Gravitational perturbation

Definition and stakes

Portrait of Henry Andrews Bumstead Henry Andrews Bumstead,  Applications of the Lorentz-FitzGerald Hypothesis to Dynamical and Gravitational Problems (1908)

“ The maximum effect is of the same order as would be produced by a perturbing body at a distance equal to that of the sun, and whose mass was only that of the earth. The perturbation, moreover, would be periodic, vanishing at perihelion and aphelion and accelerating the earth's motion in one-half the orbit, retarding it in the other half.
When the sun is also moving, the problem becomes more complicated. For the present purpose it will be sufficient to obtain the order of magnitude of the acceleration perpendicular to the radius vector.
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Source: Wikisource

Aram D'Abro,  The evolution of scientific thought from Newton to Einstein (1927)

“ Our inability to differentiate between a field of inertial forces generated by acceleration and one of gravitation generated by matter is due solely to a miraculous coincidence, that of the equality of the two masses. Again, when, in the elevator falling in the earth’s gravitational field, we experience no feeling of weight, it is not that the gravitational field has vanished; it is solely that the field of gravity has been counteracted by an equal and opposite field of inertia generated by the elevator’s accelerated motion. ”
Source: Gutenberg

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