Computational Modelling — Microscopic Origin of Electrochemical Capacitance in Metal-Organic Frameworks

Measurement evidence

Computational Modelling

Microscopic Origin of Electrochemical Capacitance in Metal-Organic Frameworks · Shin S.-J., Gittins J.W., Golomb M.J. et al. · Journal of the American Chemical Society · 2023 · 14529-14538

6 measurement groups · 38 results

Reported values remain attached to the sample, method, conditions, extraction quality and source location that produced them.

Mean squared displacement analysis of electrolyte self-diffusion

Cu3(HITP)2 QM/MM electrochemical interface model · Model

MSD of acetonitrile and ions at point of zero charge in Cu3(HITP)2 pores compared with Cu3(HHTP)2 pores and bulk electrolyte.

Temperature
300
Atmosphere
computational
Geometry
hexagonal pore model
Context
model pristine frameworks with electrolyte
Measurement source
14534 · Modulating the EDL Structure with MOF Composition · Supplementary Figures 32-33
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Anisotropy of in-pore electrolyte self-diffusionparallel to hexagonal pores is two times larger than perpendicular to the poresText
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Supplementary Figures 32-33
Cu3(HHTP)2 in-pore electrolyte self-diffusion decrease vs bulk electrolyteover 70% decreased self-diffusion coefficient compared to the bulk electrolyteoverText
Approximate
14534 · Modulating the EDL Structure with MOF Composition · Supplementary Figures 32-33

DFT-CES electronic density of states and charge-density-difference analysis

Cu3(HHTP)2 QM/MM electrochemical interface model · Model

Cu3(HHTP)2 electrochemical interface under charged conditions and PZC; counterion insertion and co-ion removal mechanisms compared.

Temperature
300
Atmosphere
computational
Geometry
QM/MM electrode-electrolyte interface
Context
model pristine framework
Measurement source
14532 · Polarization Phenomena of MOFs · Figure 4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Cu oxidation state in Cu3(HHTP)2 model/electrode windowCu2+; 3d9 open-shell doublet configurationText
Exact Reported
14532 · Polarization Phenomena of MOFs · Figure 4
Cu magnetic moment in Cu3(HHTP)2 potential window0.6 uBText
Exact Reported
14533 · Polarization Phenomena of MOFs · Figure 4b
Total magnetisation increase in Cu3(HHTP)2 simulation cell0.05 uB from the PZCText
Exact Reported
14533 · Polarization Phenomena of MOFs · Figure 4b
Cu3(HHTP)2 surface charge at DeltaU = -0.2 V, co-ion removal-1.5 uC cm^-2Text
Exact Reported
14531-14532 · Polarization Phenomena of MOFs · Figure 3b
Cu3(HHTP)2 surface charge at DeltaU = -0.2 V, counterion insertion-4.5 uC cm^-2Text
Exact Reported
14532 · Polarization Phenomena of MOFs · Figure 3c
Cu3(HHTP)2 surface charge at DeltaU = +0.2 V, co-ion removal+4.5 uC cm^-2Text
Exact Reported
14532 · Polarization Phenomena of MOFs · Figure 3e
Cu3(HHTP)2 surface charge at DeltaU = +0.2 V, counterion insertion+1.5 uC cm^-2Text
Exact Reported
14532 · Polarization Phenomena of MOFs · Figure 3d

DFT-CES density of states and magnetic moment analysis

Cu3(HITP)2 QM/MM electrochemical interface model · Model

Cu3(HITP)2 electrochemical interface at varied surface charge densities.

Temperature
300
Atmosphere
computational
Geometry
QM/MM electrode-electrolyte interface
Context
model pristine framework
Measurement source
22 · Supplementary Fig. 21 · Supplementary Figure 21
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Cu oxidation state in Cu3(HITP)2 modelCu maintained as 2+ independent of biased potentialText
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Supplementary Figure 21
Cu magnetic moment in Cu3(HITP)2 model0.6 uBCaption
Exact Reported
22 · Supplementary Fig. 21 · Supplementary Figure 21

QM/MM electrochemical interface calculation on graphite

Graphite electrochemical interface model · Model

Graphite surface charge density-biased potential curve with respect to ion-exchange ratio.

Atmosphere
computational
Geometry
graphite-electrolyte interface model
Context
non-MOF computational control
Measurement source
10 · Supplementary Fig. 9 · Supplementary Figure 9
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Graphite model differential capacitance5-7 uF cm^-2rangeCaption
Range
10 · Supplementary Fig. 9 · Supplementary Figure 9

Mean-field QM/MM DFT-CES electrochemical simulation using Quantum ESPRESSO and LAMMPS; capacitance from C = sigma/DeltaU

Cu3(HHTP)2 QM/MM electrochemical interface model · Model

Cu3(HHTP)2 electrode at QM level with 1 M NEt4BF4 in acetonitrile; surface charge density from -4.5 to +4.5 uC cm^-2; X = 1 counterion insertion, X = 0 ion exchange, X = -1 co-ion removal.

