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bTb
min
s 2
ζ
s 1
Σ i q i 2 / λ i
t
λ 3
λ 2
λ 1
max
Figure 5.5 Graphical method for the determination of critical point parameters for a three-
dimensional case; h ( t ) is given by the nonvertical dashed straight line for two different GTLS
problems (the horizontal line is the DLS); the solid curve is l ( t ).
t min
t min
B > 1
B < 1
A/(B
1)
ζ
ζ
1/(B 1)
1/(1
B)
A/(1 B)
Figure 5.6 Plots of the solution locus parameter as a function of the type of GeTLS problem
for all possible A and B .
1. The intersection for the maximum holds at t =+∞ ; it agrees with the
observation that the maximum for the DLS problem is at the TLS hyper-
plane origin.
2. The distance of a saddle to the asymptote at which its locus tends depends
on b T b .
The positions of the branches of the hyperbolas in the plane z i z j (see
Figures 5.7 and 5.8 for the two-dimensional case) depend on the signs of the
corresponding q i and q j [i.e., the signs of the coordinates of the OLS solution z
(see Theorem 101) because λ i 0 λ i ]. Hence, knowledge of the OLS solution
indicates the quadrant containing the solution locus for every plane z i z j .
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