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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 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 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 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 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 4 ) .
 
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