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ART. 117 - On Clark's Standard Cells

Published online by Cambridge University Press:  05 December 2011

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Summary

In the hope of finding a clue as to the origin of some of the minor anomalies of Clark's cells, I have made experiments upon the e.m.f. of combinations, in which two different strengths of zinc amalgam take the place of the zinc and pure mercury of the Clark cell. No mercurous sulphate is employed, the liquid being simply a saturated solution of zinc sulphate.

If the same kind of amalgam be used for both poles, the symmetry is complete, and there should be no e.m.f. But if we take for one pole a strong, but fluid, amalgam, and for the other the same amalgam diluted with an equal volume of pure mercury, we find a very sensible e.m.f., the strong amalgam corresponding to the zinc of the ordinary Clark. In my experiment the e.m.f. was ·004 Clark, and remained pretty constant from day to day. In another cell the same strong amalgam was used for one pole, and for the other pole was diluted with three times its volume of pure mercury. In this case the e.m.f. was ·009 Clark.

If we replace the diluted amalgam with pure mercury, we obtain (without mercurous sulphate) nearly the full e.m.f. of the Clark cell, but, as might be expected, the force is very unsteady. From this it would seem that the function of the mercurous sulphate in the usual form of cell is to retain the purity of the mercury, and that the e.m.f. is largely due to the affinity of mercury for zinc.

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Publisher: Cambridge University Press
Print publication year: 2009
First published in: 1900

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