A group theoretical identification of integrable equations in the Lienard-type equation x···+f(x) x···+g(x) = 0. II. Equations having maximal Lie point symmetries

Pandey, S. N. ; Bindu, P. S. ; Senthilvelan, M. ; Lakshmanan, M. (2009) A group theoretical identification of integrable equations in the Lienard-type equation x···+f(x) x···+g(x) = 0. II. Equations having maximal Lie point symmetries Journal of Mathematical Physics, 50 (10). 102701_1-102701_25. ISSN 0022-2488

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Official URL: http://jmp.aip.org/resource/1/jmapaq/v50/i10/p1027...

Related URL: http://dx.doi.org/10.1063/1.3204075

Abstract

In this second of the set of two papers on Lie symmetry analysis of a class of Lienard-type equation of the form x···+f(x) x···+g(x) = 0, where overdot denotes differentiation with respect to time and f(x) and g(x) are smooth functions of their variables, we isolate the equations which possess maximal Lie point symmetries. It is well known that any second order nonlinear ordinary differential equation which admits eight parameter Lie point symmetries is linearizable to free particle equation through point transformation. As a consequence all the identified equations turn out to be linearizable. We also show that one can get maximal Lie point symmetries for the above Lienard equation only when fxx = 0 (subscript denotes differentiation). In addition, we discuss the linearizing transformations and solutions for all the nonlinear equations identified in this paper.

Item Type:Article
Source:Copyright of this article belongs to American Institute of Physics.
Keywords:Harmonic Oscillators; Lie Groups; Nonlinear Differential Equations
ID Code:85030
Deposited On:29 Feb 2012 07:03
Last Modified:19 May 2016 01:14

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