High order compact solution of the one‐space‐dimensional linear hyperbolic equation

In this article, we introduce a high‐order accurate method for solving one‐space dimensional linear hyperbolic equation. We apply a compact finite difference approximation of fourth order for discretizing spatial derivative of linear hyperbolic equation and collocation method for the time component. The main property of this method additional to its high‐order accuracy due to the fourth order discretization of spatial derivative, is its unconditionally stability. In this technique the solution is approximated by a polynomial at each grid point that its coefficients are determined by solving a linear system of equations. Numerical results show that the compact finite difference approximation of fourth order and collocation method produce a very efficient method for solving the one‐space‐dimensional linear hyperbolic equation. We compare the numerical results of this paper with numerical results of (Mohanty, Appl Math Lett 17 (2004), 101–105) .© 2008 Wiley Periodicals, Inc. Numer Methods Partial Differential Eq 2008

[1]  Mehdi Dehghan,et al.  The dual reciprocity boundary element method (DRBEM) for two-dimensional sine-Gordon equation , 2008 .

[2]  M. Dehghan The one-dimensional heat equation subject to a boundary integral specification , 2007 .

[3]  Mehdi Dehghan,et al.  Numerical solution of the Klein–Gordon equation via He’s variational iteration method , 2007 .

[4]  Mehdi Dehghan,et al.  Multigrid solution of high order discretisation for three-dimensional biharmonic equation with Dirichlet boundary conditions of second kind , 2006, Appl. Math. Comput..

[5]  Mehdi Dehghan,et al.  Finite difference procedures for solving a problem arising in modeling and design of certain optoelectronic devices , 2006, Math. Comput. Simul..

[6]  M. Dehghan A computational study of the one‐dimensional parabolic equation subject to nonclassical boundary specifications , 2006 .

[7]  Mehdi Dehghan,et al.  Implicit Collocation Technique for Heat Equation with Non-Classic Initial Condition , 2006 .

[8]  R. K. Mohanty An unconditionally stable finite difference formula for a linear second order one space dimensional hyperbolic equation with variable coefficients , 2005, Appl. Math. Comput..

[9]  Mehdi Dehghan,et al.  On the solution of an initial‐boundary value problem that combines Neumann and integral condition for the wave equation , 2005 .

[10]  R. K. Mohanty An unconditionally stable difference scheme for the one-space-dimensional linear hyperbolic equation , 2004, Appl. Math. Lett..

[11]  Jules Kouatchou,et al.  Parallel implementation of a high-order implicit collocation method for the heat equation , 2001 .

[12]  J. Kouatchou Finite Differences and Collocation Methods for the Solution of the Two Dimensional Heat Equation , 2001 .

[13]  F. Jézéquel A validated parallel across time and space solution of the heat transfer equation , 1999 .

[14]  R. K. Mohanty,et al.  On the use of high order difference methods for the system of one space second order nonlinear hyperbolic equations with variable coefficients , 1996 .

[15]  Murli M. Gupta,et al.  High-Order Difference Schemes for Two-Dimensional Elliptic Equations , 1985 .

[16]  E. H. Twizell An explicit difference method for the wave equation with extended stability range , 1979 .