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l
2
=
l
10
α
2
+2
l
10
l
01
αβ
+
l
01
β
2
+2
l
10
l
20
α
3
+
(3.137)
+2(
l
10
l
11
+
l
01
l
20
)
α
2
β
+2(
l
01
l
20
+
l
10
l
02
)
αβ
2
+2
l
01
l
02
β
3
+O
2
(
α
4
,β
4
)
,
l
3
=
l
10
α
3
+3
l
10
l
01
α
2
β
+3
l
10
l
01
αβ
2
+O
3
(
α
4
,β
4
)
.
Box 3.21 (Taylor series expansion of the latitude function
Φ
(
A, B
), Taylor polynomials).
ΔΦ
=
Φ
−
Φ
0
=
=
∂Φ
∂A
(
A
0
,B
0
)
ΔA
+
∂Φ
∂B
(
A
0
,B
0
)
ΔB
+
∂
2
Φ
∂
2
Φ
∂
2
Φ
+
1
2
∂A∂B
(
A
0
,B
0
)
ΔAΔB
+
1
∂A
2
(
A
0
,B
0
)(
ΔA
)
2
+
∂B
2
(
A
0
,B
0
)(
ΔB
)
2
+
2
+
1
6
∂
3
Φ
∂A
3
(
A
0
,B
0
)(
ΔA
)
3
+
1
∂
3
Φ
∂B
3
(
A
0
,B
0
)(
ΔB
)
3
+
(3.138)
6
∂
3
Φ
∂
3
Φ
+
1
2
∂A
2
∂B
(
A
0
,B
0
)(
ΔA
)
2
ΔB
+
1
∂A∂B
2
(
A
0
,B
0
)
ΔA
(
ΔB
)
2
+
+O
Φ
[(
ΔA
)
4
,
(
ΔB
)
4
]
,
2
ΔΛ
=
Λ
−
Λ
0
=:
l, ΔΦ
=
Φ
−
Φ
0
=:
b,
ΔA
=
A
−
A
0
=:
α, ΔB
=
B
−
B
0
=:
β.
(3.139)
Definition of partial derivatives:
b
10
:=
∂Φ
∂A
(
A
0
,B
0
)
,b
01
:=
∂Φ
∂B
(
A
0
,B
0
)
,
b
20
:=
1
9
∂
2
Φ
∂A
2
(
A
0
,B
0
)
,b
11
:=
∂A∂B
(
A
0
,B
0
)
,b
02
:=
1
∂
2
Φ
∂
2
Φ
∂B
2
(
A
0
,B
0
)
,
2
∂
3
Φ
∂
3
Φ
∂B
3
(
A
0
,B
0
)
,
b
30
:=
1
∂A
3
(
A
0
,B
0
)
,b
03
:=
1
(3.140)
6
6
∂
3
Φ
∂
3
Φ
∂A∂B
2
(
A
0
,B
0
)
.
b
21
:=
1
2
∂A
2
∂B
(
Λ
0
,B
0
)
,b
12
:=
1
2
Taylor series, powers of Taylor series:
b
=
b
10
α
+
b
01
β
+
b
20
α
2
+
b
11
αβ
+
b
02
β
2
+
b
30
α
3
+
b
21
α
2
β
+
b
12
αβ
2
+
b
03
β
3
+O
1
(
α
4
,β
4
)
,
b
2
=
b
10
α
2
+2
b
10
b
01
αβ
+
b
01
β
2
+2
b
10
b
20
α
3
+
+2(
b
10
b
11
+
b
01
b
20
)
α
2
β
+2(
b
01
b
20
+
b
10
b
02
)
αβ
2
+2
b
01
b
02
β
3
+O
2
(
α
4
,β
4
)
,
(3.141)
l
3
=
b
10
α
3
+3
b
10
b
01
α
2
β
+3
b
10
b
01
αβ
2
+O
3
(
α
4
,β
4
)
.
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