Geography Reference
In-Depth Information
F
2
(
Φ
)+
G
2
(
Φ
)d
Φ,
f
(
Φ
)
F
2
(
Φ
)+
G
2
(
Φ
)
=1
F
(0)
F
(
Φ
)
d
f
=
F
(
Φ
)
F
(0)
Λ
1
Λ
2
=1
⇒
⇔
Φ
F
(
Φ
)
F
2
(
Φ
)+
G
2
(
Φ
)d
Φ
+const
.,
1
F
(0)
f
(0) = 0
⇒
f
(
Φ
)=
(14.54)
0
f
(0) = 0
⇒
const
.
=0
.
The following formulae define the general mapping equations and the left principal stretches for
an equiareal cylindric mapping.
=
, Λ
1
=
F
(0)
x
y
F
(0)
Λ
F
(0)
0
F
(
Φ
)
F
2
(
Φ
)+
G
2
(
Φ
)d
Φ
F
(
Φ
)
,
1
Λ
2
=
F
(
Φ
)
1
Λ
1
.
F
(0)
=
(14.55)
14-34 An Example (Mapping the Torus)
A
1
B
, especially for the parameter range
A>B,
0
<U<
2
π
,
The torus is the
product manifold
S
×
S
and 0
<V <
2
π
.
⎡
⎤
⎡
⎤
⎡
⎤
X
Y
Z
(
A
+
B
cos
V
)cos
U
(
A
+
B
cos
V
)sin
U
B
sin
V
(
A
+
B
cos
Φ
)cos
Λ
(
A
+
B
cos
Φ
)sin
Λ
B
sin
Φ
⎣
⎦
=
⎣
⎦
=
⎣
⎦
.
(14.56)
The torus is the special surface which is generated by rotating a circle of radius
B
relative to a
circle of radius
A>B
around the center of the circle.
F
(
Φ
)=
A
+
B
cos
Φ, G
(
Φ
)=
B
sin
Φ,
U
=
Λ
= arctan
Y
Z
√
X
2
+
Y
2
X
, V
=
Φ
= arctan
A
.
(14.57)
−
Let us summarize in Box
14.3
the (left) tangent vectors and the (left) coordinates of the metric
tensor of the torus.
Box 14.3 (A special rotational figure: the torus).
Left tangent vectors:
G
Λ
:=
∂
X
∂Λ
=
−
E
1
(
A
+
B
cos
Φ
)sin
Λ
+
E
2
(
A
+
B
cos
Φ
)cos
Λ,
(14.58)
G
Φ
:=
∂
X
∂Φ
=
−
E
1
B
sin
Φ
cos
Λ
−
E
2
B
sin
Φ
sin
Λ
+
E
3
B
cos
Φ,
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