Scientific American Supplement, No. 288, July 9, 1881 by Various
page 118 of 160 (73%)
page 118 of 160 (73%)
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(E_1+E_2+etc.)-(F_1+F_2+etc.) C = ----------------------------- R [TEX: C = \frac{(E_1+E_2+\text{etc.})-(F_1+F_2+\text{etc.})}{R}] C C P = ---((E_1+E_2+etc.); Q = ---(F_1+F_2+etc.) 746 746 [TEX: \frac{C}{746}(E_1+E_2+\text{etc.});\ Q = \frac{C}{746}(F_1+F_2+\text{etc.})] C squared R H = ----- . 746 [TEX: H = \frac{C^2 R}{746}.] The lifting power of an electro-magnet of given volume is proportional to the heat generated against resistance in the wire of the magnet. The future of many electrical appliances depends on how general is the public comprehension of the lessons taught by these wall sheets. If a few capitalists in London would only spend a few days in learning thoroughly what these mean, electrical appliances of a very distant future would date from a few months hence. A number of experiments were shown, in some of which electrical energy |
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