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ART. 134 - The Reaction upon the Driving-Point of a System executing Forced Harmonic Oscillations of Various Periods, with Applications to Electricity

Published online by Cambridge University Press:  05 December 2011

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Summary

The object of the present communication is to prove some general mechanical theorems, which may be regarded as in some sort extensions of that of Thomson relating to the energy of initial motions. The question involved in the latter may be thus stated:—

“Given any material system at rest. Let any parts of it be set in motion suddenly with any specified velocities possible, according to the connections of the system; and let its other parts be influenced only by its connections with these. It is required to find the motion.” And the solution is “that the motion actually taken by the system is that which has less kinetic energy than any other motion fulfilling the prescribed velocity conditions.” On the other hand, if the impulses are given, a theorem of Bertrand tells us that the kinetic energy is the greatest possible.

For our present purpose we suppose the system to be set in motion by an impulse of one particular type, which we may call the first. The impulse itself may be denoted by ∫ Ψ1dt, and the corresponding velocity generated by Ψ1. Under any given circumstances as to constraint, the velocity and the impulse are in proportion to one another; and the resulting kinetic energy T is proportional to the square of either, being equal to ½ Ψ1 ∫Ψ1dt.

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Scientific Papers , pp. 475 - 485
Publisher: Cambridge University Press
Print publication year: 2009
First published in: 1900

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