density, volume, and packing: part 2 thursday, september 4, 2008 steve feller coe college physics...
TRANSCRIPT
![Page 1: Density, Volume, and Packing: Part 2 Thursday, September 4, 2008 Steve Feller Coe College Physics Department Lecture 3 of Glass Properties Course](https://reader036.vdocuments.us/reader036/viewer/2022070307/551aa95e550346b2288b45a2/html5/thumbnails/1.jpg)
Density, Volume, and Packing: Part 2
Thursday, September 4, 2008
Steve Feller
Coe College Physics Department
Lecture 3 of Glass Properties Course
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Some Definitions
• x = molar fraction of alkali or alkaline-earth oxide (or any modifying oxide)
• 1-x = molar fraction of glass former
• R = x/(1-x) This is the compositional parameter of choice in developing structural models for borates.
• J = x/(1-x) for silicates and germanates
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Short Ranges B and Si StructuresShort-range borate units,
Fi unit Structure R value
F1 trigonal boron with three bridging oxygen 0·0
F2 tetrahedral boron with four bridging oxygen 1·0
F3 trigonal boron with two bridging oxygen (one NBO) 1·0
F4 trigonal boron with one bridging oxygen (two NBOs) 2·0
F5 trigonal boron with no bridging oxygen (three NBOs) 3·0
Short-range silicate units,
Qi unit Structure J value
Q4 tetrahedral silica with four bridging oxygen 0·0
Q3 tetrahedral silica with three bridging oxygen (one NBO) 0·5
Q2 tetrahedral silica with two bridging oxygen (two NBOs) 1·0
Q1 tetrahedral silica with one bridging oxygen (three NBOs) 1·5
Q0 tetrahedral silica with no bridging oxygen (four NBOs) 2·0
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Lever Rule Model for Silicates1.0
0.8
0.6
0.4
0.2
0.0
Fra
ction o
f Q
-Unit
2.01.51.00.50.0J-Value
Q4
Q3
Q2
Q1
Q0
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2.36
2.34
2.32
2.30
2.28
2.26
2.24
2.22
Den
sity
(g/c
c)
2.01.51.00.50.0J-Value
Model Peters et al. Literature Compilation
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Method of Least Squares
• Take (ρmod – ρexp)2 for each data point
• Add up all terms
• Vary volumes until a least sum is found.
• Volumes include empty space.
• ρmod = M/(fiVi)
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Example: Li-Silicates
• VQ4 = 1.00
• VQ3 = 1.17
• VQ2 = 1.41
• VQ1 = 1.69
• VQ0 = 1.95
• VQ4(J = 0) defined to be 1.
• The J = 0 glass is silicon dioxide with density of 2.205 g/cc
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4.5
4.0
3.5
3.0
2.5
2.0
Den
sity
(g/c
c)
2.01.51.00.50.0R-Value
Li Na K Rb Cs Mg Ca Sr Ba
Figure 1
Borate Glasses
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Borate Structural Model
• R < 0.5
• F1 = 1-R, F2 = R
• 0.5 <R <1.0
• F1 = 1-R, F2 = -(1/3)R +2/3, F3 = +(4/3)R -2/3
• 1.0 <R < 2.0
• F2 = -(1/3)R +2/3, F3 = -(2/3)R +4/3 , F4 = R-1
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Another Example: Li-Borates
• V1 = 0.98
• V2 = 0.91
• V3 = 1.37
• V4 = 1.66
• V5 = 1.95
• V1(R = 0) is defined to be 1.
• The R = 0 glass is boron oxide with density of 1.823 g/cc
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Barium Calcium
Vf1
0·96 0·99V f2
1·16 0·96V f3
1·54 1·29V f4
2·16 1·68VQ4
1·44 1·43VQ3
1.92 1.72VQ2
2.54 2.09
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Li and Ca Silicates
• Li Ca
• VQ4 = 1.00 VQ4 = 1.00
• VQ3 = 1.17 VQ3 = 1.20
• VQ2 = 1.41 VQ2 = 1.46
• VQ4(J = 0) defined to be 1.
