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Convergence of Finite Difference Scheme and Analytic Data
Author(s) -
Kantaro Hayakawa
Publication year - 1988
Publication title -
publications of the research institute for mathematical sciences
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.786
H-Index - 39
eISSN - 1663-4926
pISSN - 0034-5318
DOI - 10.2977/prims/1195174693
Subject(s) - mathematics , convergence (economics) , hyperbolic partial differential equation , partial differential equation , mathematical analysis , first order partial differential equation , differential equation , finite difference , finite difference method , ftcs scheme , rate of convergence , order of accuracy , wave equation , method of characteristics , ordinary differential equation , differential algebraic equation , economics , economic growth , channel (broadcasting) , engineering , electrical engineering
Finite difference methods are used widely to approximate solutions of partial differential equations numerically. To build up the difference scheme from the partial differential equation, we should be careful. Formal correspondence of difference schemes to the differential equation is not sufficient for the convergence of the solutions to the exact one. For equations of hyperbolic type, the convergence is assured under the CFL condition [1], which is concerned with the ratio of the space increment to the time one. However, this does not assert that, without CFL condition, every discrete solution diverges. G. Dahlquist [2] exposed an interesting example. He considered the wave equation, and descretized it by the usual finite difference scheme. He showed that if initial data for the wave equation are real analytic, then solutions of difference scheme converge to the solution of the wave equation, even in the absence of the CFL condition. Our results in this issue is in the same direction. Our aim is to show that, in the analytic case, we need not the CFL type condition for the convergence of solutions of the finite difference scheme. We treat of the linear first order system with constant coefficients;

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