Page:A Treatise on Electricity and Magnetism - Volume 2.djvu/265

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614.]
CURRENTS OF DISPLACEMENT.
233

electromagnetic phenomena depend, is not the same thing as , the current of conduction, but that the time-variation of , the electric displacement, must be taken into account in estimating the total movement of electricity, so that we must write,


(H)

or, in terms of the components,


(H*)


611.] Since both and depend on the electromotive force , we may express the true current & in terms of the electromotive force, thus


(I)

or, in the case in which C and K are constants,


(I*)



612.] The volume-density of the free electricity at any point is found from the components of electric displacement by the equation


(J)


613.] The surface-density of electricity is


(K)

where l, m, n are the direction-cosines of the normal drawn from the surface into the medium in which f, g, h are the components of the displacement, and l', m', n' are those of the normal drawn from the surface into the medium in which they are f', g', h'.

614.] When the magnetization of the medium is entirely induced by the magnetic force acting on it, we may write the equation of induced magnetization,


(L)

where μ is the coefficient of magnetic permeability, which may be considered a scalar quantity, or a linear and vector function operating on , according as the medium is isotropic or not.