Fast solvers of generalized arifoil equation of index -1 (Q2784829)
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scientific article; zbMATH DE number 1733049
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Fast solvers of generalized arifoil equation of index -1 |
scientific article; zbMATH DE number 1733049 |
Statements
16 November 2003
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generalized airfoil equation
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linear continuous Fredholm operator
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fast solvers
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weighted spaces
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cosine transformation
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1-periodic integral equation
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fully discrete trigonometric collocation method
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conjugate gradient method
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Sobolev norms
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Fast solvers of generalized arifoil equation of index -1 (English)
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The author considers the generalized airfoil equation NEWLINE\[NEWLINE(Bv)(x) :=\int_{-1}^{1}\left(\frac{1}{\pi}\frac{1}{x-y}+b_1(x,y)\log|x-y|+ b_2(x,y)\right)v(y) dy=g(x).NEWLINE\]NEWLINE The kernel functions \(b_1\) and \(b_2\) are assumed to be smooth. In this case, \(B\) represents a linear continuous Fredholm operator in different weighted spaces \(L_\sigma^2(-1, 1)\); the index of \(B\) depends on the weight \(\sigma(x)\). In the present paper, \(\sigma(x)=1/\sqrt{1-x^2}\); then the index of \(B\in\mathcal L(L_\sigma^2(-1, 1))\) is \(-1\). With the cosine transformation the above integral equation is reduced to the 1-periodic integral equation which is discretized by a fully discrete version of the trigonometric collocation method. The conjugate gradient method is applied to solve the discretized problem. The approximate solution appears to be of optimal accuracy in a scale of Sobolev norms, and the \(N\) parameters of the approximate solution can be determined by \( O(N\log N)\) arithmetical operations.
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