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Chapter 5 - Spatial and Temporal Discretizations of Partial Differential Equations

Published online by Cambridge University Press:  05 January 2014

Tapan Sengupta
Affiliation:
Indian Institute of Technology, Kanpur
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Summary

Introduction

Unlike analytic solutions where we have information everywhere in the domain at all times, in computing we can obtain answers only at discrete points in the domain, called the grid points, at discrete times. This discretization of the independent variables is the first step in computing and a typical section of a discrete grid of points in space are shown in the Cartesian two dimensional plane in Fig. 5.1. Thus, the solution space is discretized preferably with uniformly spaced nodes or discrete points, as shown in the figure.

The approach in obtaining the numerical solution of differential equation rests on representing various differential operators by an equivalent algebraic expressions, i.e., the differential equations are reduced to a set of algebraic relations, which is eventually solved to obtain the unknowns at the grid points. This step of generating algebraic equation from governing equation is known as the discretization process. There is no unique way of doing this. Hence, there is no unique way of solving governing equations. However, there are guiding principles which allow practitioners to choose methods to obtain correct answer. The main guiding principle is the consistency – by which one means that the discretized equations reproduce the original governing equations in the limit of vanishing distance in the grid network shown in Fig. 5.1 and the time step reduced to zero.

Type
Chapter
Information
High Accuracy Computing Methods
Fluid Flows and Wave Phenomena
, pp. 71 - 91
Publisher: Cambridge University Press
Print publication year: 2013

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