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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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