\centerline{\bf A Numerical Treatment of K(2,3) Kdv Type Equation} \ms \ms \baselineskip=15 pt \centerline{\bf M. S. Ismail} \centerline{Department of Mathematics} \centerline{College of Science} \centerline{P.O.Box 9028} \centerline{Jeddah-21413} \centerline{Saudi Arabia} \centerline{E-mail SCF 3005 @ KAAU.EDU.SA} \baselineskip=19pt \ms \ms {\bf Keywords: Finite difference method, PDEs, Compacton} \ms \ms \ms \centerline{\bf ABSTRACT} \ms The Koetewege-de Vries (Kdv) equation has recently been generalized by Rosenau and Hyman 1 to a class of partial differential equations (PDEs) which has solitary wave solution with compact support. These solitary wave solutions are called compactons. Compactons are solitary waves with the remarkable soliton property, that after colliding with other compactons, they reemerge with the same coherent shape. These particle-like waves exhibit elastic collision that are similar to the soliton interaction associated with completely integrable systems. The point where two compactons collide is marked by a creation of low amplitude compacton-anti compacton pairs. These equations have only a finite number of local conservation Laws. \ms \par In this paper, an implicit Numerical solution has been developed to solve the K(2,3) equation. Accuracy and stability of the method have been studied. The analytical solution and the conserved quantities are used to assess the accuracy of the numerical method. The numerical results have shown that this compacton exhibits true soliton behavior. \ms \ms \centerline{\bf REFERENCE} \ms \item{1.} R. Rosenau, J. M. Hyman: Compactons: Solitons with finite wave lengths, Phys. Rev. Lett., 70, No. 5, P. 564(1993) \vfill\eject \end{document}