Paul Ehrenfest,
Translation:The Translation of Deformable Electrons and the Theorem of Conservation of Angular…
(1907)
“ Yet it is only necessary to sacrifice the latter theorem too, as we already sacrificed the energy theorem – then we are able to define any desired apparent mass of the Lorentz electron, thus one can bring any measuring result in agreement with the relativity principle. (However, the value of zero for the apparent mass offers itself as the most simple one; like a macroscopic condenser shall obtain no increase of mass by a charge according to relativity theory.) ”
