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nydus/Relativity: The Special and General TheoryPublic

Albert Einstein provides a non-mathematical exposition of the special and general theories of relativity for readers interested in physics and philosophy. The text presents the core concepts in their original sequence and aims to explain the theories as simply as possible for those with a standard university-level education.

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Table of Contents

VII

of light must necessarily hold with respect

to the carriage–-a result contradictory to the principle of relativity.

In view of this dilemma there appears to be nothing else for it than to abandon either the principle of relativity

or the simple law of the propagation of light in vacuo. Those of you who have carefully followed the preceding discussion are almost sure to expect that we should retain the principle of relativity, which appeals so convincingly to the intellect because it is so natural and simple. The law of the propagation of light in vacuo would then have to be replaced by a more complicated law conformable to the principle of relativity. The development of theoretical physics shows, however, that we cannot pursue this course. The epoch-making theoretical investigations of H. A. Lorentz on the electrodynamical and optical phenomena

connected with moving bodies show that experience in this domain leads conclusively to a theory of electromagnetic phenomena, of which the law of the constancy of the velocity of light in vacuo is a necessary consequence. Prominent theoretical physicists were therefore more inclined to reject the principle of relativity, in spite of the fact that no empirical data had been found which were contradictory to this principle.

At this juncture the theory of relativity entered the arena. As a result of an analysis of the physical conceptions of time and space, it became evident that in

reality there is not the least incompatibility between the

principle of relativity and the law of propagation of light,

and that by systematically holding fast to both these laws a logically rigid theory could be arrived at. This theory has been called the special theory of relativity

to distinguish it from the extended theory, with which we shall deal later. In the following pages we shall present the fundamental ideas of the special theory of relativity.

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