Summary

Emil Cohn Translation:On the Electrodynamics of Moving Systems II (1904)

Everywhere, where the propagation of radiation is not the object of measurement, we define identical moments of time at different points of Earth's surface, by treating the propagation of light as timeless. In optics, however, we define these identical moments of time by assuming, that the propagation takes place in spherical waves for every relatively resting and isotropic medium. [5] This means: the "time" which actually serves us for the representation of terrestrial process, is the "local time" , for which the equations I'b to IVb hold, – not the "general time" .
Source: Wikisource

Emil Cohn Translation:On the Electrodynamics of Moving Systems II (1904)

Thus, also the consideration of mechanical forces verifies our earlier result: no experience hinders us, to arbitrarily relate our fundamental equations to a spatial reference system that is at rest in Earth, or to such a system that has an arbitrary uniform velocity, whose order is the relative velocity of Earth - fixed stars. We only have to adapt the temporal reference system to the freely chosen spatial system.
Source: Wikisource

Emil Cohn Translation:On the Electrodynamics of Moving Systems II (1904)

Everything said in this paragraph applies to media, which are in relative rest with respect to a reference system that itself has a uniform translational velocity. By assuming this references system as being fixed in Earth, we neglect the rotation of axis. Theoretically spoken, the requirement of uniform propagation of light in all directions relative to earth cannot be satisfied by any "local time", because the velocity of diurnal motion has no potential.
Source: Wikisource

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