Excitation of Surface Waves On a Unidirectionally Conducting Screen By a Phased
Excitation of Surface Waves On a Unidirectionally Conducting Screen By a Phased
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In our eReader you can find the full English version of the book. Read Excitation of Surface Waves On a Unidirectionally Conducting Screen By a Phased Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Excitation of Surface Waves On a Unidirectionally Conducting Screen By a Phased
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The expression for u then becomes (3. 7) ojep3 K -i5Tt/U cos 9 / 2 ^ ~* h ^ (k-K cos 9)(k + K cos 9) \] itkR exp{ipx + ikR ± Ikz^ sin 9} where the plus sign holds above the screen (z > 0) and the minus sign below (z < 0). -9- The scattered fields are given in terms of u by (2. 8) and (2-91 Using the operators given by (3. 6), we find , 2 2 .^ /, 2 P3 K -l^n/h cos Q r^ X k (k-K cos 0)(k+K cos 9) n/ jtkE • expfipx + iitR ± iKz„ sin 9] (3. 8) e -4 - ^ g-i3«/^ ^Q3 Q / _^ g{ipx + iKR + iKz^ sin 9} P Pk -i3ir/U sin 9 cos 9 / 2 ij- (k-K cos 9)(k+K cos 9) \/ itkR z and . Exp{ipx + iKiR ± IkZq sin 9] ojgpPK -i3rt/^ sin 9 cos 9 X k (k-K cos 9)(k+K cos 9) \J ttkR . Exp[ipx + iKiR ± iKZ^ sin 9] (3. 9) h ^0 p ujep3 k: -i3Jt/U cos 9 z ^ ~ i| (k-K cos 9)(k+K cos 9) \/ jtkR •expfipx + iKR ± iKZ„ sin 9}. The same convention regarding signs above and below the screen still holds. We next determine the cylindrical components of the scattered far field. Note that e = e X X (3. 10) e„ = e cos 9 + e sin 9 ^ R y z e„ = -e sin 9 + e cos 9 9 y z -10- and similarly for the magnetic field components.
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To quickly assess the difficulty of the text, read a short excerpt:
The expression for u then becomes (3. 7) ojep3 K -i5Tt/U cos 9 / 2 ^ ~* h ^ (k-K cos 9)(k + K cos 9) \] itkR exp{ipx + ikR ± Ikz^ sin 9} where the plus sign holds above the screen (z > 0) and the minus sign below (z < 0). -9- The scattered fields are given in terms of u by (2. 8) and (2-91 Using the operators given by (3. 6), we find , 2 2 .^ /, 2 P3 K -l^n/h cos Q r^ X k (k-K cos 0)(k+K cos 9) n/ jtkE • expfipx + iitR ± iKz„ sin 9] (3. 8) e -4 - ^ g-i3«/^ ^Q3 Q / _^ g{ipx + iKR + iKz^ sin 9} P Pk -i3ir/U sin 9 cos 9 / 2 ij- (k-K cos 9)(k+K cos 9) \/ itkR z and . Exp{ipx + iKiR ± IkZq sin 9] ojgpPK -i3rt/^ sin 9 cos 9 X k (k-K cos 9)(k+K cos 9) \J ttkR . Exp[ipx + iKiR ± iKZ^ sin 9] (3. 9) h ^0 p ujep3 k: -i3Jt/U cos 9 z ^ ~ i| (k-K cos 9)(k+K cos 9) \/ jtkR •expfipx + iKR ± iKZ„ sin 9}. The same convention regarding signs above and below the screen still holds. We next determine the cylindrical components of the scattered far field. Note that e = e X X (3. 10) e„ = e cos 9 + e sin 9 ^ R y z e„ = -e sin 9 + e cos 9 9 y z -10- and similarly for the magnetic field components.
What to read after Excitation of Surface Waves On a Unidirectionally Conducting Screen By a Phased?
You can find similar books in the "Read Also" column, or choose other free books by Samuel Karp to read online
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