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Figure 6 shows a differential circuit element of the single cell. This element is simply one segment of the circuit model used in the approximate treatment. The element is located a distance (y) from the chlorine bus, and extends a dis tance (Ay) along the width of the cell. 6 -H Figure 6. Differential circuit element of a single cell. This differential element was found to be quite similar to the differential elements in cooling fins (1) and fuel cells (2). With rectangular cooling fins, the heat transfer along the fin is analogous to the distribution of current along the chlo rine electrode. In both situations, the distributions are a function of the width direction alone. Also, the assumption that the zinc electrode is an equipotential surface is the same as assuming that the air around a cooling fin is at constant temperature. In the case of fuel cells, the only difference in the circuit elements rests in the assumption that significant resistance is present in the fuel electrode. The fuel electrode in the fuel cell is equivalent to the zinc electrode in the zinc chlorine cell. As stated previously, the resistance presented by the zinc electrode is so small that the zinc electrode may be treated as an equipotential surface. Due to the similarity between these situations, the integration technique used for the zinc chlorine cell is an adaptation of the other integration procedures. 31-10 g1y+Ay zly+AyPDF Image | Development of the Zinc-Chlorine Battery for Utility
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