Diffraction of Electromagnetic Waves By a Plane Wire Grating
Diffraction of Electromagnetic Waves By a Plane Wire Grating
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In our eReader you can find the full English version of the book. Read Diffraction of Electromagnetic Waves By a Plane Wire Grating 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 Diffraction of Electromagnetic Waves By a Plane Wire Grating
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5, page 5 -12- eymmetrlc. In the present case we deal not with the radiation field of a line current, tnit with that of a unifora distrl'bation, on a line parallel to the y ajcls, of short current elements perpendicular to the y axis, all in the same direction and in phase. Let g(r, r') be the radiation field of a single current element in the T E problem; then ^^>/ g(r, r' ), the derivative of g with respect to the primed coordinates, in a direction perpendicular both to the y axis and the dir...ection of the current flow, is the radiation field in the T M problem. Although the above discussion applied to the radiation field of a single current element, it is immediately applicable to the field generated by currents on a set of lines, distance a apart, with the appropriate phase difference between successive lines. Thus ve have (22) r (a;x, !:;x', z») = r-:^ G(s;x, z;x«, z« ) where G is defined by Eq. (S). The field is then (23) (b -^, ^f ^(p i^) ^/'a, (s;r;r. )l ^''^ ^' ' ' inc ' sc ' n, p, a J v ^tV, ^ where G is differentiated in a direction normal to the wire surface.
What to read after Diffraction of Electromagnetic Waves By a Plane Wire Grating?
You can find similar books in the "Read Also" column, or choose other free books by J Shmoys to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
5, page 5 -12- eymmetrlc. In the present case we deal not with the radiation field of a line current, tnit with that of a unifora distrl'bation, on a line parallel to the y ajcls, of short current elements perpendicular to the y axis, all in the same direction and in phase. Let g(r, r') be the radiation field of a single current element in the T E problem; then ^^>/ g(r, r' ), the derivative of g with respect to the primed coordinates, in a direction perpendicular both to the y axis and the dir...ection of the current flow, is the radiation field in the T M problem. Although the above discussion applied to the radiation field of a single current element, it is immediately applicable to the field generated by currents on a set of lines, distance a apart, with the appropriate phase difference between successive lines. Thus ve have (22) r (a;x, !:;x', z») = r-:^ G(s;x, z;x«, z« ) where G is defined by Eq. (S). The field is then (23) (b -^, ^f ^(p i^) ^/'a, (s;r;r. )l ^''^ ^' ' ' inc ' sc ' n, p, a J v ^tV, ^ where G is differentiated in a direction normal to the wire surface.
What to read after Diffraction of Electromagnetic Waves By a Plane Wire Grating?
You can find similar books in the "Read Also" column, or choose other free books by J Shmoys to read onlineMoreLess
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