CAMS/SCMA Doctoral Dissertation Award 86 Winner and Abstract
1986
Zi-Cai Li (G.F.D. Duff),
Department of Mathematics and Applied Mathematics,
University of Toronto
Numerical Methods for Elliptic Boundary Value
Problems with Singularities
Part 1: Boundary approximation techniques are described for solving
homogeneous self-adjoint elliptic equations. Piecewise expansions into
particular solutions are used which approximate both the boundary and
interface conditions in a least squares sense. Convergence of such
approximations is proved and error estimates are derived in a natural norm.
Numerical experiments are first reported for the interface problems of the
elliptic equation, Delta(u)+u=0, which yield extremely accurate solutions
and surprisingly small condition numbers of the coefficient matrix with
only a modest computational effort.
The advantage of the boundary methods over a standard finite difference or
finite element method is that it can cope with complicated boundaries and
boundary conditions as well as singularities and infinite domains. From a
computational point of view, boundary methods are easy to use, benefiting
from the reduced complexity of a boundary approximation. In addition it is
often possible to control the error in the approximation by the computable
error in the boundary, even for the elliptic problems which do not possess
a maximum principle.
Part 2: Piecewise linear functions are chosen to be admissible functions
only in part of a solution domain; singular (or analytic) functions are
chosen to be admissible functions in the rest of the solution domain. In
addition, the admissible functions used here are constrained to be
continuous only at the element nodes on their common boundary.
We have further developed this method using a new coupling strategy. If
L=O(|lnh|), the average errors of numerical solutions and their generalized
derivatives are still O(h), where h is the maximal boundary length of
regular triangular elements in the finite element method, and L is the
total of singular admissible functions in the Ritz-Galerkin method.
The coupling relation L = O(|lnh|) is significant because only a few
singular functions are required for a good approximation of solutions.
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