Outlines of the Theory of Electromagnetism a Series of Lectures Delivered Befor

Cover Outlines of the Theory of Electromagnetism a Series of Lectures Delivered Befor
Outlines of the Theory of Electromagnetism a Series of Lectures Delivered Befor
Gilbert Thomas Walker
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This is not however justifiable, for -v- gives the time-change at a stationary point, and while, is finite is infinite unless the value of K on the two sides is the same or the velocity u is parallel to the interface. HERTZ'S EQUATIONS FOR MOVING MEDIA 25 of air with velocity v parallel to OY between the plates. According to Hertz's theory this would create opposite charges on the two plates and hence on reversing L or v there would be a current along a wire joining the plates: this was not fou...nd and the theory must therefore be incorrect. In order to obtain the charges we shall suppose that L, v are constant and that the conditions have become steady so that -r = ; further the charges on the infinite plates being constant, there will be no current in the wire. As the air is uncharged p = 0, and in equation (24) -r- = both in the air and the metal, . '. Rot [Bu] = FrotE in both media. (27). Hence we may put in the air, E + [Bu] = -V (27'), where 7rp = 0.

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