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r Λ, q = Q, A 1 ln tan π
1
E/ 2
p = P, λ = A 1
4 + Φ
E sin Φ
1+ E sin Φ
2
= r ln tan π
.
4 + φ
2
(1.222)
Gauss ( 1822 , 1844 ) made some special proposals how to choose the radius r of S
r in an optimal
way. Here, let us refer to Chap. 2 , where the Gauss projection E
2 is discussed in
detail. Here, we conclude with a representation of the left as well as the right inverse mapping Φ 1
A 1 ,A 1 ,A 2 S
r
P
l
and Φ r in terms of conformal coordinates (isometric, isothermal) of Box 1.30 , which specializes
Φ l and Φ r of Box 1.21 .
End of Solution (the fourth problem).
Box 1.30 (Representation of Φ l and Φ r in terms of conformal coordinates:
2
2
E
A 1 ,A 1 ,A 2 S
r ).
Φ l : X ( Λ, Φ )=
Φ r : x ( λ, φ )=
= E 1 A 1 cos Φ cos Λ
1 − E 2 sin 2 Φ
+
= e 1 r cos φ cos λ +
+ E 2 A 1 cos Φ cos Λ
1
+
+ e 2 r cos φ sin λ +
E 2 sin 2 Φ
E 2 )sin Φ
+ E 3 A 1 (1
1
=
+ e 3 r sin φ
=
(1.223)
E 2 sin 2 Φ
= E 1 A 1 cos f 1 ( Q/A 1 )cos( P/A 1 )
+= e 1 r cos( p/r )
1
cosh( q/r ) +
E 2 sin 2 f 1 ( Q/A 1 )
+ E 2 A 1 cos f 1 ( Q/A 1 ) sin( P/A 1 )
++ e 2 r sin( p/r )
1 − E 2 sin 2 f 1 ( Q/A 1 )
cosh( q/r ) +
E 2 )sin f 1 ( Q/A 1 )
1 − E 2 sin 2 f 1 ( Q/A 1 )
+ E 3 A 1 (1
.
+ e 3 r tanh( q/r ) .
Isoparametric mapping: p = P and q = Q.
2
A 1 ,A 1 ,A 2
2
Example 1.12 (Conformal mapping of an ellipsoid-of-revolution
E
toasphere
S
r :the
2
A 1 ,A 1 ,A 2
2
Universal Stereographic Projection (UPS) of type left
r , special Korn-
Lichtenstein equations, Cauchy-Riemann equations (d'Alembert-Euler equations)).
E
and right
S
Let us assume that we have found a solution of the left Korn-Lichtenstein equations of the
ellipsoid-of-revolution
2
A 1 ,A 1 ,A 2
E
parameterized by the two coordinates
{
Λ, Φ
}
which convention-
ally are called
. Similarly, let
us depart from a solution of the right Korn-Lichtenstein equations of the sphere
{
Gauss surface normal longitude, Gauss surface normal latitude
}
r parame-
S
terized by the two coordinates
{
λ, φ
}
which are called
{
spherical longitude, spherical latitude
}
.
 
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