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⎡
⎤
R
cos
Φ
0
cos
U
−
V
sin
Φ
0
cos
U
⎣
⎦
,
X
(
U, V
)=[
E
1
,
E
2
,
E
3
]
R
cos
Φ
0
sin
U
V
sin
Φ
0
sin
U
R
sin
Φ
0
+
V
cos
Φ
0
−
⎡
⎤
R
cos
Φ
0
cos
U
R
cos
Φ
0
sin
U
R
sin
Φ
0
⎣
⎦
∈
S
1
R
cos
Φ
0
x
(
U
)=[
E
1
,
E
2
,
E
3
]
,
(4.5)
⎡
⎤
−
sin
Φ
0
cos
U
⎣
⎦
=:
C
Φ
.
Y
(
U
)=[
E
1
,
E
2
,
E
3
]
−
sin
Φ
0
sin
U
cos
Φ
0
Matrix of the metric:
2
+
V
2
2
,
G
11
=
R
2
cos
2
Φ
0
+ 1;
2
=
D
U
X
(
U, V
)
G
11
=
E
=
D
U
x
D
U
Y
(4.6)
G
12
=
G
21
=
F
=
D
U
x
(
U
)
|
Y
(
U
)
=
D
U
X
(
U, V
)
|D
V
X
(
U, V
)
,
G
12
=
G
21
= 0;
(4.7)
2
=
2
, G
22
= 1;
G
22
=
G
=
Y
(
U
)
D
V
X
(
U, V
)
(4.8)
G=
1+
R
2
cos
2
Φ
0
0
.
(4.9)
0
1
Definition 4.1 (Ruled surface.).
2
of
type
X
(
U, V
)=
x
(
U
)+
V
Y
(
U
), where
x
(
U
) is a differentiable curve and
Y
(
U
) is a vector field
along the curve
x
(
U
) which vanishes nowhere.
A surface is called
ruled surface
if there exists a parameterization of the continuity class
C
End of Definition.
The matrix of the metric, G, associated with a ruled surface is a typical element of this kind.
Compare with Box
4.2
, where we have computed the matrix G.
Box 4.2 (The matrix of the metric of a ruled surface).
2
+
V
2
2
=
D
U
X
(
U, V
)
2
,
G
11
=
E
=
D
U
x
D
U
Y
(4.10)
G
12
=
G
21
=
F
=
D
U
x
(
U
)
|
Y
(
U
)
=
D
U
X
(
U, V
)
|
D
V
X
(
U, V
)
,
(4.11)
2
=
2
,
G
22
=
G
=
Y
(
U
)
D
V
X
(
U, V
)
(4.12)
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