Abstract

In this work, we construct the lumped Galerkin approach based on cubic B-splines to obtain the numerical solution of the generalized regularized long wave equation. Applying the von Neumann approximation, it is shown that the linearized algorithm is unconditionally stable. The presented method is implemented to three test problems including single solitary wave, interaction of two solitary waves and development of an undular bore. To prove the performance of the numerical scheme, the error norms L_{2} and {L_{infty}} and the conservative quantities {I_{1}}, {I_{2}} and {I_{3}} are computed and the computational data are compared with the earlier works. In addition, the motion of solitary waves is described at different time levels.

Highlights

  • The generalized regularized long wave (GRLW) equation, which discussed here, is based upon the regularized long wave (RLW) equation

  • The equal width (EW) wave equation was used by Morrison et al (1984) as an alternative model to the RLW equation

  • The GRLW equation is related to the generalized equal width (GEW) wave equation and the generalized Korteweg-de Vries (GKdV) equation

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Summary

Background

The generalized regularized long wave (GRLW) equation, which discussed here, is based upon the regularized long wave (RLW) equation. Esen and Kutluay (2006) obtained the numerical solution of the RLW equation with lumped Galerkin method using quadratic B-spline. Finite element methods based on quintic, cubic and septic collocation were used for obtaining the numerical solution of the MRLW equation by Gardner et al (1997), Khalifa et al (2008) and Karakoç et al (2014). Roshan (2012) and Mohammadi (2015) have got the numerical results of the GRLW equation using finite element method based on Petrov Galerkin and exponential B-spline collocation. Numerical examples and results we have applied the lumped Galerkin method to three test problems including single solitary wave, interaction of two solitary waves and development of an undular bore These three examples are formed by using different values of initial condition.

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