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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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