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Geodätische Koordinaten auf dem Rotationsellipsoid
Das Rotationsellipsoid mit Kreisform der Breitenkreise (in der Äquatorebene Radius der großen Halbachse A) und Ellipsenform bezüglich der Längenkreise. Kleine Halbachse an den Polen ist B.
Die w:Exzentrizität (Mathematik) gibt die Abplattung aufgrund der unterschiedlichen Länge von A und B an.
(
X
Y
Z
)
=
(
N
⋅
cos
U
⋅
cos
V
N
⋅
sin
U
⋅
cos
V
N
⋅
sin
V
(
1
−
E
2
)
)
{\displaystyle {\begin{pmatrix}X\\Y\\Z\end{pmatrix}}={\begin{pmatrix}N\cdot \cos {U}\cdot \cos {V}\\N\cdot \sin {U}\cdot \cos {V}\\N\cdot \sin {V}(1-E^{2})\end{pmatrix}}}
V
∈
(
−
π
2
;
π
2
)
U
∈
[
−
π
;
π
)
{\displaystyle V\in (-{\frac {\pi }{2}};{\frac {\pi }{2}})\,U\in [-\pi ;\pi )}
N
=
A
1
−
E
2
sin
2
V
{\displaystyle N={\frac {A}{\sqrt {1-E^{2}\sin ^{2}V}}}}
A und B bzw. E je nach Ellipsoid.
(Gaußsche) Tangentenvektoren [ Bearbeiten ]
Siehe Gaußsches Dreibein
g
→
1
=
x
→
U
=
{\displaystyle {\vec {g}}_{1}={\vec {x}}_{U}=}
g
→
2
=
x
→
V
=
{\displaystyle {\vec {g}}_{2}={\vec {x}}_{V}=}
g
→
3
=
x
→
U
(
u
)
×
x
→
V
(
v
)
|
|
x
→
U
(
u
)
×
x
→
V
(
v
)
|
|
=
{\displaystyle {\vec {g}}_{3}={\frac {{\vec {x}}_{U}(u)\times {\vec {x}}_{V}(v)}{||{\vec {x}}_{U}(u)\times {\vec {x}}_{V}(v)||}}=}
erste Fundamentalform [ Bearbeiten ]
erste Fundamentalgrößen [ Bearbeiten ]
Siehe hier :
g
11
=
x
→
U
⋅
x
→
U
=
N
2
cos
2
V
{\displaystyle g_{11}={\vec {x}}_{U}\cdot {\vec {x}}_{U}=N^{2}\cos ^{2}V}
g
12
=
G
21
=
x
→
U
⋅
x
→
V
=
0
{\displaystyle g_{12}=G_{21}={\vec {x}}_{U}\cdot {\vec {x}}_{V}=0}
g
22
=
x
→
V
⋅
x
→
V
=
M
2
{\displaystyle g_{22}={\vec {x}}_{V}\cdot {\vec {x}}_{V}=M^{2}}
erster Fundamentaltensor [ Bearbeiten ]
G
=
(
g
11
g
12
g
21
g
22
)
=
(
N
2
cos
2
V
0
0
M
2
)
=
(
N
2
cos
2
V
0
0
N
2
(
1
−
E
2
)
2
(
1
−
E
2
sin
2
V
)
2
)
{\displaystyle \mathbf {G} ={\begin{pmatrix}g_{11}&g_{12}\\g_{21}&g_{22}\end{pmatrix}}={\begin{pmatrix}N^{2}\cos ^{2}V&0\\0&M^{2}\end{pmatrix}}={\begin{pmatrix}N^{2}\cos ^{2}V&0\\0&N^{2}{\frac {(1-E^{2})^{2}}{(1-E^{2}\sin ^{2}V)^{2}}}\end{pmatrix}}}
Inverser erster Fundamentaltensor [ Bearbeiten ]
G
−
1
=
(
g
11
g
12
g
21
g
22
)
=
1
1
(
0
0
0
0
)
{\displaystyle \mathbf {G} ^{-1}={\begin{pmatrix}g^{11}&g^{12}\\g^{21}&g^{22}\end{pmatrix}}={\frac {1}{1}}{\begin{pmatrix}0&0\\0&0\end{pmatrix}}}
zweite Fundamentalform [ Bearbeiten ]
zweifache Ableitungen [ Bearbeiten ]
x
→
u
u
=
{\displaystyle {\vec {x}}_{uu}=}
x
→
u
v
=
{\displaystyle {\vec {x}}_{uv}=}
x
→
v
v
=
{\displaystyle {\vec {x}}_{vv}=}
zweite Fundamentalgrößen [ Bearbeiten ]
Hier nachschauen!
b
11
=
x
→
u
u
⋅
n
→
=
{\displaystyle b_{11}={\vec {x}}_{uu}\cdot {\vec {n}}=}
b
12
=
b
21
=
x
→
u
v
⋅
n
→
{\displaystyle b_{12}=b_{21}={\vec {x}}_{uv}\cdot {\vec {n}}}
b
21
=
x
→
v
v
⋅
n
→
=
{\displaystyle b_{21}={\vec {x}}_{vv}\cdot {\vec {n}}=}
zweiter Fundamentaltensor [ Bearbeiten ]
B
=
(
b
11
b
12
b
21
b
22
)
=
(
L
M
M
N
)
=
(
0
0
0
0
)
{\displaystyle \mathbf {B} ={\begin{pmatrix}b_{11}&b_{12}\\b_{21}&b_{22}\end{pmatrix}}={\begin{pmatrix}L&M\\M&N\end{pmatrix}}={\begin{pmatrix}0&0\\0&0\end{pmatrix}}}
Siehe hier . Mit u1 = u, u2 = v.
