator are at a preliminary
stage, however, there is good agreement with corresponding 60πΆπ data to suggest there is
no LET effect. More data and using different ion types should further cement this
hypothesis.
In the research presented in this thesis; only gaseous systems have been investigated using
the ion accelerator. Experiments of π»2 β π2 β π΄π gas in the presence of an oxide surface
using an ion accelerator will help to create a better simulation of the ππ’π2 canisters.
However, there are several difficulties to overcome with this experiment as the penetration
of the beam will be greatly reduced from several centimetres to several microns. The
majority of the beam will be absorbed by (the first few microns of) the oxide powder; this
small portion of oxide will be heated by the beam as oxides are poor thermal conductors
and this could lead to the oxide surface becoming annealed. Due to this fact, external
cooling of the sample may be needed and/ or agitation of the sample may have to be
considered.
The short range of the incoming ions in the solid may lead to very negligible energy being
deposited into the gas phase, therefore, making comparison with gamma studies presented
in this thesis may be difficult to attain.
Chapter 10 Future Work 7131060
252
Any solutions to this issue would require the reaction vessel in Figure 3.6 to be redesigned
as the ion beam would not penetrate very far into the vessel and radiation chemistry would
only likely occur in the first few millimetres of the sample. One solution is highlighted in
Figure 10.1. In this figure, the ion beam is stopped entirely in the gas phase, therefore there
would be no energy transferred from the oxide to the gas phase and the solid would act
simply as a sink for gaseous species.
Figure 10.1: Sketch of possible reaction vessel to study heterogeneous systems using an ion accelerator
An issue with this design is in keeping the oxide powder in position during irradiations. As
the powder would not play any part in the radiation chemistry mechanism, this design is a
poor simulation of the ππ’π2 canister system.
A second reaction vessel design is illustrated in Figure 10.2. In this design, the ion beam is
absorbed by both gas and solid phase allowing for potential energy transfer to take place.
This would simulate the ππ’π2 canister system better; however, the issue of oxide annealing
would still occur at the interface with the mica window.
Chapter 10 Future Work 7131060
253
Figure 10.2: Second possible reaction vessel for heterogeneous system experiments using an ion accelerator
This vessel would require secure placement and further beam diagnostics to help determine
the energy partitioning between the two phases.
This reaction vessel could be utilised in investigations of oxide powders in air atmospheres
as well as π»2 β π2 β π΄π studies.
Chapter 11 Bibliography 7131060
254
11 Bibliography
1. Sharrad, C.A., L.M. Harwood, and F.R. Livens, Chapter 2 Nuclear Fuel Cycles: Interfaces with
the Environment, in Nuclear Power and the Environment. 2011, The Royal Society of
Chemistry. p. 40-56.
2. Various, Plutonium Separation in Nuclear Power Programs, 2015.
3. Management of the UK's plutonium stocks: a consultation on the long-term management of
UK owned separated civil plutonium, 2011, Department of Energy and Climate Change. p. 12-
13.
4. Herbst, R.S., P. Baron, and M. Nilsson, 6 - Standard and advanced separation: PUREX
processes for nuclear fuel reprocessing, in Advanced Separation Techniques for Nuclear Fuel
Reprocessing and Radioactive Waste Treatment. 2011, Woodhead Publishing. p. 141-175.
5. Stabilization, Packaging, and Storage of Plutonium-Bearing Materials, D.o. Energy, Editor
2012.
6. Machuron-Mandard, X. and C. Madic, Plutonium dioxide particle properties as a function of
calcination temperature. Journal of Alloys and Compounds, 1996. 235(2): p. 216-224.
7. Cook, P., H.E. Sims, and D. Woodhead, Safe and Secure Storage of Plutonium Dioxide in the
United Kingdom. Actinide Research Quarterly, 2013(2): p. 20-25.
8. Orr, R.M., H.E. Sims, and R.J. Taylor, A review of plutonium oxalate decomposition reactions
and effects of decomposition temperature on the surface area of the plutonium dioxide
product. Journal of Nuclear Materials, 2015. 465: p. 756-773.
9. Sims, H.E., et al., Hydrogen yields from water on the surface of plutonium dioxide. Journal of
Nuclear Materials, 2013. 437(1-3): p. 359-364.
