Hostname: page-component-77c89778f8-7drxs Total loading time: 0 Render date: 2024-07-19T11:29:56.068Z Has data issue: false hasContentIssue false

Note on the harmonic oscillator in general relativity

Published online by Cambridge University Press:  09 April 2009

N. W. Taylor
Affiliation:
Department of Mathematics, University of New England, Armidale, New South Wales.
Rights & Permissions [Opens in a new window]

Extract

Core share and HTML view are not available for this content. However, as you have access to this content, a full PDF is available via the ‘Save PDF’ action button.

The theory of relativity shows that the times measured by two observers will in general be different if they are in relative motion, so that their respective times between any two coincidences will differ. Bergmann [1] has investigated the problem of a particle moving in a small simple harmonic motion in a static gravitational field, and has found that the time difference for this particle and an observer at rest becomes zero whenever the particle passes through the centre and limits of its swing. This problem will now be dealt with in a different manner, using Schwarzschild's interior solution of the gravitational equations. The exterior solution for a point mass is not suitable in the present case, due to the singularity of the field at a point in the path of the particle.

Type
Research Article
Copyright
Copyright © Australian Mathematical Society 1961

References

[1]Bergmann, O., “Einige Bemerkungen zum Uhrenparadox”, Acta Physica Austriaca, XI (1957), 377389.Google Scholar
[2]Møller, C., The Theory of Relativity, Oxford, (1952), p. 330.Google Scholar