An iterative procedure is described for the finite-element solution of scalar scattering problems in unbounded domains. The scattering objects may have multiple connectivity, may be of different materials or with different boundary conditions. A fictitious boundary enclosing all the objects involved
Causal perfectly matched anisotropic absorbers for the numerical solution of unbounded problems in the time domain
β Scribed by E. Bermani; S. Caorsi; M. Raffetto
- Publisher
- John Wiley and Sons
- Year
- 1999
- Tongue
- English
- Weight
- 187 KB
- Volume
- 21
- Category
- Article
- ISSN
- 0895-2477
No coin nor oath required. For personal study only.
β¦ Synopsis
TABLE 3 Simulation Results of Parallel Adding Method Number of P -Code 1 2 3 3 Successful Number of P -Code 15044 77 0 7 Total Number of P -Code 823543 823543 823543 7 creases. The interference between the P -code and P -code 7 3
is more serious in VAD. That is, the interference from K is more important than N.
IV. CONCLUSION
From simulation results, we find that it is indeed a feasible way to achieve the purpose of multiplexing different prime codes system to commonly share a transmission channel. We Ε½ . use two ways VAM and PAM to insert P -codes into 3 P -codes. These two ways are the fixed slot method and easily 7 controlling the inserting P -code. On the other hand, the 3 fixed position method for inserting P -code cannot provide 3 Ε½ . the best control for various combinations of P -code 823543 .
7
The simulation results have shown that the main interference in the different prime code systems is PAM. Consider adding to P -code the number 3; the system using PAM fails, 3 and the system using VAM still has 1847 successful numbers. Therefore, we can conclude that VAM is a better design algorithm than PAM.
π SIMILAR VOLUMES
This paper presents a 3D body-conforming "nite element solution of the time-dependent vector wave equation. The method uses edge elements on tetrahedra for the electric "eld interpolation. This kind of element is suited to model Maxwell's equations since it only enforces tangential continuity of vec