We have deduced the kinematics corresponding to our two fundamental principles for the laws necessary for us, and we shall now pass over to their application in electrodynamics.
II.—ELECTRODYNAMICAL PART.
§ 6. Transformation of Maxwell’s equations for Pure Vacuum.
On the nature of the Electromotive Force caused by motion in a magnetic field.
The Maxwell-Hertz equations for pure vacuum may hold for the stationary system K, so that
and
"Equation 1."