Figure 3 Computed the normalized attenuation index NΠ versus Ε½ . y 3 the reduced film thickness Dr = 10 for different material covers. The curves from the bottom to top are related to n s 1.0, c n s 1.25, n s 1.54. The rest of the data are β X s y39.88 y i15.56 c c f w x 10 , s 0.6328 m, and s 35Π
An on-surface radiation condition for Maxwell's equations in three dimensions
β Scribed by Habib Ammari; Sailing He
- Publisher
- John Wiley and Sons
- Year
- 1998
- Tongue
- English
- Weight
- 168 KB
- Volume
- 19
- Category
- Article
- ISSN
- 0895-2477
No coin nor oath required. For personal study only.
β¦ Synopsis
An on-surface radiation condition for Maxwell's equations is deri¨ed through the asymptotic expansion of the electromagnetic pseudodifferential operator to obtain straightforward high-frequency solutions of electromagnetic scattering from three-dimensional perfectly conducting con¨ex objects. The present on-surface radiation condition ex-( ) presses the tangential scattered magnetic field unknown on the surface ( ) in terms of the tangential scattered electric field known on the surface and its surface geometrical differentions.
π SIMILAR VOLUMES
Continuing element exchange between minerals during cooling from the metamorphic peak modifies mineral compositions from those existing at the peak. After closure, when the minerals stop changing composition, the compositional relationships hold important information regarding, for example, cooling