• The J = 0 glass is silicon dioxide with density of 2.205 g/cc
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Silicates
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Densities of Barium Borate Glasses• R = x/(1-x) Density (g/cc)• 0·0 1·82• 0·2 2·68• 0·2 2·66• 0·4 3·35• 0·4 3·29• 0·6 3·71• 0·6 3·68• 0·8 3·95• 0·8 3·90• 0·9 4·09• 1·2 4·22• 1·3 4·31• 1·5 4·40• 1·7 4·50• 2·0 4·53
Use these data and the borate model to find the four borate volumes. Note this model might not yield exactly the volumes given before.
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• Volumes and packing fractions of borate short-range order groups. The volumes are reported relative to the volume of the BO1.5 unit in B2O3 glass. Packing fractions were determined from the density derived volumes and Shannon radii[i],[ii].
• System Unit Least Squares Volumes Packing Fraction•• Li f1 0.98 0.34• f2 0.94 0.65• f3 1.28 0.39• f4 1.61 0.41
• Na f1 0.95 0.35• f2 1.24 0.62• f3 1.58 0.41• f4 2.12 0.46
• K f1 0.95 0.35• f2 1.66 0.69• f3 1.99 0.52• f4 2.95 0.59
• Rb f1 0.98 0.34• f2 1.92 0.67• f3 2.27 0.52• f4 3.41 0.59
• Cs f1 0.97 0.34• f2 2.28 0.67• f3 2.62 0.54• f4 4.13 0.61•
[i] Barsoum, Michael, Fundamentals of Ceramics (McGraw-Hill: Columbus OH,1997), 85-89.• [ii] R.D. Shannon, Acta. Crystallogr., A32 (1976), 751.
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• System Unit Least Squares Volumes Packing Fraction• Mg f1 0.98 0.34• f2 0.95 0.63• f3 1.26 0.39• f4 1.46 0.44
• Ca f1 0.98 0.34• f2 0.95 0.71• f3 1.28 0.44• f4 1.66 0.48
• Sr f1 0.94 0.36• f2 1.08 0.68• f3 1.41 0.45• f4 1.92 0.48
• Ba f1 0.97 0.35• f2 1.13 0.73• f3 1.55 0.47• f4 2.16 0.51
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• Volumes and packing fractions of silicates short-range order groups. The volumes are reported relative to the volume of the Q4 unit in SiO2 glass. Packing fractions were determined from the density derived volumes and Shannon radii4,23.
• System Unit Least Squares Volumes Packing Fraction•• Li Q4 1.00 0.33• Q3 1.17 0.38• Q2 1.41 0.41• Q1 1.67 0.42• Q0 1.92 0.43
• Na Q4 1.00 0.33• Q3 1.34 0.42• Q2 1.74 0.46• Q1 2.17 0.48• Q0 2.63 0.49
• K Q4 0.99 0.33• Q3 1.58 0.52• Q2 2.27 0.58• Q1 2.97 0.61•
• Rb Q4 1.00 0.33• Q3 1.72 0.53• Q2 2.63 0.57• Q1 3.53 0.59
• Cs Q4 0.98 0.33• Q3 1.96 0.56• Q2 2.90 0.64• Q1 4.25 0.62
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Alkali Thioborates
• Data from Prof. Steve Martin
• x M2S.(1-x)B2S3 glasses
• Unusual F2 behavior
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Alkali Thioborate data
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• Volumes and packing fractions of thioborate short-range order groups. The volumes are reported relative to the volume of the BS1.5 unit in B2S3 glass.
• System Unit Least Squares Volumes Corresponding Oxide Volume• (compared with volume of
BO1.5 unit in B2O3 glass.)• __________________________ • Na f1 1.00 0.95• f2 1.37 1.24• f3 1.51 1.58• f5 2.95 2.66*
• K f1 1.00 0.95• f2 1.65 1.66• f3 1.78 1.99• f5 3.53 3.91*
• Rb f1 1.00 0.98• f2 1.79 1.92• f3 1.97 2.27• f5 3.90 4.55*
• Cs f1 1.00 0.97• f2 1.83 2.28• f3 2.14 2.62• f5 4.46 5.64*• *extrapolated
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Molar Volume
• Molar Volume = Molar Mass/density
It is the volume per mole glass.
It eliminates mass from the density and uses equal number of particles for comparison purposes.
