Hamilton-Jacobi approach for power-law potentials
The classical and relativistic Hamilton-Jacobi approach is applied to the one-dimensional homogeneous potential, V(q) = alphaq n, where alpha and n are continuously varying parameters. In the non-relativistic case, the exact analytical solution is determined in terms of alpha, n and the total energy E. It is also shown that the non-linear equation of motion can be linearized by constructing a hypergeometric differential equation for the inverse problem t(q). A variable transformation reducing the general problem to that one of a particle subjected to a linear force is also established. For any value of n, it leads to a simple harmonic oscillator if E > 0, an "anti-oscillator" if E < 0, or a free particle if E = 0. However, such a reduction is not possible in the relativistic case. For a bounded relativistic motion, the first order correction to the period is determined for any value of n. For n >> 1, it is found that the correction is just twice that one deduced for the simple harmonic oscillator (n = 2), and does not depend on the specific value of n.
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Sociedade Brasileira de Física
2006
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oai:scielo:S0103-973320060007000242007-06-21Hamilton-Jacobi approach for power-law potentialsSantos,R. C.Santos,J.Lima,J. A. S. Hamilton-Jacobi equation Power-law potentials The classical and relativistic Hamilton-Jacobi approach is applied to the one-dimensional homogeneous potential, V(q) = alphaq n, where alpha and n are continuously varying parameters. In the non-relativistic case, the exact analytical solution is determined in terms of alpha, n and the total energy E. It is also shown that the non-linear equation of motion can be linearized by constructing a hypergeometric differential equation for the inverse problem t(q). A variable transformation reducing the general problem to that one of a particle subjected to a linear force is also established. For any value of n, it leads to a simple harmonic oscillator if E > 0, an "anti-oscillator" if E < 0, or a free particle if E = 0. However, such a reduction is not possible in the relativistic case. For a bounded relativistic motion, the first order correction to the period is determined for any value of n. For n >> 1, it is found that the correction is just twice that one deduced for the simple harmonic oscillator (n = 2), and does not depend on the specific value of n.info:eu-repo/semantics/openAccessSociedade Brasileira de FísicaBrazilian Journal of Physics v.36 n.4a 20062006-12-01info:eu-repo/semantics/articletext/htmlhttp://old.scielo.br/scielo.php?script=sci_arttext&pid=S0103-97332006000700024en10.1590/S0103-97332006000700024 |
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Santos,R. C. Santos,J. Lima,J. A. S. |
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Santos,R. C. Santos,J. Lima,J. A. S. Hamilton-Jacobi approach for power-law potentials |
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Santos,R. C. Santos,J. Lima,J. A. S. |
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Santos,R. C. |
title |
Hamilton-Jacobi approach for power-law potentials |
title_short |
Hamilton-Jacobi approach for power-law potentials |
title_full |
Hamilton-Jacobi approach for power-law potentials |
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Hamilton-Jacobi approach for power-law potentials |
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Hamilton-Jacobi approach for power-law potentials |
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hamilton-jacobi approach for power-law potentials |
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The classical and relativistic Hamilton-Jacobi approach is applied to the one-dimensional homogeneous potential, V(q) = alphaq n, where alpha and n are continuously varying parameters. In the non-relativistic case, the exact analytical solution is determined in terms of alpha, n and the total energy E. It is also shown that the non-linear equation of motion can be linearized by constructing a hypergeometric differential equation for the inverse problem t(q). A variable transformation reducing the general problem to that one of a particle subjected to a linear force is also established. For any value of n, it leads to a simple harmonic oscillator if E > 0, an "anti-oscillator" if E < 0, or a free particle if E = 0. However, such a reduction is not possible in the relativistic case. For a bounded relativistic motion, the first order correction to the period is determined for any value of n. For n >> 1, it is found that the correction is just twice that one deduced for the simple harmonic oscillator (n = 2), and does not depend on the specific value of n. |
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Sociedade Brasileira de Física |
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2006 |
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http://old.scielo.br/scielo.php?script=sci_arttext&pid=S0103-97332006000700024 |
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AT santosrc hamiltonjacobiapproachforpowerlawpotentials AT santosj hamiltonjacobiapproachforpowerlawpotentials AT limajas hamiltonjacobiapproachforpowerlawpotentials |
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