Digital Signal Processing Reference
In-Depth Information
i the integration time; r 0 any point on the surface where to integrate the
functions; the delay at which the correlation function is being evaluated; and
f c the central correlation frequency;
￿
￿
R. a ; b / the distance between points a and b ;
. r 0 / is the delay of the ray-path from the transmitter to the surface point r 0
￿
and
from there to the receiver; and f D . r 0 / its Doppler frequency;
￿ 0 is the bi-static scattering coefficient, defined as the fraction of incident power
that can be scattered into certain direction and polarization state pq , normalized
by the incident power density and area.
￿ Note that other sources of power attenuation or loss might also be intro-
duced, such as atmospheric attenuation; cabling/instrumental loss; quantification
(number of bit sampling) loss.... All these factors would simply multiply the
right-hand side of Eq. 8.49
The bi-static scattering coefficient for KGO is (e.g. Ulaby et al. 1982 ; Zavorotny
and Voronovich 2000 ; Cardellach 2002 )
2 q 2
q z
pq D k 2
j R pq j
PDF.Z x ;Z y /
(8.50)
where k is the electromagnetic wavenumber; R pq the scattering coefficients; and
PDF.Z x ;Z y / is the 2-D Probability Density Function of the surface slopes Z
(along the x-direction Z x , and y-direction Z y ). In order to extend the bi-static radar
equation to other electromagnetic scattering models, 0
must be replaced by its
corresponding expression.
This bi-static radar equation can also be seen as the 2D-convolution between the
Woodward Ambiguity Function (WAF) 2 .; f c / (impulse response from a single
delay-Doppler cell) and a function †.; f c / to weight each delay-Doppler cell based
on the scattering coefficient, geometry, antenna patterns...( Marchan-Hernandez
et al. 2008 )
2 > D 2 .; f c / †.; f c /
< j Y pq .; f c / j
(8.51)
with
2 .; f c / D ƒ 2 . / j S.f c / j
2
(8.52)
and
4 i Z
G T . r 0 /G R . r 0 / pq . r 0 /
R 2 . T ; r 0 /R 2 . r 0 ; R /
P T
.4/ 2
2
ı. . r 0 //ı.f c f D . r 0 //d 2 r 0
(8.53)
†.; f c / D
S
being ı.x x 0 / Dirac delta functions.
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