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III. Experimental researches in electricity.―Twenty-eight series
Author(s) -
Michael Faraday
Publication year - 1852
Publication title -
philosophical transactions of the royal society of london
Language(s) - English
Resource type - Journals
eISSN - 2053-9223
pISSN - 0261-0523
DOI - 10.1098/rstl.1852.0004
Subject(s) - tangent , line (geometry) , electricity , line of force , series (stratigraphy) , magnetism , power (physics) , magnetic field , motion (physics) , relation (database) , physics , computer science , classical mechanics , mathematics , geometry , condensed matter physics , geology , quantum mechanics , paleontology , database
3070. From my earliest experiments on the relation of electricity and magnetism (114. note), I have had to think and speak of lines of magnetic force as representations of the magnetic power; not merely in the points of quality and direction, but also in quantity. The necessity I was under of a more frequent use of the term in some recent researches (2149. &c.), has led me to believe that the time has arrived, when the idea conveyed by the phrase should be stated very clearly, and should also be carefully examined, that it may be ascertained how far it may be truly applied in representing magnetic conditions and phenomena; how far it may be useful in their elucidation; and, also, how far it may assist in leading the mind correctly on to further conceptions of the physical nature of the force, and the recognition of the possible effects, either new or old, which may be produced by it. 3071. A line of magnetic force may be defined as that line which is described by a very small magnetic needle, when it is so moved in either direction correspondent to its length, that, the needle is constantly a tangent to the line of motion; or it is that line along which, if a transverse wire be moved in either direction, there is no tendency to the formation of any current in the wire, whilst if moved in any other direction there is such a tendency; or it is that line which coincides with the direction of the magnecrystallic axis of a crystal of bismuth, which is carried in either direction along it. The direction of these lines about and amongst magnets and electric currents, is easily represented and understood, in a general manner, by the ordinary use of iron filings.

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