Observations on the reciprocal influence which magnetic needles exercise over each other, when placed at a given distance within their respective spheres of action, at different positions on the earth; with tables of numerical results obtained at separate stations. Also a method of discovering where certain local influences are acting on the needle, from which may be obtained a proportional correction to be applied to magnetic observations in general
Author(s) -
Edward John Johnson
Publication year - 1837
Publication title -
abstracts of the papers printed in the philosophical transactions of the royal society of london
Language(s) - English
Resource type - Journals
eISSN - 2053-9142
pISSN - 0365-5695
DOI - 10.1098/rspl.1830.0158
Subject(s) - earth's magnetic field , reciprocal , deflection (physics) , spheres , compass , magnet , conjecture , action (physics) , physics , geodesy , magnetic field , mathematics , geology , optics , philosophy , combinatorics , quantum mechanics , linguistics , astronomy
The author, considering it probable that two or more magnetic needles freely suspended at a certain distance in given positions with respect to each other, would develope certain proportionate deflections determined by their position on the earth, made a set of experiments, with a few common compass needles, at Yarmouth, London, and Clifton, which so far confirmed the truth of his conjecture, as to induce him to fix on stations at a greater distance from one another, and to multiply his observations; ascertaining, from time to time, that the magnetic powers of his apparatus had undergone no material change. The results of these observations are given in a tabular form. The author conceives that comparative observations of the amount of deflection produced by one magnet on another, placed in various situations, relative to the meridian, on an horizontal plane, will afford the means of determining the peculiar local influences of the particular situation in which the experiment is made, as distinguished from the general magnetic influence; because the former will act unequally on each magnet, while the latter acts equally on all.
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