Full text: XVIIth ISPRS Congress (Part B5)

AQ ALI eere for Ag) = Ag) 
BO CB Ce for Aa — An) 
ADA = AD AD ren for Ar) = Arc) 
b® = b®): 
i k 
pO = p 
6) nd 
by = by 
i k 
pO = p 
Before these six equations can be added as constraints 
of the bundle adjustment, the formulas must be linarized 
with respect to the original exterior orientation parameters 
of the images (the perspective center and the three rotation 
angles of each image). This is rather complicated as the 
relative rotation matrices depend on parameters of both 
photos. 
The distance between the two perspective centers of any 
image-pair is constrained, which is the base-distance do that 
was measured by theodolites (7). Its accuracy is about 0.5 
mm. This constraint defines the scale of the local 
coordinate system in which 3-dimensional positioning is 
possible. 
  
d, 2 A (Xi — Xp)? + (YL — YRŸ + (ZL — Zr)? 
= Wb2 + b3 + b2 (7) 
with: XL, YL #1. coordinates of the left perspective 
center, 
XmYm ZR... coordinates of the right perspective 
center, 
NE distance measured between 
perspective centers, 
bx, by, b;......... components of the base vector. 
This constraint is only specified for one stereo-pair; all 
other base distances are automatically equaled by condition 
(6). Therefore, there are (m-1) relative orientation 
constraints for m stereo-pairs, and one base-distance 
observation. 
By collecting all the formulas mentioned before (1), (6), 
(7), and writing a system of observation equations and 
constraints, we get (8). The least squares solution is 
computed by (9). 
(8) 
b 
observation equations: v = A X — 
Iz 
px 
+ 
le 
constraints: EG 
   
  
  
    
  
    
    
  
    
  
   
  
  
  
  
  
  
  
   
  
  
  
  
  
   
  
  
   
   
   
  
   
  
  
  
  
  
   
  
  
  
   
   
  
   
    
  
  
  
  
  
  
    
    
with: A... linearized collinearity equations (1) and 
distance equation (7), 
dee unknown orientation parameters: 
Xp: Jp. €, A], A2, A3, A4, A5, AG for each camera, 
Xo, Yo, Zo, 0, 9, Kfor each image. 
I se discrepancies (observation minus 
approximation), 
D... linearized constraints of the relative 
orientation (6), 
PA absolute terms of constraints, 
a ee residuals of the observations, 
DE zero vector. 
jen Bt I= | AT] 
_— = -—- 9 
B 9 -t 2 
  
: Once these orientation parameters (x) are available, 3- 
dimensional coordinates can be computed for any point 
identified in both images. This is useful for measuring 
spatial distances or for creating local 3-dimensional models 
of small objects in the field of view of the stereo-vision 
system. However, the positions are only defined in a local 
coordinate system relative to the two cameras. These 
coordinates are referred to as local camera coordinates (X... 
Y., Zc) and will be transformed into a global system in the 
next chapter. 
4. ABSOLUTE POSITIONING 
The local coordinate system derived above corresponds 
to a stereo-model. To obtain absolute positions of points 
and features the absolute orientation of this model must be 
established. It consists of six parameters (3 translations and 
3 rotations) to convert points from the camera system (Xc, 
Yc, Zc) into a topocentric system (Xt, YT, ZT) with its 
origin at the GPS antenna, the XT axis pointing east, the YT 
axis pointing north, and the Zr axis identical to the vertical 
at the ellipsoid. The scales of the two coordinate systems 
are equivalent. The six transformation parameters are 
derived from the GPS position of the van (3 coordinates, 
which correspond to 3 translations) and the inertial 
measurements (gyros), which define 3 rotations (direction, 
pitch, roll). To visualize this transformation in a better 
way, it is separated into two steps: 
4.4 Transformation to a Vehicle System 
The vehicle coordinate system (Xy, Y y, Z,) is directly 
connected to the van; it is defined by the Yy-axis pointing 
in the driving direction and the Xy-axis parallel to the left 
image plane, as well as to the rear axle of the vehicle. The 
Zy-axis is vertical if the van is positioned on an horizontal 
surface. The vehicle coordinate system is assumed to be 
parallel to the gyro-axes of the inertial system. This 
coordinate system can be found by repeated measurements 
of the GPS antenna and the cameras by theodolite
	        
Waiting...

Note to user

Dear user,

In response to current developments in the web technology used by the Goobi viewer, the software no longer supports your browser.

Please use one of the following browsers to display this page correctly.

Thank you.