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Mechanics pp 211-254 | Cite as

Relativistic Mechanics

  • Florian A. Scheck

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.

Keywords

Inertial Frame Lorentz Transformation Rest Mass World Line Inertial System 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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References

  1. Hagedorn, R.: Relativistic Kinematics (Benjamin, New York 1963)zbMATHGoogle Scholar
  2. Jackson, J.D.: Classical Electrodynamics (Wiley, New York 1975)zbMATHGoogle Scholar
  3. Sexl, R.U., Urbantke, H.K.: Relativität, Gruppen, Teilchen (Springer, Berlin, Heidelberg 1976)Google Scholar
  4. Weinberg, S.: Gravitation and Cosmology, Principles and Applications of the General Theory of Relativity (Wiley, New York 1972)Google Scholar

Copyright information

© Springer-Verlag Berlin Heidelberg 1994

Authors and Affiliations

  • Florian A. Scheck
    • 1
  1. 1.Institut für Physik, Theoretische ElementarteilchenphysikJohannes Gutenberg-UniversitätMainzGermany

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