Abstract
In a previous paper by one of us it was shown that when an insulator of specific inductive capacity K rotates in a magnetic field there is an electromotive force induced in it equal to that in a conductor multiplied by 1 — K
-1
. The object of the experiments described below was to measure the induced electromotive force in a magnetic insulator rotating in a magnetic field parallel to the axis of rotation. According to the theory based on the “principle of relativity” this induced electromotive force should be equal to that in a conductor multiplied by 1 — (
μ
K)
-1
, where
μ
is the magnetic permeability of the insulator, whereas on the theory of H. A. Lorentz and Larmor the appropriate multiplier appears to be 1 — K
-1
, as for a non-magnetic insulator.
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