Complex analysis of elastic symbols and construction of plane wave solutions in the half-space (Q1396421)
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scientific article; zbMATH DE number 1943317
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Complex analysis of elastic symbols and construction of plane wave solutions in the half-space |
scientific article; zbMATH DE number 1943317 |
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Complex analysis of elastic symbols and construction of plane wave solutions in the half-space (English)
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30 June 2003
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In this paper, plane wave solutions for the general reduced wave equation \[ \Biggl(\sigma^2 I+\sum^n_{i,j=1} a_{ij}\partial_i \partial_j\Biggr) u(x)= 0\qquad\text{in }\mathbb{R}^n_+\tag{1} \] are considered. In (1), \(\sigma\) is an arbitrary positive fixed parameter, \(x= (x_1,x_2,\dots, x_n)\), \(\partial_i= \partial/\partial x_i\) \((i= 1,2,\dots, n)\), \(\mathbb{R}^n_+= \{x\mid x_n> 0\}\), \(a_{ij}\) \((i,j= 1,2,\dots, n)\) is a positive definite symmetric matrix. Plane wave solutions of (1) which satisfy the Dirichlet boundary condition on \(x_n= 0\) are constructed by the application of complex analysis to the inverse matrix of elastic symbols.
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complex analysis
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elastic symbols
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half space
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wave equation
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Dirichlet boundary condition
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0.8957736
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0.8818102
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0.8725345
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0.8663258
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0.86026645
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0.85942155
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