Image Processing Reference
In-Depth Information
R · ( −−−−→
O W O C ) W is constant for all points P as soon as
This is because the term
R , ( −−−−→
O W O C ) W are fixed. The parameters R , ( −−−−→
O W O C ) W are called extrinsic param-
eters because they encode the direction and the position of the camera frame relative
to the world frame. Classically, we can make the relationship between the two po-
sition vectors linear by representing ( −−−→
O W P ) W in its homogeneous coordinates. By
augmenting the matrix R , we thus obtain
( −−−→
O C P ) C = M E ( −−−→
O W P ) WH
(13.36)
where 4
O W P ) WH = ( −−−→
R ( −−−→
O W O C ) W ]=[ R , ( −−−−→
( −−−→
O W P ) W
1
O C O W ) C ] ,
M E =[ R ,
(13.37)
represent the extrinsic matrix and the homogeneous coordinates of the point P w.r.t.
the world frame, respectively. Here we have used lemma 13.4 to obtain ( −−−−→
O C O W ) C =
R ( −−−→
O W O C ) W , which is the relationship between the two representations of the dis-
placement vector between the camera and the world frames. The extrinsic matrix is
accordingly a 3
4 matrix obtained by juxtaposing R with the column vector of the
interframe displacement, which we define as follows for convenience:
×
=( −−−−→
t =( t X ,t Y ,t Z ) T
O C O W ) C =
R ( O W O C ) W
(13.38)
We summarize these results as follows:
Lemma 13.6. Given the camera and the world frames
C
,
W
at the different origins
O C ,O W , and that they are related to each other as
W R T , then the coordinates
of a point in one frame can be transformed linearly to those in the other as
( −−−→
C
=
O C P ) C = M E ( −−−→
O W P ) WH
(13.39)
where
O W P ) WH = ( −−−→
( −−−→
O W P ) W
1
M E =[ R , t ] ,
(13.40)
with
t =( −−−−→
O C O W ) C
(13.41)
4 Note that we construct matrices from other matrices by use of their symbols and brackets
[ ·, · ], and then multiply (!) these following the rules of block matrix operations in linear
algebra. A summary is given in the Appendix, Sect. 13.8.
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