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4.5
4.0
3.5
3.0
2.5
2.0
Den
sity
(g/c
c)
2.01.51.00.50.0R-Value
Li Na K Rb Cs Mg Ca Sr Ba
Figure 1
Borate Glasses
![Page 23: Density, Volume, and Packing: Part 2 Thursday, September 4, 2008 Steve Feller Coe College Physics Department Lecture 3 of Glass Properties Course](https://reader036.vdocuments.us/reader036/viewer/2022070307/551aa95e550346b2288b45a2/html5/thumbnails/23.jpg)
55
50
45
40
35
30
25
20
Mol
ar V
olum
e
3.53.02.52.01.51.00.50.0R-Value
Lithium Sodium Potassium Rubidium Cesium Magnesium Calcium Strontium Barium
Borate Glasses
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45
40
35
30
25
Mol
ar V
olum
e (c
c/m
ol)
0.60.50.40.30.20.10.0
R
Li Na K Rb Cs
Borate GlassesKodama Data
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Problem:
• Calculate the molar volumes of the barium borates given before. You will need atomic masses. Also, remember that the data are given in terms of R and there are R+1 moles of glassy materials. You could also use x to do the calculation.
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Li-Vanadate (yellow) Molar Volumes campared with Li-
Phosphates (black)
35
40
45
50
55
60
65
0 0.5 1 1.5
R
Mo
lar
Vo
lum
e (
cc
/mo
le)
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Molar volumes of Alkali Borate Glasses
26
28
30
32
34
36
38
40
42
44
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7
R
Mo
lar
Vo
lum
e (
cc/m
ol)
Top to bottom: Li, Na, K, Rb, Cs
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Stiffness vs R in Alkali Borate Glasses
5
10
15
20
25
30
35
0 0.2 0.4 0.6
R
Sti
ffn
ess
(G
Pa
)
Top to bottom: Li, Na, K, Rb, Cs
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30
25
20
15
10
Stif
fne
ss (
GP
a)
4240383634323028
Molar Volume (cc/mol)
Li Na K Rb Cs
Stiffness of Borates vs Molar Volume
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Stiffness vs Molar Volume -Cs
579
1113
37 38 39 40 41 42 43
Molar Volume (cc/mol)
Stiff
ness
(GPa
)
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Rb and Cs Stiffness using Cs Volumes
6789
101112131415
36 38 40 42
Molar Volume (cc/mol)
Sti
ffn
ess
, G
(G
Pa
)
Rb -purple squaresCs -yellow triangles
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Stiffness vs normalized Cs molar volume
5
10
15
37 38 39 40 41 42 43
molar volume (cc/mol)
Stif
fne
ss (
cc/m
ol)
K- open circles Rb -purple squaresCs -yellow triangles
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Differential Changes in Unit Volumes
• To begin the calculation, we define the glass density in terms of its dimensionless mass relative to pure borate glass (R=0), m′(R), and its dimensionless volume relative to pure borate glass, v′(R):
),0()(
)(')('
),0()('
)('
)(
)()(
R
RmRv
Rv
Rm
Rv
RmR
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Implies:
,)()()('
)()()('
2221212
2121111
vRfvRfRv
vRfvRfRv
).0()(
)(')()(
)0()(
)(')()(
2
2222121
1
1212111
R
RmvRfvRf
R
RmvRfvRf
![Page 35: Density, Volume, and Packing: Part 2 Thursday, September 4, 2008 Steve Feller Coe College Physics Department Lecture 3 of Glass Properties Course](https://reader036.vdocuments.us/reader036/viewer/2022070307/551aa95e550346b2288b45a2/html5/thumbnails/35.jpg)
• Solve for v1 and v2 simultaneously and assign it to R = (R1 +R2)/2
• This is accurate if R1 and R2 are close to each other; in Kodama’s data this condition is met.
