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The maximal current density of 220 mA cm−2 and power density of 65 mW cm−2 were obtained at ambient conditions.
The first analysis showed that, for equal anode and cathode catalyst layer thicknesses, maximal current density was achieved by placing more catalyst in the cathode than in the anode.
The second analysis showed that, for equal anode and cathode catalyst layer density, maximal current density was achieved by using a catalyst layer that is thicker on the cathode side than that on the anode side.
This peculiarity of the system leads to the anomalous dependence of the maximal current density of the bromate reaction on the electrode size: if the electrode radius is under its critical value the current density is very small since it is determined by the discharge of bromine species from the bulk solution, with no significant transformation of bromate.
As it has been demonstrated by calculations for the dependence of the local value of the maximal current density, jmax, on the local value of the diffusion layer thickness, zd, high values of the current density cannot be achieved for relatively thin diffusion layers.
Expressions for the concentration distributions inside the (thin) kinetic layer, as well as those for the maximal current density, derived within the framework of the convective-diffusion theory are in agreement with those found for the Generalized Nernst Layer model proposed by us earlier.
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maximum current density.
An Esaki diode, vertically integrated to the transistor, limits the maximal emitter current density.
Here the maximal possible current density in Cu lines and an outer magnetic field of 2 T were considered.
ICaL showed voltage-dependent activation with Vhalf≈ −7 mV (k≈ 6 mV) and a maximal inward current density at 0 mV under control conditions.
Transient peak sodium inward currents had similar amplitude in Ctrl and A-T neurons: maximal peak current density was 84.9±19.6 pA/pF, n=10 in Ctrl neurons, 82.7±13.5 pA/pF, n=13 in A-T neurons.
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