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Fifth-order Korteweg–de Vries equation : ウィキペディア英語版
Fifth-order Korteweg–de Vries equation
A fifth-order Korteweg–de Vries (KdV) equation is a nonlinear partial differential equation in 1+1 dimensions related to the Korteweg–de Vries equation.〔Andrei D. Polyanin, Valentin F. Zaitsev, HANDBOOK of NONLINEAR PARTIAL DIFFERENTIAL EQUATIONS, SECOND EDITION p 1034, CRC PRESS〕 Fifth order KdV equations may be used to model dispersive phenomena such as plasma waves when the third-order contributions are small. The term may refer to equations of the form
: u_+\alpha u_+\beta u_ = \frac f(u, u_, u_)
where f is a smooth function and \alpha and \beta are real with \beta \neq 0. Unlike the KdV system, it is not integrable. It admits a great variety of soliton solutions.〔(【引用サイトリンク】 title=Stability and instability of solitary waves of the fifth-order KdV equation: a numerical framework )
==References==


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