m the
f all
rix Q
(7)
(8)
rix Q
(9)
(10)
rix Q
not
tween
, at-
f the
e in-
rix Q
(11)
(12)
cura-
ition
Wong,
does
f the
ce is
andom
(13)
T
Lou
ratic
3 Of
func-
ix)
(14)
int,
15)
The expression Hip(X, Y,2) j-K? from equation (15),
for a specific value of K, is an ellipsoid boun-
ded by a parallelipiped with the dimensions 2KÜy
the direction of X, 2K(0y in the direction of Y
and 2K0, in the direction of Z. Such an ellipsoid
is known as an ellipsoid of constant probability
and the value of such probability depends on the
selected value of K.
In the shifted coordinate system X',Y' ;2', consi-
dering the ellipsoid with K=1 as a representativ
one, the standard ellipsoid is obtained:
x'2 Y'2 712
+ = + = | (16)
dx ox gà
the axes of the ellipsoid coincide with the axes
of a rotated coordinate system.
The system X',Y',Z' is obtained from the original
system X,Y,Z by three rotations w, f, X about the
X',Y',Z' axes respectively. With respect to this
new system, it becomes clear that Gy:7 a, Gyr = b,
(7v= c and the new random variables X' Y' D are
uncorrelated, such thatOy:y: 7Oyi7 7 0,1 7:70.
Consequently, through the transformation from X;
Y,Z to X',Y',Z' it was possible to replace a set
o three dimensions of correlated random varia-
bles by another set of the same dimensions of un-
correlated random variables.
The transformation matrix can be constructed by
determining the normalized eigenvectors of the
covariance matrix and using them as columns. This
is equivalent to diagonalizing the covariance ma-
trix 5., since the resulting covariance matrix of
the uncorrelated set of random variables X',Y',Z'
is always in diagonal form. The elements of this
diagonal matrix are the eigenvalues A 15 92, À3 of
the original covariance matrix S and the values
of the semiaxes a, 5b, c, of the ellipsoid can be
readily shown to be the square roots of the ei-
genvalues Ar» A»; Az
In actual computations, the semiaxes a, b, c of
error ellipsoid are determined by diagonalizing
the covariance matrix =; ; respectively:
as
"RIS
(17)
pc 0.20.1020 0,1 A. 9.0
0 Cy 0 0 »2 0 = 0 A2 5 |
0
0 0 Gy o 9 2 d
where R is an orthogonal matrix whose columns are
the normalized eigenvectors of the matrix >-; M
à», À3 are the eigenvalues of the matrix s and
the X',Y',Z' is a rotated coordinate system uch
that the random variables in the directions of
its axes are uncorrelated.
The computational flow itself, used to evaluate
the accuracy of photogrammetric determination of
position in threedimensional space, is actually
quite short and consists in the following major
steps :
Let 5; be a covariance matrix of the coordinates
of the triangulated j point obtained from the
least squares adjustment (12). Furthermore, let
the eigenvalue equation be defined by the charac-
teristic matrix equation:
(5 - AI)x = 0 (18)
which represents a set of homogeneous linear equ-
ations,
641
The characteristics equation of the covariance
matrix 2;is evaluated as:
2 2 2
eod C Oxv| Py Gyz| |x Gxzp _
(=A)z +Tr (= NS - 2|* + 2 =0
3 yx 714 Poy & | |%x 67 3
(19)
where :
Tr( 2) 04 qz- trace of the covariance matrix
[Ej toni of the =; covariance matrix
Since the matrix S; 02) is symmetric, then the
eigenvalues are real and the eigenvectors are all
mutually yt that is:
XIX. -X X-0 (20)
Let the three eigenvectors of the covariance ma-
trix 2 be denoted as XA,,; XA2> XA3,respectively:
X4 Xi X 1
Xa at X2 bh. Fags 1% of XA, = |X 5 (21)
X X
3 3 3
A Az ^s
For an eigenvalue A;, (i=1,2,3), we solve the set
of homogeneous linear equations:
gx À; Üxy Üxz XI 0
Ex Ay Oy; lie] «lo (22)
Üzx Üzy 027 =A; X, A 0
The eigenvalues and eigenvectors for the matrix Z;
are evaluated by an iterative procedure which con
sists in the following steps:
A. From Eq.(22), for i71 it results:
=6Gû
a) Aykı 76. ox? CO S +02 5
c) ÀX3 "Üzy X4 *GzyX) + 0x3
At the first iteration, for X) x yx.
from Eq.(23c) we obtain:
A= Try + Po (24)
At the second iteration the computed value of
can then be substituted into Eqs.(23a,b) to solve
for Xy <> X9 and Aq as below:
1
X 9T RA, Oso r1 D
1
X= SA Trust 6 + 0 yz) (25)
=0 x + X +02
M zx | zy 2 07
The iterations are stopped after the solutions
have been checked to be convergent. At the end of
the k-th iteration, the solutions are:
1
1,k 1,k=1 (1,%~1) 79
1
1
xl ‚K LA Gu ne fux M 02
(26)