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GEORG SIMON OHM (1787-1854)

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Originally appearing in Volume V20, Page 34 of the 1911 Encyclopedia Britannica.
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GEORG See also:

SIMON See also:OHM (1787-1854)  , See also:German physicist, was See also:born at See also:Erlangen on the 16th of See also:March 1787, and was educated at the university there . He became See also:professor of See also:mathematics in the See also:Jesuits' See also:college at See also:Cologne in 1817 and in the See also:polytechnic school of See also:Nuremberg in 1833, and in 1852 professor of experimental physics in the university of See also:Munich, where he died on the 7th of See also:July 1854 . His writings were numerous, but, with one important exception, not of the first See also:order . The exception is his pamphlet published in See also:Berlin in 1827, with the See also:title .See also:Die galvanische Kette mathematisth bearbeitet . This See also:work, the germs of which had appeared during the two preceding years in the See also:journals of Schweigger and See also:Poggendorff, has exerted most important See also:influence on the whole development of the theory and applications of current See also:electricity, and See also:Ohm's name has been incorporated in the terminology of See also:electrical See also:science . Nowadays " Ohm's See also:Law," as it is called, in which all that is most valuable in the pamphlet is summarized, is as universally known as anything in physics . The See also:equation for the See also:propagation. of electricity formed on Ohm's printiples is identical with that of J . B . J . See also:Fourier for the propagation of See also:heat; and if, in Fourier's See also:solution of any problem of heat-See also:conduction, we See also:change the word " temperature " to " potential " and write " electric current " instead of " See also:flux of heat," we have the solution of a corresponding problem of electric conduction . The basis of Fourier's work was his clear conception and See also:definition of conductivity . But this involves an See also:assumption, 'undoubtedly true for small temperature-gradients, but still an assumption, viz. that, all else being the same, the flux of heat is strictly proportional to the gradient of temperature .

An exactly similar assumption is made in the statement of Ohm's law, i.e. that, other things being alike, the strength of the current is at each point proportional to the gradient of potential . It happens, how-ever, that with our See also:

modern methods it is much more easy to test the accuracy of the assumption in the See also:case of electricity than in that of heat; and it has accordingly been shown by J . Clerk See also:Maxwell and See also:George Chrystal that Ohm's law is true, within the limits of experimental See also:error, even when the currents are so powerful as almost to fuse the conducting See also:wire .

End of Article: GEORG SIMON OHM (1787-1854)
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