Abstract
We shall start with a short review of the prerelativistic mechanics of Newton, Lagrange, and Hamilton. For simplicity we restrict ourselves to systems of a single-point particle having (constant) mass m > 0. Let the parameterized motion curve be given by xα = X α(t), in the Euclidean space E3. Let the three components of the force vector be given by f α(t, x, v), which are functions of seven real variables. Here t stands for the time variable, x = (x1,x2, x3) are the spatial coordinates in a Cartesian coordinate system, and v = (v1, v2, v3) are the velocity variables.
Access this chapter
Tax calculation will be finalised at checkout
Purchases are for personal use only
Preview
Unable to display preview. Download preview PDF.
References
P. G. Bergman, Introduction to the Theory of Relativity, Prentice-Hall, New Jersey, 1942. [pp. 134, 158]
P. A. M. Dirac, Canad. J. Math. 2 (1950), 129–148.
I. M. Gelfand and S. V. Fomin, Calculus of variations, Prentice-Hall, New Jersey, 1963. [p. 128]
C. Lanczos, The variational principles of mechanics, University of Toronto Press, Toronto, 1977. [pp. 126, 128, 131, 134, 136, 137]
J. L. Synge, Relativity: The special theory, North-Holland, Amsterdam, 1964. [pp. 141, 145, 147, 150]
—, Classical dynamics, Reprint from Handbuch der Physik, Springer-Verlag, Berlin, 1960. [p. 157]
Author information
Authors and Affiliations
Rights and permissions
Copyright information
© 1993 Springer Science+Business Media New York
About this chapter
Cite this chapter
Das, A. (1993). The Special Relativistic Mechanics. In: The Special Theory of Relativity. Universitext. Springer, New York, NY. https://doi.org/10.1007/978-1-4612-0893-8_5
Download citation
DOI: https://doi.org/10.1007/978-1-4612-0893-8_5
Publisher Name: Springer, New York, NY
Print ISBN: 978-0-387-94042-7
Online ISBN: 978-1-4612-0893-8
eBook Packages: Springer Book Archive