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Relativity: The Special and General Theory

Page 52 of 95, printed 52

[15] The objection is of importance more especially when the state of motion of the reference-body is of such a nature that it does not require any external agency for its maintenance, _e.g._ in the case when the reference-body is rotating uniformly. XXII. A FEW INFERENCES FROM THE GENERAL PRINCIPLE OF RELATIVITY The considerations of Section XX show that the general principle of relativity puts us in a position to derive properties of the gravitational field in a purely theoretical manner. Let us suppose, for instance, that we know the space-time course for any natural process whatsoever, as regards the manner in which it takes place in the Galileian domain relative to a Galileian body of reference _K_. By means of purely theoretical operations (_i.e._ simply by calculation) we are then able to find how this known natural process appears, as seen from a reference-body _K _ which is accelerated relatively to _K_. But since a gravitational field exists with respect to this new body of reference _K _, our consideration also teaches us how the gravitational field influences the process studied. For example, we learn that a body which is in a state of uniform rectilinear motion with respect to _K_ (in accordance with the law of Galilei) is executing an accelerated and in general curvilinear motion with respect to the accelerated reference-body _K _ (chest). This acceleration or curvature corresponds to the influence on the moving body of the gravitational field prevailing relatively to _K_. It is known that a gravitational field influences the movement of bodies in this way, so that our consideration supplies us with nothing essentially new. However, we obtain a new result of fundamental importance when we carry out the analogous consideration for a ray of light. With respect to the Galileian reference-body _K_, such a ray of light is transmitted rectilinearly with the velocity _c_. It can easily be shown that the path of the same ray of light is no longer a straight line when we consider it with reference to the accelerated chest (reference-body 52
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