The International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences. Voi. XXXVII. Part Bl. Beijing 2008
Where M 9 ,M i = rotate matrix which are denoted by the elements
of exterior orientation from the i row.
let M e M i =
a,
a,
b\ b 2 b 3
so
x . = f «.V ~ *«) + \(Y - Y si ) + c,'(Z -ZJ
a^X-X sl ) + b 3 \Y-Y si ) + c 3 \z-Z si )
y _ Q f a^{X-X si ) + b^{Y-Y si ) + c^{Z-Z si )
Fig 2. Epipolar Geometry of projection track method
This model is an approximate model which assumes the
elements of exterior orientation are the linear function of time.
Through this approximate model, the epipolar geometry could
be used in SAR image.
Scholars have put forward several epipolarity models in
photogrammetry. One is based on the polynomial fitting of
conjugate points. And, another one based on changing the
height of the corresponding object point along the light ray is
named as projection track method [4]. This paper based on
theory of projection track method. Since looking the SAR
image as the multi-central projection linear array imagery,
according to the characteristic of central projection imagery,
changing the height of the corresponding object point along the
ray connecting the perspective centre and projecting the object
points onto the other image, the track of a series of pixels
obtained is the epipolar curve, then corresponding image points
could be searched in the epipolar curve.
3. EXPERIMENT METHOD
After analyzing the epipolar geometry theory in SAR image,
the detail approach of the research is as follow steps:
Firstly, we chose a pair of airborne SAR images. In order to
improve the effective of matching, the pyramid-layered method
has been adopted in this research. The bottom of the
pyramid-image is the original airborne SAR image. The top of
the pyramid-image is formed by putting together 2*2 pixels
from the bottom of the pyramid-image. After extracting feature
points in the left image as control points, we extracted the grid
points of the left image as the feature points, and computed out
the coordinate of these points.
Secondly, we built the SAR imaging equation. Based on the
imaging model of CCD push-broom imagery, the SAR
row-center projection equation is built to represent the
relationship between the image coordinate and space coordinate.
Assuming that point q(xi,0) is the point in the i scan line of left
image, so we can construct a function to represent the space
coordinate of point Q(X,Y,Z), which is in the line of Sq by the
row-center projection equation(S is the projection center of
them i scan line)[4].
r \\ r U r U
x,
(X,Y,Z) T =(X si ,Y si ,Z si ) T +Ä
r 2 1 r 22 r 23
/31 ^32 >33 _
^ °
1
Where /1 = proportional divisor,
Tjj = coefficient of rotate matrix in left image,
(X si , Y si , Z si ) = coordinate of left photographic centre
If point Q is also projected in the j scan line of right image, the
space coordinate of point Q would be satisfied the projection
equation of the right image.
x f„(x- X'„) + rjy_ - y,')+r 3 ,(z - z; f )
f-JX -*')+r a (Y - rj)+r 3J (z - z;.)
0 = r a (X -X' sj ) + r 22 (Y-Y') + r 32 (Z - Z')
Where Y~ = coefficient of rotate matrix in right image,
(X' sj ,Y' S j,Z' S j) coordinate of right photographic
centre.
Then using the simultaneous equations to obtain the epipolar
line equation, the correlativity of left and right image would be
constructed
h x r + hy r + h x r y r + ^4 “ 0
h = m \ y l +m 2
l 2 = (jn 2) x l + m 4 )y, + (m 5 x, + m 6 )
h=m 1 y i +m 8
l 4 =(m 9 x l +m w )y l +(m n x l +m 12 )
Where li(i= 1, • • • 12) is the constant,
(x r ,y r ) and (xi,yi) are the coordinate of the homologous
image points
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