).0()(
)(')()(
)0()(
)(')()(
2
2222121
1
1212111
R
RmvRfvRf
R
RmvRfvRf
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Relative Volumes of the f2 Unit
0.50
1.00
1.50
2.00
2.50
0.00 0.10 0.20 0.30 0.40
R
Rela
tive
Volu
me
Cs
Rb
K
Na
Li
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Volume of f1 and f2 Units of Rb and Cs (Extended to R = 0.6)
26
32
38
44
50
56
62
68
74
80
0.0 0.1 0.2 0.3 0.4 0.5 0.6
R (Ratio of Alkali Oxide to Boron Oxide)
Vol
ume
(in Å
3 )
f1 Units
f2 Units
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Relative Volumes of the f1 Unit
0.90
0.95
1.00
1.05
1.10
0.00 0.10 0.20 0.30 0.40R
Rela
tive
Volu
me
Cs
Rb
K
Na
Li
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Relative Volumes of the f1 & f2 Units of Ba-B and Na-B
0.75
0.85
0.95
1.05
1.15
1.25
1.35
1.45
0.00 0.10 0.20 0.30 0.40 0.50 0.60
R
Rela
tive
Volu
me f1-Ba
f2-Ba
f1-Na
f2-Na
f2-Unit
f1-Unit
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The Volume per Mole Glass Former
• Volume per mole glass former = Mass (JM2O.SiO2)/density
It is the volume per mole glass former and R moles of modifier.
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Volume per Mol Silica of Lithium Silicates using Bansaal and Doremus
27
29
31
33
35
37
0 0.2 0.4 0.6 0.8 1
J
Vo
lum
e p
er M
ol
Sil
ica
(cc/
mo
l)
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The Volume per Mole Glass Former
• Why is there a trend linear?
• JM2O.SiO2 (1-2J)Q4 +2JQ3 J<0.5
• So slope of volume curve is the additional volume needed to form Q3 at the expense of Q4. This is proportional to J.
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Differential Volume by J for JLi2O-SiO2 Glasses
8
9
10
11
12
13
14
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9
J Average
dV/dJ
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Lead Silicate System: Bansaal and Doremus Data
Differential Volume by JPb Average
12
14
16
18
20
22
24
26
28
0 0.5 1 1.5 2 2.5 3
J Average
Vol
ume(
cc/m
ol/J
)
![Page 45: Density, Volume, and Packing: Part 2 Thursday, September 4, 2008 Steve Feller Coe College Physics Department Lecture 3 of Glass Properties Course](https://reader036.vdocuments.us/reader036/viewer/2022070307/551aa95e550346b2288b45a2/html5/thumbnails/45.jpg)
Sodium Borogermanates Volumes per Mol B2O3 Compared to Sodium
Borosilicates180
160
140
120
100
80
60
40
20
V B
2O3
(cc/
mo
l)
3.53.02.52.01.51.00.50.0
R
Si, K=0.5 Si, K=1 Si, K=2 Si, K=4 Ge, K=0.5 Ge, K=1 Ge, K=2 Ge, K=4 Na2O*B2O3
![Page 46: Density, Volume, and Packing: Part 2 Thursday, September 4, 2008 Steve Feller Coe College Physics Department Lecture 3 of Glass Properties Course](https://reader036.vdocuments.us/reader036/viewer/2022070307/551aa95e550346b2288b45a2/html5/thumbnails/46.jpg)
25
30
35
40
0 0.2 0.4
J or R
Volu
me
per
mo
le g
lass
fo
rmer
(cc
/mo
l)
LiGe
LiSi
LiB
![Page 47: Density, Volume, and Packing: Part 2 Thursday, September 4, 2008 Steve Feller Coe College Physics Department Lecture 3 of Glass Properties Course](https://reader036.vdocuments.us/reader036/viewer/2022070307/551aa95e550346b2288b45a2/html5/thumbnails/47.jpg)
Problem
• For the barium borate data provided earlier plot the volume per mol boron oxide as a function of R.
• How do you interpret the result?
Lecture 2 ends here
![Page 48: Density, Volume, and Packing: Part 2 Thursday, September 4, 2008 Steve Feller Coe College Physics Department Lecture 3 of Glass Properties Course](https://reader036.vdocuments.us/reader036/viewer/2022070307/551aa95e550346b2288b45a2/html5/thumbnails/48.jpg)
Packing in Glass
• We will now examine the packing fractions obtained in glasses. This will provide a dimensionless parameter that displays some universal trends.
• We will need a good knowledge of the ionic radii. This will be provided next.
f
ii
V
Nrpf
3
3
4