10. Gilchrist, P., Plutonium: Credible Options Analysis (Gate A), N.D. Authority, Editor 2010.
11. Choppin, G.R., J.O. Liljenzin, and J. Rydberg, Chapter 4 - Unstable Nuclei and Radioactive
Decay, in Radiochemistry and Nuclear Chemistry (Third Edition). 2002, Butterworth-
Heinemann: Woburn. p. 58-93.
12. Spinks, J.W.T. and R.J. Woods, An Introduction to Radiation Chemistry. 3rd ed. 1964: John
Wiley & Sons.
13. Choppin, G.R., J.O. Liljenzin, and J. Rydberg, Chapter 6 - Absorption of Nuclear Radiation, in
Radiochemistry and Nuclear Chemistry (Third Edition). 2002, Butterworth-Heinemann:
Woburn. p. 123-165.
14. Appleby, A. and H.A. Schwarz, Radical and molecular yields in water irradiated by gamma-
rays and heavy ions. The Journal of Physical Chemistry, 1969. 73(6): p. 1937-1941.
Chapter 11 Bibliography 7131060
255
15. Yang, K. and P.J. Manno, The Role of Free Radical Processes in the Ξ³-Radiolysis of Methane,
Ethane and Propane. Journal of the American Chemical Society, 1959. 81(14): p. 3507-3510.
16. Hauser, W.P., Radiolysis of Methane-C14 1. The Journal of Physical Chemistry, 1964. 68(6): p.
1576-1579.
17. Eller, P.G., R.E. Mason, and D.R. Horrell, 1999, Los Alamos Technical Report.
18. Ronchi, C. and J.P. Hiernaut, Helium diffusion in uranium and plutonium oxides. Journal of
Nuclear Materials, 2004. 325(1): p. 1-12.
19. Paffett, M. and G. Bailey, Gas Generation from Actinide Oxide Marterials, 1999: Los Alamos
Technical Report. p. 3-9.
20. Mason, R., T. Allen, and L. Morales, Gas Pressurization from Calcined Plutonium Oxides,
1999.
21. Almond, P.M., R.R. Livingston, and L.E. Traver, Gas Analyses from Headspace of Plutonium
Bearing Materials Containers, 2010: Savannah River National Laboratory.
22. Stakebake, J.L., Thermal desorption study of the surface interactions between water and
plutonium dioxide. The Journal of Physical Chemistry, 1973. 77(5): p. 581-586.
23. Haschke, J.M. and T.E. Ricketts, Adsorption of water on plutonium dioxide. Journal of Alloys
and Compounds, 1997. 252(1β2): p. 148-156.
24. Alexandrov, V., et al., Actinide Dioxides in Water: Interactions at the Interface. Journal of
Physical Chemistry Letters, 2011. 2(24): p. 3130-3134.
25. Petrik, N.G., A.B. Alexandrov, and A.I. Vall, Interfacial energy transfer during gamma
radiolysis of water on the surface of ZrO2 and some other oxides. Journal of Physical
Chemistry B, 2001. 105(25): p. 5935-5944.
26. Pastina, B., J.A. LaVerne, and S.M. Pimblott, Dependence of molecular hydrogen formation in
water on scavengers of the precursor to the hydrated electron. Journal of Physical Chemistry
A, 1999. 103(29): p. 5841-5846.
27. Luo, Y.R., Bond Dissociation Energies, in Handbook of Chemistry and Physics. 2009, CRC
Press. p. 9.64-9.69.
28. Aleksandrov, A.B., et al., Radiolysis of Adsorbed Substances on Oxide Surfaces. Zhurnal
Fizicheskoi Khimii, 1991. 65(6): p. 1604-1608.
29. LaVerne, J.A. and L. Tandon, H2 Production in the Radiolysis of Water on CeO2 and ZrO2. The
Journal of Physical Chemistry B, 2002. 106(2): p. 380-386.
30. Haschke, J.M., T.H. Allen, and L.A. Morales, Reactions of plutonium dioxide with water and
hydrogen-oxygen mixtures: Mechanisms for corrosion of uranium and plutonium. Journal of
Alloys and Compounds, 2001. 314(1-2): p. 78-91.
