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The variable (n(t)/N) is extended to (n(mathbf{x},t)) representing the density of active neurons at the cortical location x at time t, and the total input current (I(n)) becomes the current density I bigl(n(mathbf{x} bigr) = int d^{d} x^{prime} w_{EE} bigl(mathbf{x} - mathbf {x}'bigr) nbigl(mathbf{x}'bigr) + h_{E} (mathbf{x}).
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The cathode potentials are found to become nearly independent of the current density when it exceeds ∼ 104 A m−2, the steady-state metal concentration in the cathode layer of the electrolyte being still far from saturated.
Before the peak of the current density becomes maximum, reconnection takes place, which ejects particles from the reconnection region.
Firstly, thermionic emission will gradually increase its effect in the high fields when the current density becomes high.
As the roughness develops due to natural fluctuations, the current density becomes less uniform locally, leading to continued amplification of the roughness.
The main electrochemical parameters were determined: Ecorr: corrosion potential as zero current potential; E p : passivation potential where the current density becomes constant; | Ecorr − E p |: tendency to passivation with low values characterizes a strong, easy passivation; i p : passive current density representing the corrosion resistance of the passive layer [ 37, 44, 45, 50].
The current density became lower than that under terrestrial conditions.
The effect of microgravity on the current density became appreciable when the potential exceeded about 2.5 V.
When the current density, j, becomes zero, the equation should reduce to the open circuit voltage, E0.
Where the P1 layer porosity is low, or the layer very thick, spatial variation of the current density may become significant.
The current density for HCHO oxidation became very low with a decrease in the palladium particle size.
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CEO of Professional Science Editing for Scientists @ prosciediting.com