n co at 273 k - science 4 clean energyscience4cleanenergy.eu/.../2019/09/s4ce_poster_jh.pdf · •...

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ρ max agrees well with the liquid densities of CO 2 and CH 4 : 26.78 mol/L (CO 2 t.p.) and 26.33 mol/L (CH 4 b.p.) However, the adsorbed phase densities differ from liquid densities → agree well with GCMC results Uptake of supercritical CO 2 and CH 4 on illite-smectite clay minerals Junyoung Hwang 1 and Ronny Pini 1 1 Department of Chemical Engineering, Imperial College London Adsorption of CO 2 and hydrocarbon gases is a key mechanism in geological CO 2 storage that leads to enhanced production of oil/gas. Clay minerals are major components of cap rocks and reservoir formations, such as sandstones, mudstones, and shales. Experimental sorption of CO 2 and CH 4 on illite-smectite clay minerals – smectite (SWy-2), I-S mixed (ISCz-1), and illite (IMt-2) – measured using a gravimetric balance (up to 30 MPa) are presented at multiple temperatures (25 to 115°C). The LDFT theory models adsorption based on fluid and adsorbent properties. Figure 2. Supercritical adsorption (closed symbols) and desorption (open symbols) of CO 2 and CH 4 on smectite, I-S mixed, and illite up to 30 MPa at 25, 50, 80, and 115 °C. The solid lines are the LDFT model fits. The textural properties of three illite-smectite clay minerals were thoroughly characterized using N 2 , Ar, and CO 2 Sorption of CO 2 and CH 4 on the three clays were measured under subsurface conditions, and described using the LDFT model [1] S. L. Montgomery et al. AAPG Bulletin 89 (2005) 155-175 [2] B. Song et al. SPE 140555 (2011) [3] F. L. Lynch Clays and Clay Minerals 45 (1997) 618-631 [4] A. Busch et al. Int. J. Greenh. Gas Control 2 (2008) 297-308 Results Concluding Remarks Modelling Adsorption: Lattice DFT for Slit Pores + V + V Δ − Δ = 0 Statistical thermodynamics framework that involves discretised pores [6] Thermodynamic Equilibrium: · · · · · · · · · · · · · · · w 1 2 3 · · · J Figure 1. Adsorption (closed symbols) and desorption (open symbols) isotherms of N 2 (77 K), Ar (87 K), and CO 2 (273 K) Fluid ρ max ρ GCMC [8] ρ Smectite ρ I-S mix ρ Illite [mol/L] [mol/L] [mol/L] [mol/L] [mol/L] CO 2 25.72 25.53 22.09 20.52 21.35 CH 4 26.45 17.42 15.26 15.26 15.09 Adsorbed phase densities estimated from first two layers at 150 bar and 60 °C Pore space not completely saturated beyond T c Accounts for temperature dependent variability of density Introduction and Background Adsorption in clay nanopores contributes to: 1. Liquid-like dense phase leading to increased gas storage capacity 2. Enhanced sealing efficiency 3. Determines the amount of Gas-In-Place (GIP) approx. 20-85 % [1] [2] Why clay minerals? Approximately 30 % of all sedimentary rocks [3] Found in shales and oil sands up to 90 % [4] Determines physical characteristics of subsurface formations Characterized by micro- and mesoporosity [5] O ccupancy profiles in slit pores (CO 2 at 50 °C) LDFT ex = sat =1 pore, =1 c , max , b c , max , b HP sorption isotherms Lattice DFT V pore PSD Pore-size dependent adsorption mechanisms are shown by the model Occupancy profiles → density profiles Multiple pores of different sizes Important for naturally occurring geosorbents with broad porosities Clay mineral porosities are characterized through low-pressure adsorption isotherms of multiple gases under cryogenic temperatures (Quantachrome Autosorb iQ) High-pressure sorption isotherms are measured using a magnetic suspension balance (Rubotherm IsoSORP HP II) that also measures the bulk densities in situ Experimental methods N 2 , Ar, and CO 2 sorption isotherms Total pore volume (≤ 0.110 cm 3 /g): smectite > I-S > illite Surface area positively correlated to pore volume Dominated by mesoporosity (≈ 50-60 %) Contain microporosity (≈ 10 %): smectite > illite > I-S CO 2 and CH 4 high-pressure sorption isotherms Uptake capacity: smectite ≈ I-S mixed >> Illite Illite shows significant hysteresis loops under supercritical conditions for both CO 2 and CH 4 Interlayer trapping? – Independent study showed scCO 2 trapping within illite layers [7] 10 -6 10 -5 10 -4 10 -3 10 -2 0.1 1 10 Q [cm 3 STP/g] P/P o N 2 Ar CO 2 and CH 4 in Clay Nanopores ρ max corresponds to complete filling of the lattice at saturation Figure 3. Saturation factors plotted against T c /T 0.0 0.2 0.4 0.6 0.8 1.0 1 10 100 0.0 0.2 0.4 0.6 0.8 1.0 1 10 100 0.00 0.01 0.02 0.03 0 1 2 3 Smectite I-S mixed Illite Adsorbed volume, Q [cm 3 STP/g] Relative pressure, P/P o [-] N 2 at 77 K Ar at 87 K Smectite I-S mixed Illite Relative pressure, P/P o [-] I-S mixed Illite CO 2 at 273 K Smectite Relative pressure, P/P o [-] 0 5 10 15 20 0 100 200 300 400 0 5 10 15 20 0 100 200 300 400 0 5 10 15 20 0 100 200 300 400 Bulk density, b [mol/L] CH 4 CO 2 Excess amount, n ex [mol/g] Smectite Bulk density, b [mol/L] CH 4 CO 2 I-S mixed CH 4 CO 2 Illite Bulk density, b [mol/L] 1 2 3 4 5 6 7 8 9 10 11 12 1 2 3 0.0 0.2 0.4 0.6 0.8 1.0 b = 0.8 b = 0.5 J b = 0.2 Lattice occupancy, J 0.4 0.5 0.6 0.7 0.8 0.9 1.0 0.2 0.4 0.6 0.8 1.0 1.2 Smectite I-S mixed Illite CH 4 Saturation factor, c sat [-] Reciprocal of reduced temperature, T c /T [-] CO 2 Common temperature correlation found for both CO 2 and CH 4 for all clays [5] E. Ilton et al. Environ. Sci. Technol. 46 (2012) 4241-4248 [6] G. Aranovich and M. Donohue J. Colloid Interface Sci. 180 (1996) 537-541 [7] J. Wan et al. Proc. Natl. Acad. Sci. U.S.A 118 (2018) 873-878 [8] H. Zhao, T. Wu, A. Firoozabadi, Fuel 224 (2018) 412-423 c sat approaches unity near crit. temp. → pore saturation Figure 4. Lattice occupancy profiles at different densities for pores of varying sizes 0 5 10 15 20 0 100 200 300 400 0.0 0.3 0.6 0.9 0.0 0.3 0.6 0.9 0 5 10 15 20 25 30 0.0 0.3 0.6 0.9 Excess amount, n ex [mol/g] Bulk density, b [mol/L] CO 2 on Smectite at 50 °C b = 2.5 mol/L b = 5.8 mol/L Lattice occupancy, b = 9.5 mol/L Lattice layer, J This project has received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement No 764810

