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Brachistochrone in almost flat space

Journal Article · · J. Math. Phys. (N.Y.); (United States)
DOI:https://doi.org/10.1063/1.528158· OSTI ID:6904590

This paper is an extension, within the framework of general relativity, of the relativistic brachistochrone discussed recently by Goldstein and Bender (J. Math. Phys. 27, 507 (1986)). Assuming that the gravitational field due to a spherically symmetric source with mass M at equilibrium is weak, it is found that the brachistochrone, for a falling particle of mass m, described by THETA(r), with THETA an angle and r a distance measured from the center of symmetry, is in general a hyperelliptic integral. The latter integral can in one case be calculated exactly in terms of the normal elliptic integrals of the first and third kinds and the elementary transcendental functions. It is shown via a numerical computation using the sun's gravitational field as a reference that one can recast this exact version into a simple form, viz., (r)/sup 1/2/THETA = a, where a is a constant.

Research Organization:
Department of Mathematics, Indian Institute of Technology, Madras 600 036, India
OSTI ID:
6904590
Journal Information:
J. Math. Phys. (N.Y.); (United States), Journal Name: J. Math. Phys. (N.Y.); (United States) Vol. 29:10; ISSN JMAPA
Country of Publication:
United States
Language:
English

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