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.