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Development of complex electromagnetic problems using FDTD subgridding in hybrid computational techniques

Author: Khairan N Ramli; R A Abd-Alhameed; Peter S Excell
Publisher: Hauppauge, New York : Nova Science Publishers, Inc., [2014]
Series: Engineering tools, techniques and tables.
Edition/Format:   eBook : Document : EnglishView all editions and formats
Summary:
Complex electromagnetic problems using new hybridised computational techniques combining the frequency domain Method of Moments (MoM), Finite-Difference Time-Domain (FDTD) and a subgridded Finite-Difference Time-Domain (SGFDTD) method are studied and discussed in detail. The techniques are desirable to predict electromagnetic absorption in inhomogeneous, anisotropic and lossy dielectric materials irradiated by  Read more...
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Genre/Form: Electronic books
Additional Physical Format: Print version:
Development of complex electromagnetic problems using FDTD subgridding in hybrid computational techniques
(DLC) 2014029133
(OCoLC)883649859
Material Type: Document, Internet resource
Document Type: Internet Resource, Computer File
All Authors / Contributors: Khairan N Ramli; R A Abd-Alhameed; Peter S Excell
ISBN: 9781633216822 1633216829
OCLC Number: 890139381
Description: 1 online resource.
Series Title: Engineering tools, techniques and tables.
Responsibility: editor, Khairan N. Ramli, Raed A. Abd-Alhameed, and Peter S. Excell (Faculty of Electrical and Electronics Engineering, Universiti Tun Hussein Onn Malaysia).

Abstract:

Complex electromagnetic problems using new hybridised computational techniques combining the frequency domain Method of Moments (MoM), Finite-Difference Time-Domain (FDTD) and a subgridded Finite-Difference Time-Domain (SGFDTD) method are studied and discussed in detail. The techniques are desirable to predict electromagnetic absorption in inhomogeneous, anisotropic and lossy dielectric materials irradiated by geometrically intricate sources. In Method of Moments modelling, the surface kernel solution is derived for 1-D, 2-D and 3-D. The electric surface patch integral formulation is solved by.

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