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Equation 8 is certainly not the whole story. I haven’t done the experiment
myself, but according to “common knowledge� lead sulfate is formed on the “+� plate, more in agreement with equation 3 than equation 8. It is a tangentially interesting question whether any of the hypothetical reactions listed above play any role -- even as intermediates -- in the real reaction. That is only tangentially interesting, because whether or not those reactions occur, we are still left with a major mystery: how and why does anything containing the SO4 group attack the “+� electrode? Neutral H2SO4 could reach the plate by simple diffusion, but it is present in fantastically low concentration. The bisulfate ion is present in high concentration, but would have to swim uphill against the electric field. The sulfate ion is present in low concentration and would have to swim doubly hard uphill. That means that when the cell is under heavy load, i.e. when there is a large field across the electrolyte, the SO4-related reaction would come to a halt. Let’s put in some numbers: The cell has an open-circuit voltage of 2.2 volts are so. Suppose that we put it under heavy load, so that there is ? v = 0.4 volts “IR� drop across the electrolyte. As always, room temperature corresponds to 25 meV (.025 electron-volts). Putting it all together: the Boltzmann factor that tells you what fraction of the bisulfate ions manage to climb the potential is exp(q ? v / kT) = exp(.4 / .025) = 9,000,000. So we would expect the reaction to proceed millions of times slower when we need it to proceed faster. In the foregoing calculation, we ignored the effect of dielectric screening. This may or may not have been the right thing. Argument pro: energy is conserved. At the end of the day, to move a bisulfate ion up a hill 0.4 volts high, you have to do 0.4 eV of work. Argument con: most of the height of the hill is associated with the dipole layer at the edge of the water, at the place where the electrolyte meets the plate; within the bulk of the electrolyte the field is smaller. The ions can with relatively resonable probability get close to the “+� plate, just outside the dipole layer. Unanswered question: if they get that close, is that close enough? ********************** Note the basis of calculation, opening sentence, paragraph four: 2.2 volts per cell. From http://www.av8n.com/physics/lead-acid.htm |
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