Computational Modelling — Tunable Electrical Conductivity of Flexible Metal-Organic Frameworks

Measurement evidence

Computational Modelling

Tunable Electrical Conductivity of Flexible Metal-Organic Frameworks · Chong S., Rogge S.M.J., Kim J. · Chemistry of Materials · 2022 · 254-265

7 measurement groups · 17 results

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

DDEC6 DFT-calculated M-N bond-order analysis

Zn(NDIDP) computational model · Model

Average bond order between the metal ion and pyrazolate N atom in lp and np phases.

Atmosphere
in silico
Context
model_system
Measurement source
S21 · M-N bond lengths and bond-orders of M(NDIDP) · Table S2
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Co(NDIDP) M-N bond-order difference lp minus npdifference = 0.044SI Table
Exact Reported
S21 · M-N bond lengths and bond-orders of M(NDIDP) · Table S2
Fe(NDIDP) M-N bond-order difference lp minus npdifference = 0.102SI Table
Exact Reported
S21 · M-N bond lengths and bond-orders of M(NDIDP) · Table S2
Zn(NDIDP) M-N bond-order difference lp minus npdifference = 0.036SI Table
Exact Reported
S21 · M-N bond lengths and bond-orders of M(NDIDP) · Table S2

DFT geometry optimisation and electronic structure; VASP, PAW, PBE-D3(BJ), HSE06 band structures

Zn(NDIDP) computational model · Model

Gamma-centred k-point grids under 0.3 A-1, 600 eV cutoff, SCF 1e-6 eV, Gaussian smearing sigma 0.01 A; spin polarisation for Co and Fe.

Atmosphere
in silico
Context
model_system
Measurement source
255 · Methods - DFT Calculations
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource

Force-field MD using QuickFF-derived force fields and Yaff

Zn(NDIDP) computational model · Model

1 x 1 x 2 supercells in (N,V,sigma_a=0,T) ensemble; Nose-Hoover thermostat; Martyna-Tobias-Tuckerman-Klein barostat; 0.5 fs timestep; 0.5 ns equilibration plus 0.5 ns production.

Temperature
300
Atmosphere
in silico
Context
model_system
Measurement source
256 · Methods - MD Simulations
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
M(NDIDP) low-volume P(V) anomaly pressureca. 1.5 GPa1500 MPaca.Text
Approximate
259 · Flexibility of M(NDIDP): Pressure vs Volume Equation of State · Figure S4

MD-derived pressure-versus-volume equation of state

Co(NDIDP) computational model · Model

T = 300 K; external pressure/mechanical stress as stimulus.

Temperature
300
Atmosphere
in silico
Context
model_system
Measurement source
258 · Flexibility of M(NDIDP): Pressure vs Volume Equation of State · Figure 4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Co(NDIDP) lp-to-np transition pressure13 MPaText
Rounded Reported
258 · Flexibility of M(NDIDP): Pressure vs Volume Equation of State · Figure 4
Co(NDIDP) np-to-lp transition pressure-224 MPaText
Rounded Reported
258 · Flexibility of M(NDIDP): Pressure vs Volume Equation of State · Figure 4

MD-derived pressure-versus-volume equation of state

Fe(NDIDP) computational model · Model

T = 300 K; external pressure/mechanical stress as stimulus.

Temperature
300
Atmosphere
in silico
Context
model_system
Measurement source
258 · Flexibility of M(NDIDP): Pressure vs Volume Equation of State · Figure 4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Fe(NDIDP) lp-to-np transition pressure-42 MPaText
Rounded Reported
258 · Flexibility of M(NDIDP): Pressure vs Volume Equation of State · Figure 4
Fe(NDIDP) np-to-lp transition pressure-217 MPaText
Rounded Reported
258 · Flexibility of M(NDIDP): Pressure vs Volume Equation of State · Figure 4

MD-derived pressure-versus-volume equation of state

Zn(NDIDP) computational model · Model

T = 300 K; external pressure/mechanical stress as stimulus.

Temperature
300
Atmosphere
in silico
Context
model_system
Measurement source
258 · Flexibility of M(NDIDP): Pressure vs Volume Equation of State · Figure 4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Zn(NDIDP) lp/np energy barrier reference0.12 eVText
Exact Reported
S26 · Flexibility and Conductivity of Zn(NDIDP)-CH3 · Figure S20
Zn(NDIDP) lp-to-np transition pressure3 MPaText
Rounded Reported
258 · Flexibility of M(NDIDP): Pressure vs Volume Equation of State · Figure 4
Zn(NDIDP) np-to-lp transition pressure-234 MPaText
Rounded Reported
258 · Flexibility of M(NDIDP): Pressure vs Volume Equation of State · Figure 4

MD-derived P(V) equation of state for Zn(NDIDP)-CH3

Zn(NDIDP)-CH3 computational model · Model

DFT-derived force field parameters; two mechanically stable branches; some abnormal stacked configurations.

Atmosphere
in silico
Context
model_system
Measurement source
S27 · Flexibility and Conductivity of Zn(NDIDP)-CH3 · Figure S21
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Zn(NDIDP)-CH3 lp/np energy barrier1.20 eVText
Exact Reported
S26 · Flexibility and Conductivity of Zn(NDIDP)-CH3 · Figure S20
Zn(NDIDP)-CH3 lp energy difference from np0.04 eVText
Exact Reported
S26 · Flexibility and Conductivity of Zn(NDIDP)-CH3 · Figure S20
Zn(NDIDP)-CH3 critical pressure for lp-to-np transition322 MPaText
Exact Reported
S27 · Flexibility and Conductivity of Zn(NDIDP)-CH3 · Figure S21
Zn(NDIDP)-CH3 lp energy-minimum volumeV = 4232.1 A3Text
Exact Reported
S26 · Flexibility and Conductivity of Zn(NDIDP)-CH3 · Figure S20
Zn(NDIDP)-CH3 np energy-minimum volumeV = 2082.6 A3Text
Exact Reported
S26 · Flexibility and Conductivity of Zn(NDIDP)-CH3 · Figure S20
Zn(NDIDP)-CH3 critical pressure ratio versus Zn(NDIDP)107 times largerText
Exact Reported
S27 · Flexibility and Conductivity of Zn(NDIDP)-CH3 · Figure S21