The two incident field directions are ki, and k;,. Displacement of p and ij' by A x gives ($T( p + z3(cl,\*( P' + L)) = / d ~" / d ~' " ( G ( ij + n, F")G\*( ij' + .hx, p"')) x Ji,( P').Q( ij? The last equality is a result of the fact that the antenna Jil creates incident wave ki, and the antenna
A Hybrid Numerical Asymptotic Method for Scattering Problems
β Scribed by Eldar Giladi; Joseph B. Keller
- Publisher
- Elsevier Science
- Year
- 2001
- Tongue
- English
- Weight
- 310 KB
- Volume
- 174
- Category
- Article
- ISSN
- 0021-9991
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π SIMILAR VOLUMES
## Communicated by J. C. Nedelec A new numerical method is derived for the calculation of high-frequency asymptotic expansions of the scalar wave scattered by curved periodic structures. Optimal error estimates for this method are established. 1997 by B. G. Teubner Stuttgart-John Wiley & Sons Ltd
where R Ο UD/v is the Reynolds number. Our purpose is to present a finite difference method for solving (1a)-A numerical method for solving incompressible viscous flow problems is introduced. This method uses the velocities and the (1b) in a domain D in two or three space dimensions, with pressure a