scholarly journals Symmetry Classification of Third-Order Nonlinear Evolution Equations. Part I: Semi-simple Algebras

2012 ◽  
Vol 124 (1) ◽  
pp. 123-170 ◽  
Author(s):  
P. Basarab-Horwath ◽  
F. Güngör ◽  
V. Lahno

2004 ◽  
Vol 45 (6) ◽  
pp. 2280-2313 ◽  
Author(s):  
F. Güngör ◽  
V. I. Lahno ◽  
R. Z. Zhdanov


2011 ◽  
Vol 54 (12) ◽  
pp. 2553-2572 ◽  
Author(s):  
ShouFeng Shen ◽  
ChangZheng Qu ◽  
Qing Huang ◽  
YongYang Jin


2016 ◽  
Vol 2016 ◽  
pp. 1-39 ◽  
Author(s):  
V. O. Vakhnenko ◽  
E. J. Parkes

A variety of methods for examining the properties and solutions of nonlinear evolution equations are explored by using the Vakhnenko equation (VE) as an example. The VE, which arises in modelling the propagation of high-frequency waves in a relaxing medium, has periodic and solitary traveling wave solutions some of which are loop-like in nature. The VE can be written in an alternative form, known as the Vakhnenko-Parkes equation (VPE), by a change of independent variables. The VPE has anN-soliton solution which is discussed in detail. Individual solitons are hump-like in nature whereas the corresponding solution to the VE comprisesN-loop-like solitons. Aspects of the inverse scattering transform (IST) method, as applied originally to the KdV equation, are used to find one- and two-soliton solutions to the VPE even though the VPE’s spectral equation is third-order and not second-order. A Bäcklund transformation for the VPE is used to construct conservation laws. The standard IST method for third-order spectral problems is used to investigate solutions corresponding to bound states of the spectrum and to a continuous spectrum. This leads toN-soliton solutions andM-mode periodic solutions, respectively. Interactions between these types of solutions are investigated.



1985 ◽  
Vol 34 (3) ◽  
pp. 303-311 ◽  
Author(s):  
V.P. Gerdt ◽  
A.B. Shvachka ◽  
A.Yu. Zharkov








Sign in / Sign up

Export Citation Format

Share Document