Scientific American Supplement, No. 388, June 9, 1883 by Various
page 47 of 156 (30%)
page 47 of 156 (30%)
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consequently increased in the same ratio. Hence the dynamo, with its
maximum load, must revolve at 588 revolutions per minute, and exert a couple of forty-seven foot-pounds. Let E be the potential of the conductor from which the current is drawn, measured in volts, C the current in amperes, and E1 the E.M.F. of the dynamo. Then E1 is proportional to the product of the angular velocity, and a certain function of the current. For a velocity [omega], let this function be denoted by _f_(C). If the characteristic of the dynamo can be drawn, then _f_(C) is known. We have then w E1 = -------- f [Omega] (1.) If R be the resistance in circuit by Ohm's law, E - E1 C = -------- R w = E ------- f(C) [Omega] ---------------- R and therefore |
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