By Petr Hájíček (auth.)

ISBN-10: 3540786589

ISBN-13: 9783540786580

The geometric interpretation of gravitation is likely one of the significant foundations of contemporary theoretical physics. This primer introduces classical common relativity with emphasis at the readability of conceptual constitution and at the simple mathematical the way to increase systematically program abilities. The wealth of actual phenomena entailed by means of the Einstein‘s equations is published with the aid of particular versions describing gravitomagnetism, gravitational waves, cosmology, gravitational cave in and black holes. End-of-chapter workouts entire the most text.

This ebook is predicated on class-tested notes for classes which have been held by means of the writer over a long time on the college of Bern, the place Einstein labored on the neighborhood patent workplace and the place the rules of certain relativity have been laid.

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**Additional resources for An Introduction to the Relativistic Theory of Gravitation**

**Sample text**

1, −1, . . , −1) with n+ -times +1 and n− -times −1, where Diag(a1 , . . , an ) is an abbreviation for the diagonal matrix with the elements a1 , . . , an sitting on the diagonal, then the metric has the signature σ = n+ − n− in p. ) The signature does not depend on the way the metric is transformed to the above diagonal form. This is because the transformation of the metric at a point p is a real general linear transformation: ρ gμν (p) = Xμ (p) Xνσ (p)gρσ (p) . It is known from linear algebra [4] that every symmetric matrix can be brought by such a transformation to the form Diag(+1, .

The components of the curvature tensor thus denote a difference in the acceleration of the freely falling system in different points. On the Earth we perceive such relative accelerations, for instance in the field of the Moon. They evoke forces which produce tides. This is why it is sometimes said that the curvature tensor of general relativity describes tidal forces. It is also true in general that the components of the curvature tensor of an arbitrary affine connection contain information about the relative acceleration of its autoparallels.

I. M. Gel’fand, Lectures on Linear Algebra. Interscience Publishers, New York, 1961. 19 10. E. Cartan, Ann. Ecole Norm. Sup. 40 (1923) 325; 41 (1924) 1. 23 11. L. P. Eisenhart, Riemannian Geometry. Princeton University Press, Princeton, NJ, 1949. 1 Relativistic Gravity In Chap. 1 we learned that Newtonian gravitation can be considered as a geometry of space–time. In addition we learned the fundamentals of the corresponding mathematical apparatus, differential geometry. In this chapter we want to apply those methods to relativistic particle dynamics.

### An Introduction to the Relativistic Theory of Gravitation by Petr Hájíček (auth.)

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