Richard Chace Tolman, Some Emission Theories of Light (1912)
“ All emission theories agree in assuming that light from a moving source has a velocity equal to the vector sum of the velocity of light from a stationary source and the velocity of the source itself at the instant of emission. Thus a source in uniform motion would always remain at the center of the spherical disturbances which it emits, these disturbances moving relative to the source itself with the same velocity c as from a stationary source. [1] Emission theories differ, however, in their assumptions as to the velocity of light after its reflection from a mirror. ”
