Electrical Transport — Controllable proton-conducting pathways: Via situating polyoxometalates in targeting pores of a metal-organic framework

Measurement evidence

Electrical Transport

Controllable proton-conducting pathways: Via situating polyoxometalates in targeting pores of a metal-organic framework · Lai X., Liu Y., Yang G. et al. · Journal of Materials Chemistry A · 2017 · 9611-9617

19 measurement groups · 37 results

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

AC impedance spectroscopy

1 · Powder

Proton conductivity at 80 C and 100% RH; activation energy from Arrhenius analysis.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
HPW-loaded MIL-101 zigzag pathway
Measurement source
main p.3 · Results and discussion · Table 1
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Sample 1 activation energy0.45 eVTable
Exact Reported
main p.3 · Results and discussion · Table 1
Sample 1 HPW loading38.2 wt%Table
Exact Reported
main p.3 · Results and discussion · Table 1
Sample 1 proton conductivity3.30 x 10^-6 S cm^-1Table
Exact Reported
main p.3 · Results and discussion · Table 1

AC impedance spectroscopy

2 prime · Powder

Proton conductivity at 80 C and 100% RH for lower-loading linear-pathway sample.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
HPW-loaded MIL-101 linear pathway at loading comparable to sample 1
Measurement source
main p.4 · Results and discussion · Fig. S9
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Sample 2 prime HPW loading37.7%Text
Exact Reported
main p.4 · Results and discussion · Fig. S9
Sample 2 prime proton conductivity5.12 x 10^-6 S cm^-1Text
Exact Reported
main p.4 · Results and discussion · Fig. S9
Matched-loading linear pathway enhancement1.55-fold higher than sample 1Text
Rounded Reported
main p.4 · Results and discussion · Fig. S9

AC impedance spectroscopy

2 · Powder

Proton conductivity at 80 C and 100% RH; activation energy from Arrhenius analysis.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
HPW-loaded MIL-101 linear pathway
Measurement source
main p.3 · Results and discussion · Table 1
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Sample 2 activation energy0.42 eVTable
Exact Reported
main p.3 · Results and discussion · Table 1
Sample 2 HPW loading46.9 wt%Table
Exact Reported
main p.3 · Results and discussion · Table 1
Sample 2 proton conductivity7.09 x 10^-6 S cm^-1Table
Exact Reported
main p.3 · Results and discussion · Table 1
Linear pathway conductivity enhancement versus zigzag2.1-fold largerText
Rounded Reported
main p.4 · Results and discussion

AC impedance spectroscopy

3 · Powder

Proton conductivity at 80 C and 100% RH; activation energy from Arrhenius analysis.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
HPW-loaded MIL-101 multiple pathways
Measurement source
main p.3 · Results and discussion · Table 1
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Sample 3 activation energy0.40 eVTable
Exact Reported
main p.3 · Results and discussion · Table 1
Sample 3 HPW loading83.9 wt%Table
Exact Reported
main p.3 · Results and discussion · Table 1
Sample 3 proton conductivity2.17 x 10^-5 S cm^-1Table
Exact Reported
main p.3 · Results and discussion · Table 1

AC impedance spectroscopy and Arrhenius analysis

DETA@3 · Powder

Conductivity at 80 C and 100% RH; Ea from temperature-dependent conductivity under 100% RH.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
Polyamine@HPW@MIL-101
Measurement source
main p.5 · Results and discussion · Table 2
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
DETA@3 activation energy0.31 eVTable
Exact Reported
main p.5 · Results and discussion · Table 2
DETA@3 proton conductivity1.90 x 10^-3 S cm^-1Table
Exact Reported
main p.5 · Results and discussion · Table 2

AC impedance spectroscopy and Arrhenius analysis

EN@3 · Powder

Conductivity at 80 C and 100% RH; Ea from temperature-dependent conductivity under 100% RH.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
Polyamine@HPW@MIL-101
Measurement source
main p.5 · Results and discussion · Table 2
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
EN@3 activation energy0.37 eVTable
Exact Reported
main p.5 · Results and discussion · Table 2
EN@3 proton conductivity6.02 x 10^-4 S cm^-1Table
Exact Reported
main p.5 · Results and discussion · Table 2