Chapter 11 Bibliography 7131060
256
31. Lloyd, J.A., Literature search on hydrogen/oxygen recombination and generation in
plutonium storage environments, 1999.
32. Haschke, J.M. and T.H. Allen, Interactions of Plutonium Dioxide with Water and Oxygen-
Hydrogen Mixtures, 1999.
33. Morales, L.A., Preliminary report on the recombination rates of hydrogen and oxygen over
pure and impure plutonium oxides, 1998.
34. Korzhavyi, P.A., et al., Oxidation of plutonium dioxide. Nature Materials, 2004. 3(4): p. 225-
228.
35. Quigley, G.P., Hydrogen/Oxygen Recombination Rates in 3013-Type Environments: An
Interim Report on the Rate of Loss of Hydrogen in Dry Air from Cell Containing Non-Radiolytic
Samples, 1998.
36. Katz, S., The Reaction of Hydrogen and Oxygen in the Presence of Concrete Incorporating
Simulated Radioactive Waste, 1979.
37. Lind, S.C., Chemical action produced by radium emanation I The combination of hydrogen
and oxygen. Journal of the American Chemical Society, 1919. 41: p. 531-551.
38. Schiflett, C.H. and S.C. Lind, The temperature coefficient of the rate of combination of
hydrogen and oxygen under alpha radiation. Journal of Physical Chemistry, 1934. 38(3): p.
327-337.
39. Lind, S.C. and C.H. Schiflett, Chemical action produced by alpha particles: The combination of
deuterium and oxygen. Journal of the American Chemical Society, 1935. 57(1): p. 1051-1052.
40. Benjamin, B.M. and H.S. Isbin, Recombination of Hydrogen and Oxygen in Presence of Water
Vapour under Influence of Radiation. Energia Nucleare, 1966. 13(4): p. 165-172.
41. Dautzenberg, D., Gamma-radiolysis of Hydrogen Oxygen Mixtures 1 Influences of
Temperature, Vessel Wall, Pressure and Added Gases (N2, AR, H2) on the Reactivity of
H2/O2-Mixtures. Radiation Physics and Chemistry, 1989. 33(1): p. 61-67.
42. Willis, C., A.W. Boyd, and M.J. Young, Radiolysis of air and nitrogenβoxygen mixtures with
intense electron pulses: determination of a mechanism by comparison of measured and
computed yields. Canadian Journal of Chemistry, 1970. 48(10): p. 1515-1525.
43. Harteck, P. and S. Dondes, Decomposition of Nitric Oxide and Nitrogen Dioxide by the Impact
of Fission Fragments of Uranium-235. The Journal of Chemical Physics, 1957. 27(2): p. 546-
551.
44. Harteck, P. and S. Dondes, The Kinetic Radiation Equilibrium of Air. The Journal of Physical
Chemistry, 1959. 63(6): p. 956-961.
Chapter 11 Bibliography 7131060
257
45. Kanda, Y., et al., Measurement of radiolytic yield of nitric acid in air. Radiation Physics and
Chemistry, 2005. 74(5): p. 338-340.
46. Jones, A.R., Radiation Induced Reactions in the N2-O2-H2O System. Radiation Research,
1959. 10(6): p. 655-663.
47. Rouessac, F. and A. Rouessac, Chemical Analysis - Modern Instrumentation Methods and
Techniques. 1994: John Wiley & Sons Ltd.
48. Webb, P.A. and C. Orr, Analytical Methods in Fine Particle Technology. 1997: Micromeritics
Instrument Corporation.
49. Finlayson-Pitts, B.J. and J.N. Pitts Jr, Chapter 7 - Chemistry of Inorganic Nitrogen Compounds,
in Chemistry of the Upper and Lower Atmosphere. 2000, Academic Press. p. 264-293.
50. Schuler, R.H. and A.O. Allen, Absolute Measurement of Cyclotron Beam Currents for
Radiation-Chemical Studies. Review of Scientific Instruments, 1955. 26(12): p. 1128-1130.
