Relativity: The Special and the General Theory
Albert Einstein
Adapted for Modern Readers
First published 1916 (German) · Lucid Classics edition 2026 · 129 pages
Original and Lucid edition, side by side
Lawson translation, 1920
In your schooldays most of you who read this book made acquaintance with the noble building of Euclid's geometry, and you remember—perhaps with more respect than love—the magnificent structure, on the lofty staircase of which you were chased about for uncounted hours by conscientious teachers. By reason of your past experience, you would certainly regard everyone with disdain who should pronounce even the most out-of-the-way proposition of this science to be untrue. But perhaps this feeling of proud certainty would leave you immediately if some one were to ask you: "What, then, do you mean by the assertion that these propositions are true?" Let us proceed to give this question a little consideration.
Geometry sets out from certain conceptions such as "plane," "point," and "straight line," with which we are able to associate more or less definite ideas, and from certain simple propositions (axioms) which, in virtue of these ideas, we are inclined to accept as "true." Then, on the basis of a logical process, the justification of which we feel ourselves compelled to admit, all remaining propositions are shown to follow from those axioms, i.e. they are proven. A proposition is then correct ("true") when it has been derived in the recognised manner from the axioms. The question of the "truth" of the individual geometrical propositions is thus reduced to one of the "truth" of the axioms.
Lucid Classics
In school, most of you who read this book encountered Euclid's geometry — and you probably remember it with more respect than love: that magnificent structure up whose steep staircase you were driven for countless hours by conscientious teachers. Given that experience, you would almost certainly dismiss anyone who claimed that even the most obscure proposition of this science was false. But that feeling of confident certainty might vanish the moment someone asked you: “What exactly do you mean when you say these propositions are true?” Let us think about this.
Geometry starts from certain concepts — “plane,” “point,” “straight line” — with which we can associate more or less definite ideas, and from certain simple propositions (axioms) which, given those ideas, we feel compelled to accept as “true.” From those axioms, through a logical process whose validity we feel forced to grant, all the remaining propositions are shown to follow — that is, they are proven. A proposition is then correct (“true”) when it has been derived in the accepted way from the axioms. The question of whether any individual geometrical proposition is “true” thus reduces to the question of whether the axioms are “true.”
Lawson translation, 1920
Up to now our considerations have been referred to a particular body of reference, which we have styled a "railway embankment." We suppose a very long train travelling along the rails with the constant velocity v and in the direction indicated in Fig. 1. People travelling in this train will with advantage use the train as a rigid reference-body (co-ordinate system); they regard all events in reference to the train. Then every event which takes place along the line also takes place at a particular point of the train. Also the definition of simultaneity can be given relative to the train in exactly the same way as with respect to the embankment. As a natural consequence, however, the following question arises:
Lucid Classics
Up to now our considerations have been referred to a particular reference body, which we have called a “railway embankment.” We suppose a very long train traveling along the rails with the constant velocity in the direction indicated in the figure. People traveling in this train will find it convenient to use the train itself as a rigid reference body (coordinate system); they describe all events in reference to the train. Then every event that takes place along the line also takes place at a particular point of the train. The definition of simultaneity can also be given relative to the train in exactly the same way as with respect to the embankment. As a natural consequence, however, the following question arises:
Contents
- Preface
- Note to the Third Edition
- Biographical Note
- Translator's Note
- Physical Meaning of Geometrical Propositions
- The System of Coordinates
- Space and Time in Classical Mechanics
- The Galilean System of Coordinates
- The Principle of Relativity (In the Restricted Sense)
- The Theorem of the Addition of Velocities Employed in Classical Mechanics
- The Apparent Incompatibility of the Law of Propagation of Light with the Principle of Relativity
- On the Idea of Time in Physics
- The Relativity of Simultaneity
- On the Relativity of the Conception of Distance
- The Lorentz Transformation
- The Behavior of Measuring-Rods and Clocks in Motion
- Theorem of the Addition of Velocities: The Experiment of Fizeau
- The Heuristic Value of the Theory of Relativity
- General Results of the Theory
- Experience and the Special Theory of Relativity
- Minkowski's Four-Dimensional Space
- Special and General Principle of Relativity
- The Gravitational Field
- The Equality of Inertial and Gravitational Mass as an Argument for the General Postulate of Relativity
- In What Respects Are the Foundations of Classical Mechanics and of the Special Theory of Relativity Unsatisfactory?
- A Few Inferences from the General Principle of Relativity
- Behavior of Clocks and Measuring-Rods on a Rotating Body of Reference
- Euclidean and Non-Euclidean Continuum
- Gaussian Coordinates
- The Space-Time Continuum of the Special Theory of Relativity Considered as a Euclidean Continuum
- The Space-Time Continuum of the General Theory of Relativity Is Not a Euclidean Continuum
- Exact Formulation of the General Principle of Relativity
- The Solution of the Problem of Gravitation on the Basis of the General Principle of Relativity
- Cosmological Difficulties of Newton's Theory
- The Possibility of a “Finite” and Yet “Unbounded” Universe
- The Structure of Space According to the General Theory of Relativity
- Simple Derivation of the Lorentz Transformation
- Minkowski's Four-Dimensional Space (“World”)
- The Experimental Confirmation of the General Theory of Relativity