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Figure 31-10 illustrates the effect of variations in the chlorine-electrode resis tivity-thickness ratio on current density. Again, the zinc-electrode current den sity at the chlorine bus is used as a reference, as it serves to indicate the sen sitivity of the parameter variations on current density. The graph reveals that an essentially linear relationship exists between the current density at the chlo rine bus and the chlorine-electrode resistivity-thickness ratio. 54 - > 48 Z 44 CC 34 STANDARD CASE CHLORINE-ELECTRODE RESISTIVITY-THICKNESS RATIO thickness ratio, Pg/<5g, —ohm Figure 31-10. Active cell current density adjacent to the chlorine electrode bus as a function of the chlorine-electrode resistivity-thickness ratio. Figure 31-11 shows the effect of the compound resistivity-gap product on current density at the chlorine bus. It is clear from this curve that the effect of this parameter on the current-density distribution is significant. This parameter is of course the most susceptible to physical variation. Even a simple temperature change in the electrolyte will cause a change in the compound resistivity, p^_. Although the current-density distribution curve in Figure 31-7 may be smoothed or leveled by an increase in p *6 , this will also increase the voltaic losses in the te 31-18 10oPDF Image | Development of the Zinc-Chlorine Battery for Utility
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