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A Study of Relative Motion in Connection with Classical Mechanics

H. Zanstra

  • Department of Physics, University of Minnesota

Phys. Rev. 23, 528 – Published 1 April, 1924

DOI: https://doi.org/10.1103/PhysRev.23.528

Abstract

Derivation of equations of motion of the second order, containing relative coordinates only.—This article is a continuation of the work of many authors, among others Berkeley, Neumann, Maxwell, Lange, Mach, Boltzmann, Föppl, and Kolkmeyer, whose work is briefly discussed. The main difficulty in Newton's mechanics seems to be to define the system of axes (inertial system) to which the motion is referred. Three solutions have been proposed. Föppl defined the system on a relative basis. Another and apparently more direct solution is to refer the motion of particles to other particles, that is, to use "relative coordinates" in the equations of motion. A third solution would be to obtain invariant equations, the same for all systems of reference. Introducing an hypothesis stated by Föppl, that for a system with its origin at the center of mass the angular momentum of the universe vanishes, invariant equations are obtained from the Newtonian, (though this is sometimes denied to be possible), and they degenerate into the Newtonian form if certain functions of coordinates and velocities occurring in them become zero by a suitable choice of the system of reference. It is believed, however, that such equations do not offer a complete solution of the problem of relativation of motion so as to satisfy the physicist; whereas the introduction of relative coordinates does. In this article this second solution has been applied to the Newtonian theory. Equations of motion are derived by introducing Föppl's hypothesis, which are of the second order and contain relative coordinates only. These equations may be taken as the basis for a complete system of mechanics. As examples the systems of Ptolemy and of Kepler are worked out.

Application of relative coordinates to Einstein's theory of gravitation.—It is believed that the possibility of introducing relative coordinates is not limited to the Newtonian theory. As an example of the application of these coordinates to Einstein's theories, the case of the motion of a heavy and a light particle is considered and it is suggested that an hypothesis similar to Föppl's may give equations of motion into which only the distance apart of the particles measured by an observer on the heavier, enters.

References (15)

  1. A. Föppl, Vorlesungen über technische Mechanik, VI, Erster Abschnitt, Die relative Bewegung
  2. N. H. Kolkmeyer. Eliminatie van de begrippen assenstelsel, lengte en tijd uit de vergelijkingèn voor de planetenbewegingen. Thesis Amsterdam 1915
  3. Omitted endnote

  4. Omitted endnote

  5. Zanstra, Proc. Kon. Acad. van Wet., Amsterdam 23, 1421, 1921 Ann. der Physik (IV) 70, 153, 1923
  6. L. Lange, Geschichtliche Entwickelung des Bewegungsbegriffs E. Mach, Die Mechanik in ihrerEntwickelung Enzyklopedie der Math. Wiss. VI 1, p. 30
  7. G. Berkeley, The Principles of Human Knowledge, Sections 111
  8. L. Lange. loc. cit.[6]
  9. C. Neumann, Ueber die Prinzipien der Galilei-Newtonschen Mechanik
  10. Omitted endnote

  11. H. Seeliger, Sitz. Math. Phys. Kl. Bayr. Acad. Wiss. 36, 85, 1906
  12. Boltzmann. Vorlesungen über die Prinzipien der Mechanik. Leipzig 1904 C. Neumann[9]
  13. A. Föppl, Vorlesungen über technische Mechanik, VI, Erster Abschnitt, Die relative Bewegung
  14. N. H. Kolkmeyer, Eliminatie van de begrippen assenstelsel, lengte en tijd uit de vergelijkingen voor de planetenbewegingen, Thesis, Amsterdam, 1915
  15. K. Schwarzschild, Sitz. Preus. Akad. der Wiss., Berlin 1916, p. 189

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