51. Ziegler, J.F. SRIM (Stopping Range of Ions in Matter). Available from: www.srim.org.
52. Charlesby, A., The Effects of Ionising Radiation on Polymers, in Irradiation Effects on
Polymers. 1991, Elsevier Science Publishers. p. 55-57.
53. Nilsson, S. and M. Jonsson, H2O2 and radiation induced dissolution of UO2 and SIMFUEL
pellets. Journal of Nuclear Materials, 2011. 410(1β3): p. 89-93.
54. Stone, J.A., Radiolysis of cyclohexane in a xenon matrix at 77 Β°K. Canadian Journal of
Chemistry, 1968. 46(8): p. 1267-1277.
55. Sagert, N.H. and R.W. Robinson, Radiolysis in the adsorbed state. II. N2O adsorbed on silica
gel and zirconia. Canadian Journal of Chemistry, 1968. 46(12): p. 2075-2080.
56. LaVerne, J.A. and L. Tandon, H2 Production in the Radiolysis of Water on UO2 and Other
Oxides. The Journal of Physical Chemistry B, 2003. 107(49): p. 13623-13628.
57. Armstrong, D.A., The Radiation Chemistry of Gases, in Radiation Chemistry Principles and
Applications. 1987, VCH Publishers inc. p. 263-319.
58. Johnson, G.R.A., The nitrous oxide radiation dosimeter. Journal of Inorganic and Nuclear
Chemistry, 1962. 24(5): p. 461-468.
59. McLaren, K.G., Gas phase dosimetry based on nitrogen yield from nitrous oxide. The
International Journal of Applied Radiation and Isotopes, 1974. 25(2): p. 87-93.
60. Janovsky, I., Use of Nitrous-Oxide and Ethylene for Gas-phase Dosimetry. International
Journal for Radiation Physics and Chemistry, 1976. 8(3): p. 396-397.
61. Ikezoe, Y., S. Sato, and A. Danno, Chemical Dosimeters for Mixed Radiations in a Nuclear
Reactor. Journal of Nuclear Science and Technology, 1971. 8(7): p. 394-399.
Chapter 11 Bibliography 7131060
258
62. Srinivas.S and W.E. Smith, Ethylene as a Dosimeter at high Pressures, Temperatures and
Dose Rates. International Journal of Applied Radiation and Isotopes, 1966. 17(11-1): p. 643-
647.
63. Leay, L., et al., Development of irradiation capabilities to address the challenges of the
nuclear industry. Nuclear Instruments and Methods in Physics Research Section B: Beam
Interactions with Materials and Atoms, 2015. 343(0): p. 62-69.
64. LaVerne, J.A. and R.H. Schuler, Radiation chemical studies with heavy ions: oxidation of
ferrous ion in the Fricke dosimeter. The Journal of Physical Chemistry, 1987. 91(22): p. 5770-
5776.
65. Brunauer, S., et al., On a Theory of the van der Waals Adsorption of Gases. Journal of the
American Chemical Society, 1940. 62(7): p. 1723-1732.
66. Socrates, G., Infrared and Raman Characteristic Group Frequencies. Third Edition ed. 2001:
John Wiley and Sons Ltd.
67. Busca, G. and V. Lorenzelli, Infrared spectroscopic identification of species arising from
reactive adsorption of carbon oxides on metal oxide surfaces. Materials Chemistry, 1982.
7(1): p. 89-126.
68. Baltrusaitis, J., et al., Carbon dioxide adsorption on oxide nanoparticle surfaces. Chemical
Engineering Journal, 2011. 170(2β3): p. 471-481.
69. Goodman, A.L., E.T. Bernard, and V.H. Grassian, Spectroscopic study of nitric acid and water
adsorption on oxide particles: Enhanced nitric acid uptake kinetics in the presence of
adsorbed water. Journal of Physical Chemistry A, 2001. 105(26): p. 6443-6457.
70. Sauer, M.C. and L.M. Dorfman, The Radiolysis of Ethylene: Details of the Formation of
Decomposition Products. The Journal of Physical Chemistry, 1962. 66(2): p. 322-325.
71. Ausloos, P. and R. Gorden, Hydrogen Formation in the Ξ³ Radiolysis of Ethylene. The Journal of
Chemical Physics, 1962. 36(1): p. 5-9.