AC impedance spectroscopy

MIL-101 · Powder

Proton conductivity of pristine MIL-101, cited for comparison with 1 and 2.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
Pristine MIL-101 control
Measurement source
main p.4 · Results and discussion
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
MIL-101 proton conductivity7.56 x 10^-8 S cm^-1Text
Exact Reported
main p.4 · Results and discussion

AC impedance spectroscopy

PT · Powder

Conductivity under the same experimental conditions as TETA@3.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
Non-MOF HPW/TETA blend comparison
Measurement source
main p.5 · Results and discussion · Table 2
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
PT proton conductivity8.84 x 10^-7 S cm^-1Table
Exact Reported
main p.5 · Results and discussion · Table 2

AC impedance spectroscopy and Arrhenius analysis

TEPA@3 · Powder

Conductivity at 80 C and 100% RH; Ea from temperature-dependent conductivity under 100% RH.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
Polyamine@HPW@MIL-101
Measurement source
main p.5 · Results and discussion · Table 2
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
TEPA@3 activation energy0.25 eVTable
Exact Reported
main p.5 · Results and discussion · Table 2
TEPA@3 proton conductivity9.60 x 10^-3 S cm^-1Table
Exact Reported
main p.5 · Results and discussion · Table 2

AC impedance spectroscopy

1.7TETA@3 · Powder

1.7TETA@3 TETA-loading-series conductivity at 80 C and 100% RH; exact value not stated in main text.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
TETA loading optimisation on HPW@MIL-101 sample 3
Measurement source
main p.6 · Results and discussion · Fig. S17
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
1.7TETA@3 conductivity qualitative positionnot among the similar but largest proton conductivities in the main-text summaryQualitative
Qualitative
main p.6 · Results and discussion · Fig. S17

AC impedance spectroscopy

2.7TETA@3 · Powder

2.7TETA@3 TETA-loading-series conductivity at 80 C and 100% RH; main text reports approximate largest-group value.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
TETA loading optimisation on HPW@MIL-101 sample 3
Measurement source
main p.6 · Results and discussion · Fig. S17
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
2.7TETA@3 approximate proton conductivityMarked as a best value within this paperaround 1.52 x 10^-2 S cm^-1Text
Approximate
main p.6 · Results and discussion · Fig. S17

AC impedance spectroscopy

3.2TETA@3 · Powder

3.2TETA@3 TETA-loading-series conductivity at 80 C and 100% RH; main text reports approximate largest-group value.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
TETA loading optimisation on HPW@MIL-101 sample 3
Measurement source
main p.6 · Results and discussion · Fig. S17
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
3.2TETA@3 approximate proton conductivityMarked as a best value within this paperaround 1.52 x 10^-2 S cm^-1Text
Approximate
main p.6 · Results and discussion · Fig. S17

AC impedance spectroscopy

4.2TETA@3 · Powder

4.2TETA@3 TETA-loading-series conductivity at 80 C and 100% RH; main text reports approximate largest-group value.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
TETA loading optimisation on HPW@MIL-101 sample 3
Measurement source
main p.6 · Results and discussion · Fig. S17
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
4.2TETA@3 approximate proton conductivityMarked as a best value within this paperaround 1.52 x 10^-2 S cm^-1Text
Approximate
main p.6 · Results and discussion · Fig. S17

AC impedance-derived proton conductivity versus relative humidity

TETA@3 · Powder

RH dependence of TETA@3 at 25 C from SI Fig. S19; values read visually from the plotted log(sigma/S cm^-1) axis.

