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The measured resistivity values were then used to estimate the aging factor.
The measured resistivity values were compared with values calculated using the combined Fuchs Sondheimer/Mayadas Shatzkes model.
The Nb-TiO2 films deposited on glass by co-sputtering at room temperature were amorphous, and the films crystallized into an anatase structure after vacuum-annealing, with the measured resistivity values comparative to the reported.
Cymgrd simulation software is then used to determine the acceptability of these measured resistivity values by finding out the root mean square error between the measured and calculated values for both wet and dry soil sites.
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True formation measured resistivity.
The measured soil resistivity values were then used to evaluate the ground resistance values of a grounding grid 'with rod' for the wet soil site and 'without rods' for the dry soil site, and then compared with the simulated ground resistance values.
The measured apparent resistivity values were plotted against the half the distance between current electrodes (AB/2) on a log log graph to calculate the vertical electrical sounding curves, which were interpreted using IPI2 win software to determine the apparent resistivity and the thickness of subsurface layer of different composition.
The rms errors between the measured and calculated soil resistivity values are found to be 0%% and 4.92 %, respectively.
Figure 4a shows the change of the transconductance and resistivity values measured for samples a, b, c, d, and e as a function of the growth conditions.
The resistivity values were measured for the prepared crystals, and the thermal conductivity data were taken from the literature [4, 24]. Figure 6b shows the conversion efficiency plotted as a function of (V_{mathrm{light}}).
In the absence of light, both the InSe as-grown crystals and flakes were found to be highly resistive with resistivity values of ρ > 10 Ωcm at room temperature, as measured by a standard two-probe method and under electric fields of up to ∼1 kV cm 1.
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