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Page 1: N CO at 273 K - Science 4 Clean Energyscience4cleanenergy.eu/.../2019/09/S4CE_Poster_JH.pdf · • ρ max agrees well with the liquid densities of CO 2 and CH 4: 26.78 mol/L (CO 2

• ρmax agrees well with the liquid densities of CO2 and CH4: 26.78 mol/L (CO2 t.p.) and 26.33 mol/L (CH4 b.p.)

• However, the adsorbed phase densities differ from liquid densities → agree well with GCMC results

Uptake of supercritical CO2 and CH4 on illite-smectite clay mineralsJunyoung Hwang1 and Ronny Pini1 1Department of Chemical Engineering, Imperial College London

Adsorption of CO2 and hydrocarbon gases is a key mechanism in geological CO2 storage that leads to enhanced production of oil/gas.

Clay minerals are major components of cap rocks and reservoir formations, such as sandstones, mudstones, and shales.

Experimental sorption of CO2 and CH4 on illite-smectite clay minerals – smectite (SWy-2), I-S mixed (ISCz-1), and illite (IMt-2) – measured using a gravimetric balance (up to 30 MPa) are presented at multiple temperatures (25 to 115°C).

The LDFT theory models adsorption based on fluid and adsorbent properties.

Figure 2. Supercritical adsorption (closed symbols) and desorption (open symbols) of CO2 and CH4 on smectite, I-Smixed, and illite up to 30 MPa at 25, 50, 80, and 115 °C. The solid lines are the LDFT model fits.

• The textural properties of three illite-smectite clay minerals were thoroughly characterized using N2, Ar, and CO2

• Sorption of CO2 and CH4 on the three clays were measured under subsurface conditions, and described using the LDFT model

[1] S. L. Montgomery et al. AAPG Bulletin 89 (2005) 155-175[2] B. Song et al. SPE 140555 (2011)[3] F. L. Lynch Clays and Clay Minerals 45 (1997) 618-631[4] A. Busch et al. Int. J. Greenh. Gas Control 2 (2008) 297-308

Results

Concluding Remarks

Modelling Adsorption: Lattice DFT for Slit Pores

𝐿𝑗 + 𝐵V ⇌ 𝐵𝑗 + 𝐿V

Δ𝐻 − 𝑇Δ𝑆 = 0

Statistical thermodynamics framework that involves discretised pores[6]

Thermodynamic Equilibrium:· · ·· · ·· · ·

· · ·· · ·

w

1 2 3 · · · J

Figure 1. Adsorption (closed symbols) and desorption (open symbols) isotherms of N2 (77 K), Ar (87 K), and CO2 (273 K)

Fluidρmax ρGCMC

[8] ρSmectite ρI-S mix ρIllite

[mol/L] [mol/L] [mol/L] [mol/L] [mol/L]

