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Theorem 22.2 (Harmonic maps, isometric coordinates (conformal, isothermal) of an ellipsoid of
revolution, variational formulation).
Let x = ξ ( q,l ) ,y = η ( q,l ) denote the mapping equations in terms of isometric coordinates (con-
formal, isothermal) of Mercator type of
2
2 subject to the Reference Meridian Strip L 0 ,
E
A 1 ,A 2 P
namely
2
( q,l ) ∈{ ( q,l )
|L W − L 0 ≤ l ≤ L E − L 0 ,Q s − Q 0 ≤ q ≤ Q N − Q 0 }
(22.41)
namely to Cartesian coordinates ( x, y ) P
2 of the chart {
2 ij } of the ellipsoid of revolution
E
A 1 ,A 2 , coordinated by ( q,l ). The functions ξ ( q,l ) ( q,l ) are assumed to be analytical. If the
distortion energy
L E
dL Q N
Q S
1
2
dQA 2 ( Q ) tr C l G l =min
ξ,η
(22.42)
L W
is minimal over a Reference Meridian Strip {L w ≤ L ≤ L E ,Q S ≤ Q ≤ Q N } with respect to the
West-East isometric longitude L w ,L E and South-North isometric latitude Q S ,Q N of type fixed
boundaries.
L E
dL Q N
Q S
dQ ξ L + ξ Q + η L + η Q = in
ξ ( Q,L ) ( Q,L )
1
2
(22.43)
L W
l E
dl q N
q S
dq ξ l + ξ q + η l + η q =min
ξ ( q,l ) ( q,l )
1
2
(22.44)
l W
l E
dl q N
q S
dq
=min
ξ ( q,l ) ( q,l )
1
2
gradξ 2
gradη 2
+
(22.45)
l W
is assumed to be minimal the mapping equations, namely the functions ξ ( q,l ) ( q,l )are har-
monic,
Δξ ( q,l )=0 ,Δη ( q,l )=0 ,
(22.46)
Λ 2 ( Q ) [ 2
∂l 2 + 2
1
Δ :=
∂q 2 ]
(22.47)
is the Laplace-Beltrami operator in isometric coordinates of Mercator type subject to
G l = Λ 2 ( Q ) 10
(22.48)
01
C l = ξ l + η l η l η q
(22.49)
η q
η l η q
The coordinates of the left metric tensor G l of conformal type and the coordinates of the left
Cauchy-Green deformation tensor C l where the left factor of conformality is given by
A 1 cos 2 ( lam 1 Q )
A 1 cos 2 Q
1 − E 2 sin 2 Q
A 2 ( Q )=
1 − E 2 sin 2 ( lam 1 Q ) =
(22.50)
expQ =tan π
1 E sin B
1+ E sin B
E/ 2
4 + B
(22.51)
2
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