Henry Andrews Bumstead,
Applications of the Lorentz-FitzGerald Hypothesis to Dynamical and Gravitational Problems
(1908)
“ In the special case before us, the principle of relativity relieves us entirely from the difficulty of even these small variations from the Newtonian law. This is apparent from the general statement of the principle; but it is of some interest to see how the matter works out in detail. What is subject to observation is not the force but the acceleration; if we let and be the components of the acceleration parallel and perpendicular to the common motion of the two bodies, we shall have and the resultant of these is along so that there is no aberration of the acceleration. ”
