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Scattering from a perfectly conducting cube
The cube epitomizes the complex, three-dimensional scatterer with its multiple interactions and vertex diffraction playing a critical part in the far-field patterns of some bistatic planes. the results presented are for a cube on the order of 1.5-3 wavelengths on edge which is illuminated by a plane...
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Published in: | Proceedings of the IEEE 1989-05, Vol.77 (5), p.815-823 |
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container_title | Proceedings of the IEEE |
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creator | Penno, R.P. Thiele, G.A. Pasala, K.M. |
description | The cube epitomizes the complex, three-dimensional scatterer with its multiple interactions and vertex diffraction playing a critical part in the far-field patterns of some bistatic planes. the results presented are for a cube on the order of 1.5-3 wavelengths on edge which is illuminated by a plane wave at broadside incidence. The method employed is the hybrid iterative method (HIM) which utilizes an initial approximation of the surface currents on the cube faces. These currents are inserted into the magnetic-field integral equation (MFIE) to produce improved or updated approximations to these surface currents. This process is repeated to convergence by the method of successive approximations. These currents are then used to find the bistatic radar cross section (RCS) for an arbitrary plane of measurement (emphasis has been placed upon the H-plane and the E-plane). Of particular interest is the development of cross-polarized currents, which are initially approximated by zero. As the iteration process progresses, it is seen that all physical scattering processes present in this body are introduced by enforcing the MFIE.< > |
doi_str_mv | 10.1109/5.32072 |
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The method employed is the hybrid iterative method (HIM) which utilizes an initial approximation of the surface currents on the cube faces. These currents are inserted into the magnetic-field integral equation (MFIE) to produce improved or updated approximations to these surface currents. This process is repeated to convergence by the method of successive approximations. These currents are then used to find the bistatic radar cross section (RCS) for an arbitrary plane of measurement (emphasis has been placed upon the H-plane and the E-plane). Of particular interest is the development of cross-polarized currents, which are initially approximated by zero. As the iteration process progresses, it is seen that all physical scattering processes present in this body are introduced by enforcing the MFIE.< ></description><identifier>ISSN: 0018-9219</identifier><identifier>EISSN: 1558-2256</identifier><identifier>DOI: 10.1109/5.32072</identifier><identifier>CODEN: IEEPAD</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Applied sciences ; Convergence ; Diffraction ; Diffraction, scattering, reflection ; Electromagnetic scattering ; Engine cylinders ; Exact sciences and technology ; Health information management ; Integral equations ; Iterative methods ; Magnetic resonance ; Moment methods ; Radar scattering ; Radiocommunications ; Radiowave propagation ; Telecommunications ; Telecommunications and information theory</subject><ispartof>Proceedings of the IEEE, 1989-05, Vol.77 (5), p.815-823</ispartof><rights>1991 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c302t-35afeeef341b3b37283131397f76a0a355f6542b4c0d944fcc2c71fd9c857cc33</citedby><cites>FETCH-LOGICAL-c302t-35afeeef341b3b37283131397f76a0a355f6542b4c0d944fcc2c71fd9c857cc33</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/32072$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,776,780,27901,27902,54771</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=19658750$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Penno, R.P.</creatorcontrib><creatorcontrib>Thiele, G.A.</creatorcontrib><creatorcontrib>Pasala, K.M.</creatorcontrib><title>Scattering from a perfectly conducting cube</title><title>Proceedings of the IEEE</title><addtitle>JPROC</addtitle><description>The cube epitomizes the complex, three-dimensional scatterer with its multiple interactions and vertex diffraction playing a critical part in the far-field patterns of some bistatic planes. the results presented are for a cube on the order of 1.5-3 wavelengths on edge which is illuminated by a plane wave at broadside incidence. The method employed is the hybrid iterative method (HIM) which utilizes an initial approximation of the surface currents on the cube faces. These currents are inserted into the magnetic-field integral equation (MFIE) to produce improved or updated approximations to these surface currents. This process is repeated to convergence by the method of successive approximations. These currents are then used to find the bistatic radar cross section (RCS) for an arbitrary plane of measurement (emphasis has been placed upon the H-plane and the E-plane). Of particular interest is the development of cross-polarized currents, which are initially approximated by zero. As the iteration process progresses, it is seen that all physical scattering processes present in this body are introduced by enforcing the MFIE.