Abstract
IT is well known that a magnetic field is almost completely excluded from a superconductor, so that a long cylinder has a diamagnetic susceptibility which is 1/4 for a field parallel to the cylinder axis, or 1/2 for a transverse field. The magnetic field does, however, penetrate slightly, so that the actual diamagnetic susceptibility should be slightly smaller than X0, and elementary considerations show that we should have where defines a penetration depth and r is the cylinder radius. Previous experiments by one of us1 on colloidal mercury, and by Appleyard and others2 on thin mercury films (in both cases involving specimen size comparable to or smaller than ), showed that is of the order of 10-5 cm. and increases several times as the temperature approaches the transition point (4.17° K.). Thus for cylinders with radii of order 10-3 cm. should vary by a few percent close to 4.17° K.
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References
Shoenberg, D., Proc. Roy. Soc., A, 175, 49 (1940).
Appleyard, E. T. S., Bristow, J. R., London, H., and Misener, A. D., Proc. Roy. Soc., A, 172, 540 (1939).
Ginsburg, V., J. Phys. (U.S.S.R.), 9, 305 (1945).
Casimir, H. B. G., Physica, 7, 887 (1940).
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DÉSIRANT, M., SHOENBERG, D. Penetration of Magnetic Field into Superconducting Mercury. Nature 159, 201–202 (1947). https://doi.org/10.1038/159201b0
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DOI: https://doi.org/10.1038/159201b0
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