The simplified form of equation (26) of [21] for a 'simple metallic-metallic' configuration (ref. [20]) is: σ T t = ε 0 Δ x N φ 0 t - ε 0 Δ x ∑ j = 0 N - 1 φ 1 j t - Δ x 2 ∑ j = 0 N - 1 ρ 0 j (21 where, φ 0 t, φ 1 j t, N are the potential on the anode at 't', potential at x1(=1 × Δx) and number of divisions along y-axis.
This inhomogeneous broadening effect was observed and reported by others for simular metallic shell configurations [69 74].
The effects of dopants on different DWCNT configurations (metallic inner/semiconducting outer and vice versa) are studied by changing the laser excitation energy.
The proposed methodology is used to analyse the travelling waves in a bipolar configuration with metallic return.
There was not a direct contact of the atmospheric plasma with the metallic electrode in this configuration.
In this study, effects of the cross-sectional configuration of metallic gas channels on pressure drops are numerically investigated for the comprehensive fluid dynamic analysis of channel flow.
Among the configurations considered in this study, both asymmetrical monopolar/bipolar configuration with metallic returns regardless of grounding and low resistive-grounded/solidly grounded asymmetrical monopolar/bipolar configuration with ground return are effectively low-impedance grounded in terms of fast transients.
However, in metallic thorium, the [Rn]5f16d17s2 configuration is a low-lying excited state and hence the 5f orbitals contribute, existing in a rather broad energy band.
Generally, metallic nanostructures show the controllable configuration, shape, size, and distribution.
The mass of metallic and composite wingbox configurations was calculated via finite element analysis and design optimization techniques.