72. Sauer, M.C. and L.M. Dorfman, Molecular Detachment Processes in the Vacuum uv Photolysis
of Gaseous Hydrocarbons. I. Ethylene. II. Butane. The Journal of Chemical Physics, 1961.
35(2): p. 497-502.
73. Meisels, G.G. and T.J. Sworski, Radiolysis of Ethylene. I. Yield of Hydrogen Atoms and
Formation of Saturated Hydrocarbons1. The Journal of Physical Chemistry, 1965. 69(3): p.
815-821.
74. Meisels, G.G., Radiolysis of Ethylene. II. Primary Free Radicals and Their Reactions1. Journal
of the American Chemical Society, 1965. 87(5): p. 950-957.
Chapter 11 Bibliography 7131060
259
75. Yang, K. and P.J. Manno, Gamma Radiolysis of Ethylene. Journal of Physical Chemistry, 1959.
63(5): p. 752-753.
76. Emeline, A., et al., Spectroscopic and photoluminescence studies of a wide band gap
insulating material: Powdered and colloidal ZrO2 sols. Langmuir, 1998. 14(18): p. 5011-5022.
77. Ren, Y., et al., Elastic properties and electronic structure of transition metal atoms in CeO2
solid solution: First principle studies. Computational Materials Science, 2015. 98: p. 459-465.
78. Chelnokov, E., et al., Electron Transfer at Oxide/Water Interfaces Induced by Ionizing
Radiation. Journal of Physical Chemistry C, 2014. 118(15): p. 7865-7873.
79. Haschke, J.M., T.H. Allen, and L.A. Morales, Reaction of plutonium dioxide with water:
Formation and properties of PuO2+x. Science, 2000. 287(5451): p. 285-287.
80. Penneman, R.A. and M.T. Paffett, An alternative structure of Pu4O9 ("PuO2.25")
incorporating interstitial hydroxyl rather than oxide. Journal of Solid State Chemistry, 2005.
178(2): p. 563-566.
81. Il Pae, Y., D.C. Shin, and J.R. Sohn, CeO2-Promoted highly active catalyst, NiSO4/CeO2-ZrO2
for ethylene dimerization. Bulletin of the Korean Chemical Society, 2006. 27(12): p. 1989-
1996.
82. Gray, L.H., An Ionization Method for the Absolute Measurement of Gamma Ray Energy.
Proceedings of the Royal Society of London A: Mathematical, Physical and Engineering
Sciences, 1936. 156(889): p. 578-596.
83. Attix, F.H., L.D. Vergne, and V.H. Ritz, Cavity Ionisation as a Function of Wall Material.
Journal of Research of the National Bureau of Standards, 1958. 60(3): p. 235-243.
84. Spencer, L.V. and F.H. Attix, A Theory of Cavity Ionization. Radiation Research, 1955. 3(3): p.
239-254.
85. Lias, S.G., Ionization Energies of Gas-Phase Molecules, in Handbook of Chemistry and Physics.
2009, CRC Press. p. 10.206-10.221.
86. Phelps, A.V., Collisions of H+, H2(+), H3(+), ARH+, H-, H, and H2 with AR and of AR+ and ARH+
with H2 for Energies from 0.1 EV to 10 KEV. Journal of Physical and Chemical Reference Data,
1992. 21(4): p. 883-897.
87. Kobayashi, N., Low Energy Ion-Netural Reactions. III. Ar++NO, Kr++NO, Ar++O2, Kr++O2 and
Ar++CO. Journal of the Physical Society of Japan, 1974. 36(1): p. 259-266.
88. Hasan, A.T., Single electron capture in slow collisions of H2+ ions with H2, O2 and N2
diatomic molecules. International Journal of Mass Spectrometry, 2005. 247(1β3): p. 81-84.
89. Willis, C. and A.W. Boyd, Excitation in the radiation chemistry of inorganic gases.
International Journal for Radiation Physics and Chemistry, 1976. 8(1β2): p. 71-111.
Chapter 11 Bibliography 7131060
260
90. Tully, J.C., Reactions of O(1D) with atmospheric molecules. The Journal of Chemical Physics,
1975. 62(5): p. 1893-1898.
