Cyclopedia of Telephony & Telegraphy Vol. 1 - A General Reference Work on Telephony, etc. etc. by Robert Millikan;Samuel McMeen;George Patterson;Kempster Miller;Charles Thom
page 69 of 497 (13%)
page 69 of 497 (13%)
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resistance. Electromotive force being a cause, and resistance a state,
current is the result. The formula of this relation, Ohm's law, is C = E/R _C_ being the current which results from _E_, the electromotive force, acting upon _R_, the resistance. The units are: of current, the ampere; of electromotive force, the volt; of resistance, the ohm. As the conductivity or resistance of a line is the property of controlling importance in telegraphy, a similar relation was expected in early telephony. As the current in the telephone line varies rapidly, certain other properties of the line assume an importance they do not have in telegraphy in any such degree. The importance that these properties assume is, that if they did not act and the resistance of the conductors alone limited speech, transmission would be possible direct from Europe to America over a pair of wires weighing 200 pounds per mile of wire, which is less than half the weight of the wire of the best long-distance land lines now in service. The distance from Europe to America is about twice as great as the present commercial radius by land lines of 435-pound wire. In other words, good speech is possible through a mere resistance twenty times greater than the resistance of the longest actual open-wire line it is possible to talk through. The talking ratio between a mere resistance and the resistance of a regular telephone cable is still greater. Electrostatic Capacity. It is the possession of electrostatic capacity which enables the condenser, of which the Leyden jar is a |
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