Temperature
298
Atmosphere
45-100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
Best polyamine@HPW@MIL-101 sample under varying humidity
Measurement source
SI p.17 · Supplementary Information · Figure S19
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
TETA@3 log proton conductivity at 100% RH, 25 CMarked as a best value within this paperapprox. -2.33 log(sigma/S cm^-1) at 100% RHvisual estimate from plotted axisFigure Axis
Approximate
SI p.17 · Supplementary Information · Figure S19
TETA@3 log proton conductivity at 45% RH, 25 Capprox. -4.6 log(sigma/S cm^-1) at 45% RHvisual estimate from plotted axisFigure Axis
Approximate
SI p.17 · Supplementary Information · Figure S19
TETA@3 log proton conductivity at 60% RH, 25 Capprox. -4.3 log(sigma/S cm^-1) at 60% RHvisual estimate from plotted axisFigure Axis
Approximate
SI p.17 · Supplementary Information · Figure S19
TETA@3 log proton conductivity at 70% RH, 25 Capprox. -3.75 log(sigma/S cm^-1) at 70% RHvisual estimate from plotted axisFigure Axis
Approximate
SI p.17 · Supplementary Information · Figure S19
TETA@3 log proton conductivity at 80% RH, 25 Capprox. -3.42 log(sigma/S cm^-1) at 80% RHvisual estimate from plotted axisFigure Axis
Approximate
SI p.17 · Supplementary Information · Figure S19
TETA@3 log proton conductivity at 90% RH, 25 Capprox. -2.85 log(sigma/S cm^-1) at 90% RHvisual estimate from plotted axisFigure Axis
Approximate
SI p.17 · Supplementary Information · Figure S19

Time-dependent proton conductivity stability test

TETA@3 · Powder

TETA@3 held at 80 C and 100% RH; SI Fig. S20 plots log(sigma/S cm^-1) versus time for about 14 days.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
Best polyamine@HPW@MIL-101 sample stability
Measurement source
SI p.17 · Supplementary Information · Figure S20
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
TETA@3 approximate log conductivity after 14 daysapproximately -1.96 log(sigma/S cm^-1) after 14 days, essentially unchanged across the plotted periodvisual estimate from plotted axisFigure Axis
Approximate
SI p.17 · Supplementary Information · Figure S20

AC impedance spectroscopy and Arrhenius analysis

TETA@3 · Powder

Conductivity at 80 C and 100% RH; temperature-dependent conductivity from 25 to 80 C under 100% RH; humidity and long-term stability tests referenced in SI.

Temperature
298-353
Atmosphere
100% RH; RH-dependence at 25 C referenced
Geometry
Pressed powder pellet between copper electrodes
Context
Best polyamine@HPW@MIL-101 sample
Measurement source
main p.6 · Results and discussion · Fig. 4; Table 2
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
TETA@3 activation energyMarked as a best value within this paper0.22 eVTable
Exact Reported
main p.5 · Results and discussion · Table 2
TETA@3 proton conductivityMarked as a best value within this paper1.52 x 10^-2 S cm^-1Table
Exact Reported
main p.5 · Results and discussion · Table 2
TETA@3 long-term stability conditionmore than half a month at 80 C and 100% RH with no degradationText
Approximate
main p.6 · Results and discussion · Fig. S20

AC impedance spectroscopy

1.2TETA@3 · Powder

TETA-loading series compared at 80 C and 100% RH; exact table result available for 1.2TETA@3, qualitative/approximate values for higher-loading variants in main text.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
TETA loading optimisation on HPW@MIL-101 sample 3
Measurement source
main p.6 · Results and discussion · Fig. S17
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
1.2TETA@3 proton conductivity6.70 x 10^-4 S cm^-1Table
Exact Reported
main p.5 · Results and discussion · Table 2

AC impedance spectroscopy

TETA@MIL-101 · Powder

Conductivity under the same experimental conditions as TETA@3.

Temperature
353
Atmosphere
100% RH
Geometry
Pressed powder pellet between copper electrodes
Context
TETA-modified MIL-101 control without HPW
Measurement source
main p.5 · Results and discussion · Table 2
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
TETA@MIL-101 proton conductivity2.15 x 10^-7 S cm^-1Table
Exact Reported
main p.5 · Results and discussion · Table 2

AC impedance spectroscopy on pressed powder discs

MIL-101 · Powder

Powders pressed at 10 MPa for 1 min into discs of 10 mm diameter and 3.0 +/- 0.2 mm thickness, sandwiched between copper electrodes; 1 Hz to 1 MHz, 150 mV input; target condition held for 4 h.

Atmosphere
Relative humidity controlled using an HDHWHS-50 incubator
Geometry
Pressed powder pellet between two copper electrodes
Context
General transport method for all powder samples
Measurement source
main p.3 · Experimental - AC impedance measurements
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource