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1 A GENERAL EFFECTIVE PROCEDURE FOR COMBINING COLLOCATION AND DOMAIN DECOMPOSITION METHODS Ismael Herrera* and Robert Yates** *UNAM and **Multisistemas de Computo MEXICO
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2 THE PROBLEM The main technical difficulty stems from the fact that the standard collocation method (orthogonal spline collocation: OSC) yields non-symmetric matrices, even for formally symmetric differential operators. Combining collocation and DDM presents difficulties that must be overcome
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3 SOLUTION OF THE PROBLEM In recent years new collocation methods have been introduced which yield symmetric matrices when the differential operators are formally symmetric. Generically they are known as TH-collocation. TH-collocation combines orthogonal collocation with a special kind of Finite Element Method: FEM-OF. New collocation methods
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4 STRUCTURE OF THIS TALK This talk is divided into two parts: 1.Finite Element Method with Optimal Functions (FEM-OF). 2.TH-collocation
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5 NOTATIONS
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6 PIECEWISE DEFINED FUNCTIONS Σ
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7 THE BOUNDARY VALUE PROBLEM WITH PRESCRIBED JUMPS (BVPJ)
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8 GREEN´S FORMULAS IN DISCONTINUOUS FUNCTIONS (GREEN-HERRERA FORMULAS,1985)
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10 A GENERAL GREEN-HERRERA FORMULA FOR OPERATORS WITH CONTINUOUS COEFFICIENTS
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11 WEAK FORMULATIONS OF THE BVPJ
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12 FINITE ELEMENT METHOD with OPTIMAL FUNCTIONS A target of information is defined. This is denoted by “S*u”. FEM-OF are procedures for gathering such information.
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13 CONJUGATE DECOMPOSITIONS
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14 OPTIMAL FUNCTIONS
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15 THE STEKLOV-POINCARÉ APPROACH THE TREFFTZ-HERRERA APPROACH THE PETROV-GALERKIN APPROACH
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16 ESSENTIAL FEATURES OF FEM-OF METHODS
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17 THREE VERSIONS OF FEM-OF
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18 EXAMPLE SECOND ORDER ELLIPTIC
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19 A POSSIBLE CHOICE OF THE ‘SOUGHT INFORMATION’
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20 CONJUGATE DECOMPOSITIONS
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21 THE SYMMETRIC POSITIVE CASE
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22 TH-COLLOCATION This is obtained by locally applying orthogonal collocation to construct the approximate optimal functions.
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23 SECOND ORDER ELLIPTIC EQUATIONS
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25 CONSTRUCTION OF THE OPTIMAL FUNCTIONS An optimal function is uniquely defined when its ‘trace’ is given on Σ. Piecewise polynomials, up to a certain degree, are chosen for the traces on the internal boundary Σ. Then the well-posed local problems are solved by orthogonal collocation.
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26 Support of an ‘Optimal Function’ CONSTRUCTION BY ORTHOGONAL COLLOCATION Cubic-Cubic: Four Collocation Points Collocation at each
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27 COMPARISON WITH ‘OSC’ Steklov-Poincaré FEM-OF yields the same solution as OSC. However, now the system-matrix is positive definite for differential systems that are symmetric and positive. Trefftz-Herrera FEM-OF yields the same order of accuracy as OSC, although its solution is not necessarily the same. The system-matrix is positive definite for differential systems that are symmetric and positive.
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28 Support of an ‘Optimal Function’ CONSTRUCTION BY ORTHOGONAL COLLOCATION Linear-Quadratic (One collocation point) Collocation at each
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29 THE BILINEAR FORM
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30 TH-COLLOCATION FOR ELASTOSTATIC PROBLEMS OF ANISOTROPIC MATERIALS AND ITS PARALLELIZATION
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32 CONSTRUCTION OF THE OPTIMAL FUNCTIONS The displacement fields are chosen to be piecewise polynomials, up to a certain degree, on the internal boundary, Σ. Then the well-posed local problems are solved by orthogonal collocation.
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33 THE BILINEAR FORM
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34 ISOTROPIC MATERIALS
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36 CONCLUSIONS For any linear differential equation or system of such equations, TH-collocation supplies a new and more effective manner of using orthogonal collocation in combination with DDM. It has attractive features such as: 1. Better structured matrices, 2. The approximating polynomials on the internal boundary and in the element interiors can be chosen independently, 3. The number of collocation points can be reduced.
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