Asymptotic stability of a pendulum with quadratic damping

The equation considered in this paper is x ′ ′ + h ( t ) x ′ | x ′ | + ω 2 sin x = 0 , where h ( t ) is continuous and nonnegative for t ≥ 0 and ω is a positive real number. This may be regarded as an equation of motion of an underwater pendulum. The damping force is proportional to the square of th...

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Bibliographic Details
Published inZeitschrift für angewandte Mathematik und Physik Vol. 65; no. 5; pp. 865 - 884
Main Author Sugie, Jitsuro
Format Journal Article
LanguageEnglish
Published Basel Springer Basel 01.10.2014
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ISSN0044-2275
1420-9039
DOI10.1007/s00033-013-0361-x

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Summary:The equation considered in this paper is x ′ ′ + h ( t ) x ′ | x ′ | + ω 2 sin x = 0 , where h ( t ) is continuous and nonnegative for t ≥ 0 and ω is a positive real number. This may be regarded as an equation of motion of an underwater pendulum. The damping force is proportional to the square of the velocity. The primary purpose is to establish necessary and sufficient conditions on the time-varying coefficient h ( t ) for the origin to be asymptotically stable. The phase plane analysis concerning the positive orbits of an equivalent planar system to the above-mentioned equation is used to obtain the main results. In addition, solutions of the system are compared with a particular solution of the first-order nonlinear differential equation u ′ + h ( t ) u | u | + 1 = 0 . Some examples are also included to illustrate our results. Finally, the present results are extended to be applied to an equation with a nonnegative real-power damping force.
ISSN:0044-2275
1420-9039
DOI:10.1007/s00033-013-0361-x