scholarly journals Homotopic mapping solution of soliton for perturbed KdV equation

2008 ◽  
Vol 57 (12) ◽  
pp. 7419
Author(s):  
Mo Jia-Qi ◽  
Yao Jing-Sun
Open Physics ◽  
2010 ◽  
Vol 8 (4) ◽  
Author(s):  
Octavio Cornejo-Pérez ◽  
Haret Rosu

AbstractIn this paper, we obtain some new explicit travelling wave solutions of the perturbed KdV equation through recent factorization techniques that can be performed when the coefficients of the equation fulfill a certain condition. The solutions are obtained by using a two-step factorization procedure through which the perturbed KdV equation is reduced to a nonlinear second order differential equation, and to some Bernoulli and Abel type differential equations whose solutions are expressed in terms of the exponential andWeierstrass functions.


2000 ◽  
Vol 64 (4) ◽  
pp. 475-480 ◽  
Author(s):  
M. A. ALLEN ◽  
G. ROWLANDS

We derive the approximate form and speed of a solitary-wave solution to a perturbed KdV equation. Using a conventional perturbation expansion, one can derive a first-order correction to the solitary-wave speed, but at the next order, algebraically secular terms appear, which produce divergences that render the solution unphysical. These terms must be treated by a regrouping procedure developed by us previously. In this way, higher-order corrections to the speed are obtained, along with a form of solution that is bounded in space. For this particular perturbed KdV equation, it is found that there is only one possible solitary wave that has a form similar to the unperturbed soliton solution.


1995 ◽  
Vol 05 (04) ◽  
pp. 1221-1233 ◽  
Author(s):  
X. TIAN ◽  
R. H. J. GRIMSHAW

Spatial chaos has been observed in the steady state from a numerical study of a perturbed Korteweg–de Vries equation. The onset of chaos is due to a subharmonic bifurcation sequence. A second route to chaos is also observed via a period-doubling sequence generated from each fundamental subharmonic state. In this paper, the question of determining low-dimensional chaos in this perturbed KdV equation is addressed. The dimension of this system in the steady state is estimated from the corresponding ordinary differential equation via the Lyapunov spectrum, and also from a numerical investigation via a reconstructed attractor using a spatial series.


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