Radio Propagation and Remote Sensing of the Environment - Chapter 1 docx

... as: (1. 16) The divergence of this density is described by the transport equation: . (1. 17) The value: (1. 18) describes the mean for the period losses of the electromagnetic power density, and (1. 19) is ... Bodies 13 3 5.9 Scattering by the Assembly of Particles 14 1 5 .10 Effective Dielectric Permittivity of Medium 14 5 5 .11 The Acting Field 14 8 5 .12 I...

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... q ′ ()     = + () ′ () ′ res s res re , 2 2 2 82 1 ss res () + − () + ′ ()     πν 2 2 2 211 ml q l TF1 710 _book.fm Page 13 1 Thursday, September 30, 2004 1: 43 PM © 2005 by CRC Press 11 6 Radio Propagation and Remote Sensing of the Environment ... exp ⋅⋅ ′       ′ =×       ∫ r rH r E rr ss d V 3 ,. TF1 710 _book.fm Page 11 1 Thursday, September...

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... Press 212 Radio Propagation and Remote Sensing of the Environment (7.2) Here s is the vector orthogonal to the main wave propagation direction (z-axis). The solution of the obtained ... . ν = 11 6 s cog l klL       = 5 3 22 10 7. , µ TF1 710 _book.fm Page 219 Thursday, September 30, 2004 1: 43 PM © 2005 by CRC Press 220 Radio Propagatio...

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... cos , cos 1 1 1 1 2 n vv vu u u v 12 2 224 1 21 21 4 1 , sin sin = − − () − () − ±+− ( ββ )) 2 2 cos . β nv u uu 12 22222 11 2 1 2 4 , sin sin cos .= − ++       βββ∓ nv= − = −≅ 11 1 2 2 2 2 ω ω ω ω p 2 p . EEE zxy ≅−iv ... + ′ ⋅ v 1+ 2 c c cos cos cos .ϑ ϑβ βϑ = ′ + + ′ 1 TF1 710 _book.fm Page 51 Thursday, September 30, 2004 1: 43 PM © 2005 by CRC Press 48 Rad...

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... Press 66 Radio Propagation and Remote Sensing of the Environment logical compared to their energy flows. If the following is the power flow density of the incident wave: then the flow density of its ... Press 76 Radio Propagation and Remote Sensing of the Environment , (3.94) where, as before, F 23 (d) is the Fresnel coefficient of reflection from t...

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... ⋅ − 310 13 2 TF1 710 _book.fm Page 10 0 Thursday, September 30, 2004 1: 43 PM © 2005 by CRC Press 94 Radio Propagation and Remote Sensing of the Environment and (4.37) The rule for choosing the appropriate ... September 30, 2004 1: 43 PM © 2005 by CRC Press 88 Radio Propagation and Remote Sensing of the Environment If angle α between the...

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... the equation: (6 .17 7) Er s s 11 1 1 2 1 1 2 1 1 () = − ()     − ++ ( F F i i h h cos sin θ εθ ))           () g s i ik e φ 1 . Er 12 () kR 1 >> 1. ′ ∇≅−gikg 11 11 ε R R 1 . d >>||,||ζζ 12 RR 11 ≅ + ′ −     ˆ cos ( ) ( ) ,θζ ζ 11 1 22 ss ˆ ,cos ˆ .R R 1 2 1 = − ′ +=ss 21 2 1 d d θ Er s s e 12 1 1 1 4 11 () = ... 22 2 () +...

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... TF1 710 _book.fm Page 2 31 Thursday, September 30, 2004 1: 43 PM © 2005 by CRC Press 232 Radio Propagation and Remote Sensing of the Environment We will now introduce the black body con- cept ... mind the definitions of the extinction coefficient (Equation (5 .13 )) and albedo (Equation (5 .14 )), then we can define the emissivity of the layer filled by the...

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... µ µ= − − ∫ 1 2 1 1 TF1 710 _book.fm Page 266 Thursday, September 30, 2004 1: 43 PM © 2005 by CRC Press 274 Radio Propagation and Remote Sensing of the Environment with each other, and we obtain a Kirchhoff’s ... ν νν νν ν + () + ′ + ′ − ′ () ′ () − ± e XBe d z ∓ ∓ ˆ A −− ′ ′′ ∫ z d d ν νν. 0 1 TF1 710 _book.fm Page 260 Thursday, September 30, 2004 1: 43 PM © 2005 by...

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... for remote sensing of the environment. UV OPT 0.28−0.38 µ 0.38−0.78 µ 0.78−3 µ 3−8 µ 8 10 00 µ 3 10 −7 3 10 −6 3 10 −5 3 10 −4 3 10 −3 3 10 −2 3 10 1 10 8 10 9 10 10 10 11 10 12 10 13 10 14 10 15 3 λm λ ... further in Chapter 11 ) for © 2005 by CRC Press 276 Radio Propagation and Remote Sensing of the Environment 10 .1 FORMULATION OF...

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