Abstract
Mechanics, as we studied it in the first three chapters, is based on two fundamental principles. On the one hand one makes use of simple functions such as the Lagrangian function and of functionals such as the action integral whose properties are clear and easy to grasp. In general, Lagrangian and Hamiltonian functions do not represent quantities that are directly measurable. However, they allow us to derive the equations of motion in a general and simple way. Also, they exhibit the specific symmetries of a given dynamical system more clearly than the equations of motion themselves, whose form and transformation properties are usually complicated.
Access this chapter
Tax calculation will be finalised at checkout
Purchases are for personal use only
Preview
Unable to display preview. Download preview PDF.
Bibliography
Hagedorn, R.: Relativistic Kinematics ( Benjamin, New York 1963 )
Jackson, J.D.: Classical Electrodynamics ( Wiley, New York 1975 )
Sexl, R.U., Urbantke, H.K.: Relativität, Gruppen, Teilchen (Springer, Berlin, Heidelberg 1976 )
Weinberg, S.: Gravitation and Cosmology, Principles and Applications of the General Theory of Relativity ( Wiley, New York 1972 )
Author information
Authors and Affiliations
Rights and permissions
Copyright information
© 1990 Springer-Verlag Berlin Heidelberg
About this chapter
Cite this chapter
Scheck, F.A. (1990). Relativistic Mechanics. In: Mechanics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-02630-4_4
Download citation
DOI: https://doi.org/10.1007/978-3-662-02630-4_4
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-540-52715-2
Online ISBN: 978-3-662-02630-4
eBook Packages: Springer Book Archive