Page:BatemanElectrodynamical.djvu/39

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From this we may obtain the reciprocal invariant

where

(3)

Multiplying these and rejecting the invariant factor , we obtain the invariant

(4)

Multiplying

by

we obtain the invariant

(5)

We now assume that

is an invariant multiple of this invariant. This gives the relation

or

(6)

The constitutive relations are of the type

(7)

and can be expressed in terms of E and B by means of the relations connecting these quantities with D and H.