α
=
1
{\displaystyle \alpha =1}
,
β
=
1
{\displaystyle \beta =1}
,
γ
=
1
{\displaystyle \gamma =1}
Γ
11
1
:=
1
2
g
11
(
∂
g
11
∂
u
1
+
∂
g
11
∂
u
1
−
∂
g
11
∂
u
1
)
+
1
2
g
12
(
∂
g
12
∂
u
1
+
∂
g
21
∂
u
1
−
∂
g
11
∂
u
2
)
=
{\displaystyle \Gamma _{11}^{1}:={\frac {1}{2}}g^{11}({\frac {\partial g_{11}}{\partial u^{1}}}+{\frac {\partial g_{11}}{\partial u^{1}}}-{\frac {\partial g_{11}}{\partial u^{1}}})+{\frac {1}{2}}g^{12}({\frac {\partial g_{12}}{\partial u^{1}}}+{\frac {\partial g_{21}}{\partial u^{1}}}-{\frac {\partial g_{11}}{\partial u^{2}}})=}
α
=
2
{\displaystyle \alpha =2}
,
β
=
1
{\displaystyle \beta =1}
,
γ
=
1
{\displaystyle \gamma =1}
Γ
12
1
:=
1
2
g
11
(
∂
g
11
∂
u
2
+
∂
g
12
∂
u
1
−
∂
g
21
∂
u
1
)
+
1
2
g
12
(
∂
g
12
∂
u
2
+
∂
g
22
∂
u
1
−
∂
g
21
∂
u
2
)
=
{\displaystyle \Gamma _{12}^{1}:={\frac {1}{2}}g^{11}({\frac {\partial g_{11}}{\partial u^{2}}}+{\frac {\partial g_{12}}{\partial u^{1}}}-{\frac {\partial g_{21}}{\partial u^{1}}})+{\frac {1}{2}}g^{12}({\frac {\partial g_{12}}{\partial u^{2}}}+{\frac {\partial g_{22}}{\partial u^{1}}}-{\frac {\partial g_{21}}{\partial u^{2}}})=}
α
=
1
{\displaystyle \alpha =1}
,
β
=
2
{\displaystyle \beta =2}
,
γ
=
1
{\displaystyle \gamma =1}
Γ
11
2
:=
1
2
g
21
(
∂
g
11
∂
u
1
+
∂
g
11
∂
u
1
−
∂
g
11
∂
u
1
)
+
1
2
g
22
(
∂
g
12
∂
u
1
+
∂
g
21
∂
u
1
−
∂
g
11
∂
u
2
)
=
{\displaystyle \Gamma _{11}^{2}:={\frac {1}{2}}g^{21}({\frac {\partial g_{11}}{\partial u^{1}}}+{\frac {\partial g_{11}}{\partial u^{1}}}-{\frac {\partial g_{11}}{\partial u^{1}}})+{\frac {1}{2}}g^{22}({\frac {\partial g_{12}}{\partial u^{1}}}+{\frac {\partial g_{21}}{\partial u^{1}}}-{\frac {\partial g_{11}}{\partial u^{2}}})=}
α
=
1
{\displaystyle \alpha =1}
,
β
=
1
{\displaystyle \beta =1}
,
γ
=
2
{\displaystyle \gamma =2}
Γ
21
1
=
Γ
12
1
{\displaystyle \Gamma _{21}^{1}=\Gamma _{12}^{1}}
α
=
2
{\displaystyle \alpha =2}
,
β
=
1
{\displaystyle \beta =1}
,
γ
=
2
{\displaystyle \gamma =2}
,
Γ
12
2
:=
1
2
g
11
(
∂
g
21
∂
u
2
+
∂
g
12
∂
u
2
−
∂
g
22
∂
u
1
)
+
1
2
g
12
(
∂
g
22
∂
u
2
+
∂
g
22
∂
u
2
−
∂
g
22
∂
u
2
)
=
{\displaystyle \Gamma _{12}^{2}:={\frac {1}{2}}g^{11}({\frac {\partial g_{21}}{\partial u^{2}}}+{\frac {\partial g_{12}}{\partial u^{2}}}-{\frac {\partial g_{22}}{\partial u^{1}}})+{\frac {1}{2}}g^{12}({\frac {\partial g_{22}}{\partial u^{2}}}+{\frac {\partial g_{22}}{\partial u^{2}}}-{\frac {\partial g_{22}}{\partial u^{2}}})=}
α
=
1
{\displaystyle \alpha =1}
,
β
=
2
{\displaystyle \beta =2}
,
γ
=
2
{\displaystyle \gamma =2}
Γ
21
2
=
Γ
12
2
{\displaystyle \Gamma _{21}^{2}=\Gamma _{12}^{2}}
α
=
2
{\displaystyle \alpha =2}
,
β
=
2
{\displaystyle \beta =2}
,
γ
=
2
{\displaystyle \gamma =2}
Γ
22
2
:=
1
2
g
21
(
∂
g
21
∂
u
2
+
∂
g
12
∂
u
2
−
∂
g
22
∂
u
1
)
+
1
2
g
22
(
∂
g
22
∂
u
2
+
∂
g
22
∂
u
2
−
∂
g
22
∂
u
2
)
=
{\displaystyle \Gamma _{22}^{2}:={\frac {1}{2}}g^{21}({\frac {\partial g_{21}}{\partial u^{2}}}+{\frac {\partial g_{12}}{\partial u^{2}}}-{\frac {\partial g_{22}}{\partial u^{1}}})+{\frac {1}{2}}g^{22}({\frac {\partial g_{22}}{\partial u^{2}}}+{\frac {\partial g_{22}}{\partial u^{2}}}-{\frac {\partial g_{22}}{\partial u^{2}}})=}
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