A formalism of integrating the equations of geodesics and of geodesic deviation is examined based upon the Hamilton–Jacobi equation for geodesics. The latter equation has been extended to the case of geodesic deviation and theorems analogous to Jacobi’s theorem on the complete integral has been proved. As a result, a straightforward algorithm of integrating the geodesic deviation equations on Riemannian (or pseudo‐Riemannian) manifolds is obtained.
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C. G. J. Jacobi’s Vorlesungen über Dynamik, edited by A. Clebsch (Reimer, Berlin, 1884).
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L. D. Landau and E. M. Lifschitz, The Classical Theory of Fields, translated by M. Hamermesh, 3rd English ed. (Pergamon, Oxford, 1971).
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C. W. Misner, K. S. Thorne, and J. A. Wheeler, Gravitation (Freeman, San Francisco, 1973).
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See, e.g., S. W. Hawking and G. F. R. Ellis, The Large Scale Structure of Space‐time (Cambridge U.P., Cambridge, 1973), p. 106.
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In the notation adopted here, the dependence of the functions on the function f will be very often suppressed.
11.
Strictly speaking the most general function Φ should be of the form where f is an arbitrary function such that This more general case would lead to an equation analogous to Eq. (4.3), in which should be replaced For the sake of simplicity, however, the dependence of the functions f and λ on is in the sequel suppressed.
12.
S. L. Bażański, in Proceedings of the Fourth Marcel Grossman Meeting on General Relativity, edited by R. Ruffini (Elsevier, Amsterdam, 1986), p. 1615.
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S. L. Bażański and P. Jaranowski, to be published in J. Math. Phys.
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S. L. Bażański, to be published in Acta Phys. Pol.
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16.
Strictly speaking, this second transformation results in adding to the action an integral of a complete differential, which has no effect on the equations of motion.
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© 1989 American Institute of Physics.
1989
American Institute of Physics
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