3 edition of Computer code for scattering from impedance bodies of revolution. found in the catalog.
Computer code for scattering from impedance bodies of revolution.
by University of Illinois at Chicago, Dept. of Electrical Engineering and Computer Science, National Aeronautics and Space Administration, National Technical Information Service, distributor in Chicago, Ill, [Washington, DC, Springfield, Va
Written in English
|Other titles||Surface impedance with s and phi variation; analytical and numerial results.|
|Statement||principal investigator: Piergiogio L.E. Uslenghi, co-principal investigator: Sharad R. Laxpati.|
|Series||[NASA contractor report] -- NASA CR-193396.|
|Contributions||Laxpati, Sharad R., United States. National Aeronautics and Space Administration.|
|The Physical Object|
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Get this from a library. Computer code for scattering from impedance bodies of revolution. Part III, Surface impedance with s and phi variation ; analytical and numerial results. [Piergiorgio L E Uslenghi; Sharad R Laxpati; United States.
National Aeronautics and Space Administration.]. The electromagnetic scattering from partially or totally penetrable bodies of revolution (BOR) is formulated in terms of coupled Fredholm integral equations, solved by the method of moments (MM).
Efficient Analysis of EM Scattering From Bodies of Revolution via the ACA Article in IEEE Transactions on Antennas and Propagation 62(2) February with 9 Reads How we measure 'reads'. Founder and Editor of the book series on “Electromagnetism in Information and Communication” published Electromagnetic scattering from anisotropic materials - er.
code and numerical results in two dimensions", IEEE Trans. Antennas Propagat., Electromagnetic scattering by impedance bodies of revolution", IEEE Trans.
Computer code for scattering from impedance bodies of revolution. Part III, Surface impedance with s and On the calculation of an average surface impedance for a periodic surface / [by] Rayner K. Rosich [and] To facilitate or impede. [microform]: the impact. ISBN: X OCLC Number: Description: xvi, pages: illustrations ; 24 cm.
Contents: Spectral Domain Theory of Higher Order Impedance Boundary Conditions --Planar Higher Order Impedance Boundary Conditions --Boundary Conditions for Curved Dielectric and Chiral Coatings --Scattering by a Dielectric-Filled Groove in a.
Ford, A.P., IV* and Collins, P.J., “Computation of Scattering from Bodies of Revolution Using an Entire Domain Basis Implementation of the Moment Method, ” Proceedings of the 17th Annual Review of Progress in Applied Computational Electromagnetics, Monterey, California, pp.
INR. Harrington and J. Mautz, Computation of Green's Functions for Bodies of Revolution, Syracuse University, AFCRL, AD INH. Chao and B. Strait, Computer Programs for Radiation and Scattering by Arbitrary Configurations of Bent Wires, 15 Syracuse University, AFCRL, AD H. Anastassiu, N. Tsitsas, and P.
Papakanellos, “Scattering Analysis of Discrete Bodies of Revolution via an Efficient Numerical Algorithm”, XX URSI Commission B International Symposium on Electromagnetic Theory (EMT-S ), Berlin, Germany, August, pp You can write a book review and share your experiences.
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In reality, a much smaller current flows along each segment of the antenna, limited by the high capacitive impedance of the segments, and the radar cross-section is finite but small.
The scattering cross-section of a matched antenna depends only on the wavelength and the gain, and for the small antennas used in tags, gain is at most about that.
Convergence of the MM solution for TM scattering by a rectangular dielectric cylinder. 16 E.H. Newman, K Kingsley / An introduction to the method of moments AZ,~ tenns in eq.
(69). Using eqs. (52) and (62), the total electric field in the center of cell n is simply In E(x~, y~) = e0)A where I~ is the coefficient of J~ and A is the cross-section Cited by: Shareable Link.
Use the link below to share a full-text version of this article with your friends and colleagues. Learn more. Darko Kajfez and Atef Z. Elsherbeni, "Determination of Antenna Q from the Reflection-Coefficient Data," IEEE Antennas Propag.
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() PDE techniques for solving the problem of radar scattering by a body of revolution. Proceedings of the IEEE() Generalized impedance boundary conditions in by: American Institute of Aeronautics and Astronautics Sunrise Valley Drive, Suite Reston, VA.
Taylor Francis Group, p. ISBN 1 1 This book is for a one- or two-semester course in computational electromagnetics and a reference for the practicing engineer. It is expected that the reader will be familiar with time-harmonic electromagnetic fields and vector calculus.In this thesis, the calculation of the electromagnetics(EM) scattering of three dimensional, irregular, inhomogeneous and lossy dielectric objects is discussed.
The iterative moment method (MM) which can solve problems involving a large number of unknowns than the conventional MM is used. For result comparison and checking, conventional MM is discussed too.
Generally, the method also applies.R. Mittra and R. Gordon, "Radar scattering from bodies of revolution using an efficient partial differential equation algorithm," IEEE Trans.
on Antennas & Propagation, Special Issue on Radar Cross Sections of Complex Objects, vol. AP, no. 5, pp.May