91. Presser, N. and R.J. Gordon, The kinetic isotope effect in the reaction of O(3P) with H2, D2,
and HD. The Journal of Chemical Physics, 1985. 82(3): p. 1291-1297.
92. Lin, C.L. and M.T. Leu, Temperature and third-body dependence of the rate constant for the
reaction O + O2 + M β O3 + M. International Journal of Chemical Kinetics, 1982. 14(4): p.
417-434.
93. Kurzius, S.C. and M. Boudart, Kinetics of the branching step in the hydrogen-oxygen reaction.
Combustion and Flame, 1968. 12(5): p. 477-491.
94. Schulz, W.R. and D.J. Le Roy, Kinetics of the Reaction H+pH2 = oH2+H. The Journal of
Chemical Physics, 1965. 42(11): p. 3869-3873.
95. Campbell, I.M. and C.N. Gray, Rate constants for O(3P) recombination and association with
N(4S). Chemical Physics Letters, 1973. 18(4): p. 607-609.
96. Larkin, F.S. and B.A. Thrush, Recombination of hydrogen atoms in the presence of
atmospheric gases. Discussions of the Faraday Society, 1964. 37(0): p. 112-117.
97. Orkin, V.L., et al., Rate constant for the reaction of OH with H2 between 200 and 480 K.
Journal of Physical Chemistry A, 2006. 110(21): p. 6978-6985.
98. Lewis, R.S. and R.T. Watson, Temperature dependence of the reaction O(3P) + OH(2II) = O2 +
H. The Journal of Physical Chemistry, 1980. 84(26): p. 3495-3503.
99. Michael, J.V., et al., Rate Constants For H + O2 + M β HO2 + M in Seven Bath Gases. The
Journal of Physical Chemistry A, 2002. 106(21): p. 5297-5313.
100. Dobis, O. and S.W. Benson, Reaction of the ethyl radical with oxygen at millitorr pressures at
243-368 K and a study of the Cl + HO2, ethyl + HO2, and HO2 + HO2 reactions. Journal of the
American Chemical Society, 1993. 115(19): p. 8798-8809.
101. Vaghjiani, G.L., A.R. Ravishankara, and N. Cohen, Reactions of hydroxyl and hydroxyl-d with
hydrogen peroxide and hydrogen peroxide-d2. The Journal of Physical Chemistry, 1989.
93(23): p. 7833-7837.
102. Dubey, M.K., et al., Isotope specific kinetics of hydroxyl radical (OH) with water (H2O):
Testing models of reactivity and atmospheric fractionation. Journal of Physical Chemistry A,
1997. 101(8): p. 1494-1500.
103. Anderson, A.R. and J.V.F. Best, Use of Ethylene as a Gas Phase Dosimeter for Accelerator
Radiation. Nature, 1967. 216(5115): p. 576-577.
104. Housecroft, C.E. and A.G. Sharpe, Structures and Energetics of Metallic and Ionic Solids, in
Inorganic Chemistry. 2008, Pearson Education Limited. p. 164-171.
Chapter 11 Bibliography 7131060
261
105. Rodriguez, J.A., et al., Properties of CeO2 and Ce1-xZrxO2 Nanoparticles:β X-ray Absorption
Near-Edge Spectroscopy, Density Functional, and Time-Resolved X-ray Diffraction Studies.
The Journal of Physical Chemistry B, 2003. 107(15): p. 3535-3543.
106. Teufer, G., The crystal structure of tetragonal ZrO2. Acta Crystallographica, 1962. 15(11): p.
1187.
107. Lane, C.D., et al., Site-dependent electron-stimulated reactions in water films on TiO2(110).
The Journal of Chemical Physics, 2007. 127(22): p. 224706.
108. Reed, D.T. and R.A. Van Konynenburg, Effect of ionizing radiation on moist air systems, 1987.
109. Karasawa, H., et al., Radiation Induced Decomposition of Nitrogen. Radiation Physics and
Chemistry, 1991. 37(2): p. 193-197.
110. Tokunaga, O., et al., Radiation Treatment of Exhaust Gases 4 Oxidation of NO in Moist
Mixtures of O2 and N2. Radiation Physics and Chemistry, 1978. 11(3): p. 117-122.
