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          <dc:identifier>https://hdl.handle.net/2286/R.I.46239</dc:identifier>
                  <dc:rights>http://rightsstatements.org/vocab/InC/1.0/</dc:rights>
          <dc:rights>All Rights Reserved</dc:rights>
                  <dc:date>2017</dc:date>
                  <dc:format>vi, 54 pages : illustrations (some color)</dc:format>
                  <dc:type>Masters Thesis</dc:type>
          <dc:type>Academic theses</dc:type>
          <dc:type>Text</dc:type>
                  <dc:language>eng</dc:language>
                  <dc:contributor>Cao, Jiahao</dc:contributor>
          <dc:contributor>Pan, George</dc:contributor>
          <dc:contributor>Balanis, Constantine A</dc:contributor>
          <dc:contributor>Cochran, Douglas</dc:contributor>
          <dc:contributor>Arizona State University</dc:contributor>
                  <dc:description>Partial requirement for: M.S., Arizona State University, 2017</dc:description>
          <dc:description>Includes bibliographical references (pages 52-54)</dc:description>
          <dc:description>Field of study: Electrical engineering</dc:description>
          <dc:description>Scattering from random rough surface has been of interest for decades. Several&lt;br/&gt;&lt;br/&gt;methods were proposed to solve this problem, and Kirchho approximation (KA)&lt;br/&gt;&lt;br/&gt;and small perturbation method (SMP) are among the most popular. Both methods&lt;br/&gt;&lt;br/&gt;provide accurate results on rst order scattering, and the range of validity is limited&lt;br/&gt;&lt;br/&gt;and cross-polarization scattering coecient is zero for these two methods unless these&lt;br/&gt;&lt;br/&gt;two methods are carried out for higher orders. Furthermore, it is complicated for&lt;br/&gt;&lt;br/&gt;higher order formulation and multiple scattering and shadowing are neglected in these&lt;br/&gt;&lt;br/&gt;classic methods.&lt;br/&gt;&lt;br/&gt;Extension of these two methods has been made in order to x these problems.&lt;br/&gt;&lt;br/&gt;However, it is usually complicated and problem specic. While small slope approximation&lt;br/&gt;&lt;br/&gt;is one of the most widely used methods to bridge KA and SMP, it is not easy&lt;br/&gt;&lt;br/&gt;to implement in a general form. Two scale model can be employed to solve scattering&lt;br/&gt;&lt;br/&gt;problems for a tilted perturbation plane, the range of validity is limited.&lt;br/&gt;&lt;br/&gt;A new model is proposed in this thesis to deal with cross-polarization scattering&lt;br/&gt;&lt;br/&gt;phenomenon on perfect electric conducting random surfaces. Integral equation&lt;br/&gt;&lt;br/&gt;is adopted in this model. While integral equation method is often combined with&lt;br/&gt;&lt;br/&gt;numerical method to solve the scattering coecient, the proposed model solves the&lt;br/&gt;&lt;br/&gt;integral equation iteratively by analytic approximation. We utilize some approximations&lt;br/&gt;&lt;br/&gt;on the randomness of the surface, and obtain an explicit expression. It is shown&lt;br/&gt;&lt;br/&gt;that this expression achieves agreement with SMP method in second order.</dc:description>
                  <dc:subject>Electromagnetism</dc:subject>
          <dc:subject>Backscattering</dc:subject>
          <dc:subject>perfect conducting</dc:subject>
          <dc:subject>Random rough surface</dc:subject>
          <dc:subject>Scattering</dc:subject>
          <dc:subject>Electromagnetism</dc:subject>
          <dc:subject>Backscattering</dc:subject>
                  <dc:title>A new model for cross-polarization scattering from perfect conducting random rough surfaces in backscattering direction</dc:title></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>
