2013-03-07
Electromagnetic Wave Scattering from Cylindrical Structure with Mixed-Impedance Boundary Conditions
By
Progress In Electromagnetics Research M, Vol. 29, 207-222, 2013
Abstract
Recently, a new boundary condition is introduced in which surface shows different impedances for TE and TM electromagnetic fields. This new boundary condition is called mixed-impedance (MI) boundary condition and can be expressed in terms of normal components of electromagnetic fields. In this paper, the cylindrical structures with MI boundary condition were investigated and the scattering of such structures was obtained for both normal and oblique incidence and both TEZ and TMZ polarizations. The interesting feature of MI boundary condition was that the boundary conditions of PEC, PMC, DB, D'B', and isotropic impedance boundaries were special cases of the MI boundary. Therefore, by calculating the electromagnetic scattering from a MI boundary, scattering from various boundary conditions could be easily obtained. It was also demonstrated that, by proper choice of boundary conditions the forward or backward RCS (radar cross section) could be significantly increased or decreased.
Citation
Mostafa Mashhadi, Ali Abdolali, and Nader Komjani, "Electromagnetic Wave Scattering from Cylindrical Structure with Mixed-Impedance Boundary Conditions," Progress In Electromagnetics Research M, Vol. 29, 207-222, 2013.
doi:10.2528/PIERM12122809
References

1. Hoppe, D. J. and Y. Rahmat-Samii, Impedance Boundary Conditions in Electromagnetics, Taylor & Francis, 1995.

2. Lindell, I. V. and A. Sihvola, "Perfect electromagnetic conductor," Journal of Electromagnetic Waves and Applications, Vol. 19, No. 7, 861-869, 2005.
doi:10.1163/156939305775468741        Google Scholar

3. Kildal, P. S., "Artificially soft and hard surfaces in electromagnetic," IEEE Trans. on Antennas and Propag., Vol. 38, No. 10, 1537-1544, 1990.
doi:10.1109/8.59765        Google Scholar

4. Lindell, I. V. and A. Sihvola, "Electromagnetic boundary conditions defined in terms of normal field components," IEEE Trans. on Antennas and Propag., Vol. 58, No. 4, 1128-1135, Apr. 2010.
doi:10.1109/TAP.2010.2041149        Google Scholar

5. Lindell, I. V. and A. Sihvola, "Uniaxial IB-medium interface and novel boundary conditions," IEEE Trans. on Antennas and Propag., Vol. 57, No. 3, 694-700, Mar. 2009.
doi:10.1109/TAP.2009.2013431        Google Scholar

6. Lindell, I. V. and A. Sihvola, "Electromagnetic boundary condition and its realization with anisotropic metamaterial," Phys. Rev. E, Vol. 79, No. 2, 026604-7, 2009.        Google Scholar

7. Lindell, I. V. and A. Sihvola, "Simple skewon medium realization of DB boundary conditions," Progress In Electromagnetics Research, Vol. 30, 29-39, 2012.        Google Scholar

8. Zalu·ski, D., D. Muha, and S. Hrabar, "Numerical investigation and possible realization of metamaterial-based DB boundary surface," Proc. on ICECOM, Dubrovnik, Croatia, 251-253, 2010.        Google Scholar

9. Lindell, I. V. and A. Sihvola, "Zero axial parameter (ZAP) sheet," Progress In Electromagnetics Research, Vol. 89, 213-224, 2009.
doi:10.2528/PIER08120307        Google Scholar

10. Lindell, I. V., A. Sihvola, L. Bergamin, and A. Favaro, "Realization of the D'B' boundary condition," IEEE Antennas Wireless Propag. Lett., Vol. 10, 643-646, 2011.
doi:10.1109/LAWP.2011.2159698        Google Scholar

11. Wallen, H., I. V. Lindell, and A. Sihvola, "Mixed-impedance boundary conditions," IEEE Trans. on Antennas and Propag., Vol. 59, No. 5, 1580-1586, May 2011.
doi:10.1109/TAP.2011.2123064        Google Scholar

12. Lindell, I. V., A. Sihvola, P. Yla-Oijala, and H. Wallen, "Zero backscattering from self-dual objects of finite size," IEEE Trans. on Antennas and Propag., Vol. 57, No. 9, 2725-2731, Sep. 2009.
doi:10.1109/TAP.2009.2027180        Google Scholar

13. Balanis, A., Advanced Engineering Electromagnetic, John Wiley & Sons, 1989.