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E
2
)(1 + 2
E
2
sin
2
Φ
)
A
1
(1
−
=
−
E
2
sin
2
Φ
)
5
/
2
cos
2
Φ
+sin
2
Φ
1+2
E
2
sin
2
Φ
(1
−
=
3
E
2
1+2
E
2
sin
2
Φ
−
(9.14)
E
2
)
(1
− E
2
sin
2
Φ
)
5
/
2
(cos
2
Φ
+2
E
2
sin
2
Φ
cos
2
Φ
+sin
2
Φ
+2
E
2
sin
4
Φ −
3
E
2
sin
2
Φ
)
A
1
(1
−
=
−
E
2
)
A
1
(1
−
E
2
(3 sin
2
Φ
2sin
2
Φ
cos
2
Φ
2sin
4
Φ
)] =
=
−
E
2
sin
2
Φ
)
5
/
2
[1
−
−
−
(1
−
E
2
)
A
1
(1
−
=
−
E
2
sin
2
Φ
)
5
/
2
(1
−
E
2
(3 sin
2
Φ
2sin
2
Φ
cos
2
Φ
2sin
2
Φ
+2sin
2
Φ
cos
2
Φ
)] =
[1
−
−
−
A
1
(1
− E
2
)
A
1
(1
− E
2
)
E
2
sin
2
Φ
)
5
/
2
(1
− E
2
sin
2
Φ
)=
−
=
−
E
2
sin
2
Φ
)
3
/
2
.
(1
−
(1
−
9-14 The Metric Tensor of the Sphere, the First Differential Form
Third, we compute the first differential form of the surface of type
sphere
.In(
9.15
)and(
9.16
),
r
is the radius of the sphere. The basis vectors finally lead to the elements of the
spherical metric
tensor
.
3
∂x
j
∂u
k
∂x
j
∂u
l
,
g
kl
=
g
k
|
g
l
=
j
=1
g
1
=
g
λ
:=
∂
x
∂λ
=
r
cos
φ
(
−
sin
λe
1
+cos
λe
2
)
,
(9.15)
g
2
=
g
φ
:=
∂
x
∂φ
=
−
r
(sin
φ
cos
λe
1
+sin
φ
sin
λe
2
−
cos
φe
3
)
,
e
(Gauss) :=
g
λ
|
g
λ
:=
g
λλ
=
g
11
=
r
2
cos
2
φ,
f
(Gauss) :=
g
λ
|
g
φ
:=
g
λφ
=
g
12
=
g
21
=
g
φλ
=0
,
(9.16)
:=
g
φφ
=
g
22
=
r
2
.
g
(Gauss) :=
g
φ
|
g
φ
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