Global Positioning System Reference
In-Depth Information
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TABLE 4.8
Magnification Factor for Standard Ellipses
Probability 1 − α
n r
95%
98%
99%
1
20.00
50.00
100.00
2
6.16
9.90
14.10
3
4.37
6.14
7.85
4
3.73
4.93
6.00
5
3.40
4.35
5.15
6
3.21
4.01
4.67
8
2.99
3.64
4.16
10
2.86
3.44
3.89
12
2.79
3.32
3.72
15
2.71
3.20
3.57
[14
20
2.64
3.09
3.42
30
2.58
2.99
3.28
50
2.52
2.91
3.18
Lin
- ——
Lon
PgE
100
2.49
2.85
3.11
2.45
2.80
3.03
The magnification factor, 2 F 2 ,n r, α , as a function of the probability and the de-
gree of freedom, is shown in Table 4.8. The table shows immediately that a small
degree of freedom requires a large magnification factor to obtain, e.g., 95% prob-
ability. It is seen that in the range of small degrees of freedom, an increase in the
degree of freedom rapidly decreases the magnification factor, whereas with a large
degree of freedom, any additional observations cause only a minor reduction of the
magnification factor. After a degree of freedom of about 8 or 10, the decrease in the
magnification factor slows down noticeably. Thus, based on the speed of decreas-
ing magnification factor, a degree of 10 appears optimal, considering the expense of
additional observations and the little gain derived from them in the statistical sense.
For a degree of freedom of 10, the magnification factor is about 3 to cover 95%
probability.
The hypothesis (4.290) can readily be generalized to three dimensions encompass-
ing the Cartesian coordinates of a three-dimensiona l network station. The magnifica-
[14
tion factor of the respective standard ellipsoid is 3 F 3 ,n r, α for it to contain ( 1
)
probability. Similarly, the standard deviation of an individual coordin ate is co nverted
to a ( 1
− α
) probability confidence interval by multiplication with F 1 ,n r, α . These
magnification factors are shown in Figure 4.4 for
− α
0 . 05. For higher degrees of
freedom, the magnification factors converge toward the respective chi-square values
because of the relationship rF r, = χ
α =
r .
For drawing the confidence ellipse at station P i , we need the rotation angle ϕ
between the ( x i ) and ( z i ) coordinate systems as well as the semimajor and semiminor
axis of the ellipse. Let ( y i ) denotes the translated ( x i ) coordinate system through the
adjusted point x i , then Equation (4.296) becomes
R i y i
z i =
(4.299)
 
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