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The open-circuit voltage has small differences, but the current density varies significantly.
But the current density somewhat fluctuated at high external cathodic voltage of −2.4 V, and it became more unstable at −2.8 V.
For TNT-based support catalyst (A and B), the EASA seem to be lower than non-TNT-based support catalyst (C and D) but the current density normalised by EASA calculated was higher than that non-TNT-based support catalyst.
The sloped flat region of the discharge curves could be attributed to several factors such as current density and crystal structure of the active material, but the current density of 1 μA/cm2 was quite low compared to the capacity of 44.7 μAh/cm2.
With ΔCTPxxP bestrophin-1, currents showed the same time-dependent activation as with wild-type bestrophin-1, but the current density was further reduced due to decreased number of Ca2+ channels proteins in the cell membrane.
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It is observed that with the substitution of cerium on calcium site not only the phase pure material is obtained but also the current density increases.
EDTA or HEDTA did not significantly affect the silver and zinc deposition potentials, but decreased the current density for silver zinc deposition.
The Au_TA_HKUST electrode reveals a similar response regarding the potential range, but the current densities are lower.
With the decrease of the CCL thickness and the Nafion content, the cell voltage reduces at the low current density but increases when the current density is higher.
Currents of several amperes per square centimetre can be drawn from such oxide cathodes, but in practice the current density is generally less than 0.2 ampere per square centimetre.
The deposition time at which such a transition was detected depended not only on the amount of deposited ZnO but also on the current density during electrodeposition, pointing at a different growth mode of ZnO, and on the electrode geometry, pointing at the influence of different diffusion profiles of the reacting ions.
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but the current trend
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