< ></description><subject>Applied sciences</subject><subject>Convergence</subject><subject>Diffraction</subject><subject>Diffraction, scattering, reflection</subject><subject>Electromagnetic scattering</subject><subject>Engine cylinders</subject><subject>Exact sciences and technology</subject><subject>Health information management</subject><subject>Integral equations</subject><subject>Iterative methods</subject><subject>Magnetic resonance</subject><subject>Moment methods</subject><subject>Radar scattering</subject><subject>Radiocommunications</subject><subject>Radiowave propagation</subject><subject>Telecommunications</subject><subject>Telecommunications and information theory</subject><issn>0018-9219</issn><issn>1558-2256</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1989</creationdate><recordtype>article</recordtype><recordid>eNpFkDtPwzAUhS0EEqUgZrYswIBSrh83jkdU8ZIqMQCz5dzaKChNip0M_fekBIHucIbz6ZPuYeycw4JzMLe4kAK0OGAzjljmQmBxyGYAvMyN4OaYnaT0CQASCzljN6_k-t7Huv3IQuw2mcu2PgZPfbPLqGvXA_X7jobKn7Kj4Jrkz35zzt4f7t-WT_nq5fF5ebfKSYLoc4kueO-DVLySldSilHw8o4MuHDiJGApUolIEa6NUIBKkeVgbKlETSTlnV5N3G7uvwafebupEvmlc67shWYFKlVrDCF5PIMUupeiD3cZ64-LOcrD7MSzanzFG8vJX6RK5JkTXUp3-cVNgqXFvvJi4evzgr54c3_tDZKs</recordid><startdate>19890501</startdate><enddate>19890501</enddate><creator>Penno, R.P.</creator><creator>Thiele, G.A.</creator><creator>Pasala, K.M.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>19890501</creationdate><title>Scattering from a perfectly conducting cube</title><author>Penno, R.P. ; Thiele, G.A. ; Pasala, K.M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c302t-35afeeef341b3b37283131397f76a0a355f6542b4c0d944fcc2c71fd9c857cc33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1989</creationdate><topic>Applied sciences</topic><topic>Convergence</topic><topic>Diffraction</topic><topic>Diffraction, scattering, reflection</topic><topic>Electromagnetic scattering</topic><topic>Engine cylinders</topic><topic>Exact sciences and technology</topic><topic>Health information management</topic><topic>Integral equations</topic><topic>Iterative methods</topic><topic>Magnetic resonance</topic><topic>Moment methods</topic><topic>Radar scattering</topic><topic>Radiocommunications</topic><topic>Radiowave propagation</topic><topic>Telecommunications</topic><topic>Telecommunications and information theory</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Penno, R.P.</creatorcontrib><creatorcontrib>Thiele, G.A.</creatorcontrib><creatorcontrib>Pasala, K.M.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Proceedings of the IEEE</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Penno, R.P.</au><au>Thiele, G.A.</au><au>Pasala, K.M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Scattering from a perfectly conducting cube</atitle><jtitle>Proceedings of the IEEE</jtitle><stitle>JPROC</stitle><date>1989-05-01</date><risdate>1989</risdate><volume>77</volume><issue>5</issue><spage>815</spage><epage>823</epage><pages>815-823</pages><issn>0018-9219</issn><eissn>1558-2256</eissn><coden>IEEPAD</coden><abstract>The cube epitomizes the complex, three-dimensional scatterer with its multiple interactions and vertex diffraction playing a critical part in the far-field patterns of some bistatic planes. the results presented are for a cube on the order of 1.5-3 wavelengths on edge which is illuminated by a plane wave at broadside incidence. The method employed is the hybrid iterative method (HIM) which utilizes an initial approximation of the surface currents on the cube faces. These currents are inserted into the magnetic-field integral equation (MFIE) to produce improved or updated approximations to these surface currents. This process is repeated to convergence by the method of successive approximations. These currents are then used to find the bistatic radar cross section (RCS) for an arbitrary plane of measurement (emphasis has been placed upon the H-plane and the E-plane). Of particular interest is the development of cross-polarized currents, which are initially approximated by zero. As the iteration process progresses, it is seen that all physical scattering processes present in this body are introduced by enforcing the MFIE.< ></abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/5.32072</doi><tpages>9</tpages></addata></record> |
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source | IEEE Electronic Library (IEL) Journals |
subjects | Applied sciences Convergence Diffraction Diffraction, scattering, reflection Electromagnetic scattering Engine cylinders Exact sciences and technology Health information management Integral equations Iterative methods Magnetic resonance Moment methods Radar scattering Radiocommunications Radiowave propagation Telecommunications Telecommunications and information theory |
title | Scattering from a perfectly conducting cube |
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