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Ta b l e 6 Coefficients ( a i , b i ,and c i ) for FCULa and FCULb mapping functions (Mendes et al.
2002 )
FCULa
FCULb
10 7
10 7
a 0
(
12100
.
8
±
1
.
9
) ×
(
11613
.
1
±
1
.
6
) ×
10 9
10 8
a 1
(
1729
.
5
.
8
±
4
.
3
) ×
(
933
.
8
±
9
.
7
) ×
10 7
10 11
a 2
(
319
.
1
±
3
.
1
) ×
(
595
.
8
±
4
.
1
) ×
10 11
10 11
a 3
(
1847
.
8
±
6
.
5
) ×
(
2462
.
7
±
6
.
8
) ×
10 7
a 4
(
1286
.
4
±
2
.
2
) ×
10 7
10 7
b 0
(
30496
.
5
±
6
.
6
) ×
(
29814
.
1
±
4
.
5
) ×
10 8
10 7
b 1
(
234
.
6
±
1
.
5
) ×
(
56
.
9
±
2
.
7
) ×
10 6
10 10
b 2
(
103
.
5
±
1
.
1
) ×
(
165
.
5
±
1
.
1
) ×
10 10
10 10
b 3
(
185
.
6
±
2
.
2
) ×
(
272
.
5
±
1
.
9
) ×
10 7
b 4
(
302
.
0
±
5
.
9
) ×
10 5
10 6
c 0
(
6877
.
7
±
1
.
2
) ×
(
68183
.
9
±
9
.
1
) ×
10 7
10 6
c 1
( 197 . 2 ± 2 . 8 ) ×
( 93 . 5 ± 5 . 4 ) ×
10 5
10 9
c 2
( 345 . 8 ± 2 . 0 ) ×
( 239 . 4 ± 2 . 3 ) ×
10 9
10 9
c 3
( 106 . 0 ± 4 . 2 ) ×
( 30 . 4 ± 3 . 8 ) ×
10 5
c 4
( 230 . 8 ± 1 . 2 ) ×
two-color SLR measurements (the 2C-SLR formula). This formula was later studied
by several investigators (Greene and Herring 1986 ).
From the two-color SLR measurements theoretical path lengths
R 2 are
obtained (assume that the systemmeasures simultaneously individual optical paths).
With the 2C-SLR formula (Abshire and Gardner 1985 ), the chord (straight line)
distance
R 1 and
σ
can be calculated by adding the term
μ(R 2 R 1 )
to
R 1
σ = R 1 + μ(R 1 R 2 ),
(164)
where
k
1 )
μ =
1 ) ,
(165)
k
2 )
k
with k
being the dispersion factor. This factor depends on frequency and can be
calculated using (Edlén 1966 ; Abshire and Gardner 1985 )
i )
0
.
0164
λ
0
.
000228
λ
k
i ) =
0
.
9650
+
+
,
(166)
2
i
2
i
where
λ i is the i :th wavelength in meters.
The 2C-SLR formula presented in Eq. ( 164 ) remove the largest part of the total
propagation delay, namely that associatedwith the dry atmospheric density. However,
the water vapor density and curvature effects still remain (Abshire and Gardner 1985 ;
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