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September 2003©2003 by H.L. Bertoni1 VII. Diffraction by an Absorbing Half-Screen Kirchhoff-Huygens Approximation for Plane Wave Diffraction by an Edge Geometrical Theory of Diffraction Uniform Theory of Diffraction
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September 2003©2003 by H.L. Bertoni2 Plane Wave Illumination of an Absorbing Half-Plane z x y r dy dz ( x, y, 0 )
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September 2003©2003 by H.L. Bertoni3 Evaluation of the Integration Over z The Contribution to the integral come from a small region about z = 0
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September 2003©2003 by H.L. Bertoni4 Evaluation of the Integration Over y We distinguish two cases that are most easily solved 1) Well inside the region y > 0 illuminated by the plane wave. 2) Well inside the shadow region y < 0. R X y’ y R X y’ y
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September 2003©2003 by H.L. Bertoni5 Inside the Illuminated Region y > 0 y y Interrupted cancellation Cancellation of alternate half cycles
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September 2003©2003 by H.L. Bertoni6 Evaluating y Integral for y > 0
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September 2003©2003 by H.L. Bertoni7 Evaluating y Integral for y > 0 - cont.
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September 2003©2003 by H.L. Bertoni8 Evaluating y Integral for y > 0 - cont. Y x Incident plane wave
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September 2003©2003 by H.L. Bertoni9 Inside the Shadow Region y < 0 y y Interrupted cancellation Cancellation of alternate half cycles
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September 2003©2003 by H.L. Bertoni10 Evaluating y Integral for y < 0
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September 2003©2003 by H.L. Bertoni11 Geometrical Theory of Diffraction (GTD ) ( ) y x Shadow boundary Diffracted Cylindrical wave Incident Plane wave
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September 2003©2003 by H.L. Bertoni12 GTD Valid Outside Transition Region Fresnel zone Shadow boundary Incident plane wave y x
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September 2003©2003 by H.L. Bertoni13 Example of Shadowing at Building Corners Building y x From Transmitter 2 m
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September 2003©2003 by H.L. Bertoni14 Uniform Theory of Diffraction for Small y
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September 2003©2003 by H.L. Bertoni15 Evaluating End Point Integrals
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September 2003©2003 by H.L. Bertoni16 Evaluating End Point Integrals - cont.
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September 2003©2003 by H.L. Bertoni17 Evaluating End Point Integrals - cont.
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September 2003©2003 by H.L. Bertoni18 Approximation for F(s)
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September 2003©2003 by H.L. Bertoni19 Field at the Shadow Boundary
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September 2003©2003 by H.L. Bertoni20 Value of F(s) for Large s
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September 2003©2003 by H.L. Bertoni21 Variation of Field Near Shadow Boundary Y x x= 30 m -10-50510 -30 -25 -20 -15 -10 -5 0 5 Received Signal(dB) y(meters) WFWF -W F
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