111. Morris, E.D. and H. Niki, Reaction of dinitrogen pentoxide with water. The Journal of Physical
Chemistry, 1973. 77(16): p. 1929-1932.
112. Rodriguez, J.A., et al., Chemistry of NO2 on CeO2 and MgO: Experimental and theoretical
studies on the formation of NO3. Journal of Chemical Physics, 2000. 112(22): p. 9929-9939.
113. Nanayakkara, C.E., W.A. Larish, and V.H. Grassian, Titanium Dioxide Nanoparticle Surface
Reactivity with Atmospheric Gases, CO2, SO2, and NO2: Roles of Surface Hydroxyl Groups
and Adsorbed Water in the Formation and Stability of Adsorbed Products. The Journal of
Physical Chemistry C, 2014. 118(40): p. 23011-23021.
114. Hadjiivanov, K., et al., Infrared spectroscopy study of the species arising during nitrogen
dioxide adsorption on titania (anatase). Langmuir, 1994. 10(2): p. 464-471.
115. Haubrich, J., et al., In Situ Ambient Pressure Studies of the Chemistry of NO2 and Water on
Rutile TiO2(110). Langmuir, 2010. 26(4): p. 2445-2451.
116. Sorescu, D.C., C.N. Rusu, and J.T. Yates, Adsorption of NO on the TiO2(110) surface: An
experimental and theoretical study. Journal of Physical Chemistry B, 2000. 104(18): p. 4408-
4417.
117. Hadjiivanov, K.I., D.G. Klissurski, and V.P. Bushev, IR spectroscopic study of NO2 adsorption
on chromia. Journal of the Chemical Society, Faraday Transactions, 1995. 91(1): p. 149-153.
118. Ansari, S.A., et al., Band gap engineering of CeO2 nanostructure using an electrochemically
active biofilm for visible light applications. Rsc Advances, 2014. 4(32): p. 16782-16791.
119. Saliba, N.A., H. Yang, and B.J. Finlayson-Pitts, Reaction of Gaseous Nitric Oxide with Nitric
Acid on Silica Surfaces in the Presence of Water at Room Temperature. The Journal of
Physical Chemistry A, 2001. 105(45): p. 10339-10346.
Chapter 11 Bibliography 7131060
262
120. De Almeida, L., et al., Insights into the Thermal Decomposition of Lanthanide(III) and
Actinide(III) Oxalates β from Neodymium and Cerium to Plutonium. European Journal of
Inorganic Chemistry, 2012. 2012(31): p. 4986-4999.
121. AltaΕ, Y. and H. Tel, Structural and thermal investigations on cerium oxalate and derived
oxide powders for the preparation of (Th,Ce)O2 pellets. Journal of Nuclear Materials, 2001.
298(3): p. 316-320.
122. Moosath, S.S., J. Abraham, and T.V. Swaminathan, Thermal Decomposition of Rare Earth
Metal Oxalates 4 Oxalates of Cerium and Thorium. Zeitschrift Fur Anorganische Und
Allgemeine Chemie, 1963. 324(1-2): p. 103-105.
123. Hirschfelder, J.O. and H.S. Taylor, The Alpha-Particle Reactions in Carbon Monoxide, Oxygen
and Carbon Dioxide Systems. The Journal of Chemical Physics, 1938. 6(12): p. 783-790.
124. Arin, L.M. and P. Warneck, Reaction of ozone with carbon monoxide. The Journal of Physical
Chemistry, 1972. 76(11): p. 1514-1516.
125. Harteck, P. and S. Dondes, Decomposition of Carbon Dioxide by Ionizing Radiation. Part I. The
Journal of Chemical Physics, 1955. 23(5): p. 902-908.
126. Jennings, S.G., The mean free path in air. Journal of Aerosol Science, 1988. 19(2): p. 159-166.
127. Foy, B.R. and S.A. Joyce, Gas-phase Radiolysis in Plutonium Dioxide Powder, 2008, Los
Alamos National Laboratory.
128. Lane, C.D., et al., Electron-stimulated oxidation of thin water films adsorbed on TiO2(110).
Journal of Physical Chemistry C, 2007. 111(44): p. 16319-16329.
top related