Temperature
300
Atmosphere
canonical ensemble MD
Geometry
cylindrical pore model; two-layer (1 x sqrt(3)) rectangular electrode cell
Context
model pristine framework with explicit electrolyte
Measurement source
14535 · Computational Details · Table 1
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
DeltaU range for Cu3(HHTP)2 co-ion removal mechanism-0.8 to 0.2 V as sigma changes from -4.5 to +4.5 uC cm^-2rangeText
Range
14530 · Electrochemical Interface and Differential Capacitance · Figure 2b
DeltaU range for Cu3(HHTP)2 counterion insertion mechanism-0.3 to 0.5 V as sigma changes from -4.5 to +4.5 uC cm^-2rangeText
Range
14530 · Electrochemical Interface and Differential Capacitance · Figure 2b
Cu3(HHTP)2 simulated gravimetric capacitance, X=1, negative sigma231 F g^-1SI Table
Exact Reported
36 · Supplementary Table 2 · Supplementary Table 2
Cu3(HHTP)2 simulated gravimetric capacitance, X=-1, positive sigmaMarked as a best value within this paper308 F g^-1SI Table
Exact Reported
36 · Supplementary Table 2 · Supplementary Table 2
Cu3(HHTP)2 simulated capacitance, X=0.5, negative sigma range12 uF cm^-2Table
Exact Reported
14531 · Results and Discussion · Table 1
Cu3(HHTP)2 simulated capacitance, X=0.5, positive sigma range12 uF cm^-2Table
Exact Reported
14531 · Results and Discussion · Table 1
Cu3(HHTP)2 simulated capacitance, X=0 ion exchange, negative sigma range8 uF cm^-2Table
Exact Reported
14531 · Results and Discussion · Table 1
Cu3(HHTP)2 simulated capacitance, X=0 ion exchange, positive sigma range12 uF cm^-2Table
Exact Reported
14531 · Results and Discussion · Table 1
Cu3(HHTP)2 simulated capacitance, X=1 counterion insertion, negative sigma rangeMarked as a best value within this paper18 uF cm^-2 for -4.5 < sigma < 0 uC cm^-2Table
Exact Reported
14531 · Results and Discussion · Table 1
Cu3(HHTP)2 simulated capacitance, X=1 counterion insertion, positive sigma range8 uF cm^-2 for 0 < sigma < +4.5 uC cm^-2Table
Exact Reported
14531 · Results and Discussion · Table 1
Cu3(HHTP)2 simulated capacitance, X=-0.5, negative sigma range7 uF cm^-2Table
Exact Reported
14531 · Results and Discussion · Table 1
Cu3(HHTP)2 simulated capacitance, X=-0.5, positive sigma range11 uF cm^-2Table
Exact Reported
14531 · Results and Discussion · Table 1
Cu3(HHTP)2 simulated capacitance, X=-1 co-ion removal, negative sigma range6 uF cm^-2Table
Exact Reported
14531 · Results and Discussion · Table 1
Cu3(HHTP)2 simulated capacitance, X=-1 co-ion removal, positive sigma rangeMarked as a best value within this paper24 uF cm^-2Table
Exact Reported
14531 · Results and Discussion · Table 1
Cu3(HHTP)2 simulation cell Connolly surface area1286 m2 g^-1Caption
Exact Reported
2 · Supplementary Fig. 1 · Supplementary Figure 1

Mean-field QM/MM DFT-CES electrochemical simulation; capacitance from inverse sigma-DeltaU slope

Cu3(HITP)2 QM/MM electrochemical interface model · Model

Cu3(HITP)2 electrode model with 1 M NEt4BF4/acetonitrile; X parameter varied across counterion insertion, ion exchange and co-ion removal.

Temperature
300
Atmosphere
canonical ensemble MD
Geometry
cylindrical pore model; (1 x sqrt(3)) rectangular unit cell
Context
model pristine framework with explicit electrolyte
Measurement source
14534 · Modulating the EDL Structure with MOF Composition · Table 2
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Cu3(HITP)2 simulated capacitance, X=0.5, negative sigma range13 uF cm^-2Table
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Table 2
Cu3(HITP)2 simulated capacitance, X=0.5, positive sigma range24 uF cm^-2Table
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Table 2
Cu3(HITP)2 simulated capacitance, X=0 ion exchange, negative sigma range11 uF cm^-2Table
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Table 2
Cu3(HITP)2 simulated capacitance, X=0 ion exchange, positive sigma range23 uF cm^-2Table
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Table 2
Cu3(HITP)2 simulated capacitance, X=1 counterion insertion, negative sigma range17 uF cm^-2Table
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Table 2
Cu3(HITP)2 simulated capacitance, X=1 counterion insertion, positive sigma rangeMarked as a best value within this paper25 uF cm^-2Table
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Table 2
Cu3(HITP)2 simulated capacitance, X=-0.5, negative sigma range10 uF cm^-2Table
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Table 2
Cu3(HITP)2 simulated capacitance, X=-0.5, positive sigma range23 uF cm^-2Table
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Table 2
Cu3(HITP)2 simulated capacitance, X=-1 co-ion removal, negative sigma range9 uF cm^-2Table
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Table 2
Cu3(HITP)2 simulated capacitance, X=-1 co-ion removal, positive sigma rangeMarked as a best value within this paper25 uF cm^-2Table
Exact Reported
14534 · Modulating the EDL Structure with MOF Composition · Table 2
Cu3(HITP)2 simulation cell Connolly surface area1333 m2 g^-1Caption
Exact Reported
21 · Supplementary Fig. 20 · Supplementary Figure 20