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XX.—Changes of Electrical Resistance accompanying Longitudinal and Transverse Magnetizations in Nickel

Published online by Cambridge University Press:  15 September 2014

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Extract

In 1903 I communicated to the Society a paper on the relation between magnetization and resistance of nickel at high temperatures (1). In this paper the magnetization was along the direction in which the resistance was measured. A second paper, in which the magnetization was transverse to the direction in which the resistance was measured, was communicated in 1906 (2). In these later experiments a flat coil of nickel wire was used; and it was necessary to use very high fields before an appreciable change of resistance was obtained.

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Proceedings
Copyright
Copyright © Royal Society of Edinburgh 1914

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References

REFERENCES

(1)Knott, C. G., “Magnetization and Resistance of Nickel at High Temperatures,” Trans. R.S.E., xli. p. 39.Google Scholar
(2)Knott, C. G., “Magnetization and Resistance of Nickel at High Temperatures,” part 2, 1906, Trans. R.S.E., xlv. p. 547.Google Scholar
(3)Thomson (Kelvin), W., “The Electro-dynamic Properties of Metals,” Bakerian Lecture, Phil. Trans., cxlvi. p. 649, 1856; Math, and Phys. Papers, vol. ii. p. 307.Google Scholar
(4)Grunmach, L., “Über den Einfluss transversaler Magnetisierung auf die electrische Leitungsfähigkeit der Metalle,” Ann. d. Physik, vol. xxii. p. 141, 1906.Google Scholar
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(8)Adams, E. P., “The Effect of a Transverse Magnetic Field on Metallic Resistance,” Physical Review, vol. xxiv. p. 428, 1907.Google Scholar
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