Scientific American Supplement, No. 388, June 9, 1883 by Various
page 48 of 156 (30%)
page 48 of 156 (30%)
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[Omega](E - CR) (2.)
w = ----------------- f(C) Let _a_ be the efficiency with which the motor transforms electrical into mechanical energy, then-- Power required = L w = a E1 C w = a C ------- f(C) [Omega] Dividing by _w_, a C f(C) L = -------- . (3.) [Omega] It must be noted that L is here measured in electrical measure, or, adopting the unit given by Dr. Siemens in the British Association Address, in joules. One joule equals approximately 0.74 foot pound. Equation 3 gives at once an analytical proof of the second principle stated above, that for a given motor the current depends upon the couple, and upon it alone. Equation 2 shows that with a given load the speed depends upon E, the electromotive force of the main, and R the resistance in circuit. It shows also the effect of putting into the circuit the resistance frames placed beneath the car. If R be increased, until CR is equal to E, then _w_ vanishes, and the car remains at rest. If R be still further increased, Ohm's law applies, |
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