Page:A Treatise on Electricity and Magnetism - Volume 2.djvu/438

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406
MAGNETIC ACTION ON LIGHT.
[818.

satisfy the equations, one positive and the other negative, the positive value being numerically greater than the negative.

818.] We may obtain the equations of motion from a consideration of the potential and kinetic energies of the medium. The potential energy, , of the system depends on its configuration, that is, on the relative position of its parts. In so far as it depends on the disturbance due to circularly-polarized light, it must be a function of , the amplitude, and , the coefficient of torsion, only. It may be different for positive and negative values of of equal numerical value, and it probably is so in the case of media which of themselves rotate the plane of polarization.

The kinetic energy, , of the system is a homogeneous function of the second degree of the velocities of the system, the coefficients of the different terms being functions of the coordinates.

819.] Let us consider the dynamical condition that the ray may be of constant intensity, that is, that may be constant.

Lagrange's equation for the force in becomes


.(5)

Since is constant, the first term vanishes. We have therefore the equation


,(6)

in which is supposed to be given, and we are to determine the value of the angular velocity , which we may denote by its actual value, .

The kinetic energy, , contains one term involving ; other terms may contain products of with other velocities, and the rest of the terms are independent of . The potential energy, , is entirely independent of . The equation is therefore of the form


.(7)

This being a quadratic equation, gives two values of . It appears from experiment that both values are real, that one is positive and the other negative, and that the positive value is numerically the greater. Hence, if is positive, both and are negative, for, if and are the roots of the equation,


.(8)

The coefficient, , therefore, is not zero, at least when magnetic force acts on the medium. We have therefore to consider the expression , which is the part of the kinetic energy involving the first power of , the angular velocity of the disturbance.