CO2 25.72 25.53 22.09 20.52 21.35

CH4 26.45 17.42 15.26 15.26 15.09

Adsorbed phase densities estimated from first two layers at 150 bar and 60 °C

• Pore space not completely saturated beyond Tc

• Accounts for temperature dependent variability of density

Introduction and BackgroundAdsorption in clay nanopores contributes to:1. Liquid-like dense phase leading to increased gas storage capacity2. Enhanced sealing efficiency3. Determines the amount of Gas-In-Place (GIP) approx. 20-85 %[1]

[2]

Why clay minerals?• Approximately 30 % of all sedimentary rocks[3]

• Found in shales and oil sands up to 90 %[4]

• Determines physical characteristics of subsurface formations

• Characterized by micro- and mesoporosity

[5]

Occupancy profiles in slit pores (CO2 at 50 °C)

𝑛LDFTex = 𝑐sat

𝑘=1

𝐾𝑣pore,𝑘

𝐽𝑘

𝑗=1

𝐽

𝜌𝑗 𝜌c, 𝜌max, 𝜃𝑗 − 𝜌b 𝜌c, 𝜌max, 𝜃b

HP sorption isotherms

LatticeDFT

Vpore

PSD

• Pore-size dependent adsorption mechanisms are shown by the model

• Occupancy profiles → density profiles

• Multiple pores of different sizes

• Important for naturally occurring geosorbents with broad porosities

• Clay mineral porosities are characterized through low-pressure adsorption isotherms of multiple gases under cryogenic temperatures (Quantachrome Autosorb iQ)

• High-pressure sorption isotherms are measured using a magnetic suspension balance (Rubotherm IsoSORP HP II) that also measures the bulk densities in situ

Experimental methods

N2, Ar, and CO2 sorption isotherms

• Total pore volume (≤ 0.110 cm3/g): smectite > I-S > illite

• Surface area positively correlated to pore volume

• Dominated by mesoporosity (≈ 50-60 %)

• Contain microporosity (≈ 10 %): smectite > illite > I-S

CO2 and CH4 high-pressure sorption isotherms

• Uptake capacity: smectite ≈ I-S mixed >> Illite

• Illite shows significant hysteresis loops under supercritical conditions for both CO2 and CH4

• Interlayer trapping? – Independent study showed scCO2 trapping within illite layers[7]

10-6 10-5 10-4 10-3 10-2

0.1

1

10

Q [

cm3 S

TP/g

]

P/Po

N2

Ar

CO2 and CH4 in Clay Nanopores

• ρmax corresponds to complete filling of the lattice at saturation

Figure 3. Saturation factors plotted against Tc/T

0.0 0.2 0.4 0.6 0.8 1.0

1

10

100

0.0 0.2 0.4 0.6 0.8 1.0

1

10

100

0.00 0.01 0.02 0.030

1

2

3

Smectite

I-S mixed

Illite

Ad

sorb

ed v

olu

me,

Q [

cm3 S

TP/g

]

Relative pressure, P/Po [-]

N2 at 77 K Ar at 87 K

Smectite

I-S mixed

Illite

Relative pressure, P/Po [-]

I-S mixed

Illite

CO2 at 273 K

Smectite

Relative pressure, P/Po [-]

0 5 10 15 200

100

200

300

400

0 5 10 15 200

100

200

300

400

0 5 10 15 200

100

200

300

400

Bulk density, b [mol/L]

CH4

CO2

Exce

ss a

mo

un

t, n

ex [

mo

l/g] Smectite

Bulk density, b [mol/L]

CH4

CO2

I-S mixed

CH4

CO2

Illite

Bulk density, b [mol/L]

1 2 3 4 5 6 7 8 9 10 11 121 2 30.0

0.2

0.4

0.6

0.8

1.0

b = 0.8

b = 0.5

J

b = 0.2La

ttic

e o

ccu

pan

cy,

J

0.4 0.5 0.6 0.7 0.8 0.9 1.00.2

0.4

0.6

0.8

1.0

1.2Smectite

I-S mixed

Illite

CH4

Satu

rati

on

fac

tor,

csa

t [-]

Reciprocal of reduced temperature, Tc/T [-]

CO2 Common temperature correlation found for both CO2 and CH4 for all clays

[5] E. Ilton et al. Environ. Sci. Technol. 46 (2012) 4241-4248[6] G. Aranovich and M. Donohue J. Colloid Interface Sci. 180 (1996) 537-541[7] J. Wan et al. Proc. Natl. Acad. Sci. U.S.A 118 (2018) 873-878[8] H. Zhao, T. Wu, A. Firoozabadi, Fuel 224 (2018) 412-423

csat approaches unity near crit. temp. → pore saturation

Figure 4. Lattice occupancy profiles at different densities for pores of varying sizes

0 5 10 15 200

100

200

300

400

0.00.30.60.9

0.00.30.60.9

0 5 10 15 20 25 300.00.30.60.9

Exce

ss a

mo

un

t, n

ex [

mo

l/g]

Bulk density, b [mol/L]

CO2 on Smectite at 50 °C b = 2.5 mol/L

b = 5.8 mol/L

Latt

ice

occ

up

ancy

,

b = 9.5 mol/L

Lattice layer, J

This project has received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement No 764810