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x = AΛ,
ln 1+ E sin Φ
1
=
y = A (1 E 2 )
4 E
2 E sin 1 Φ
E sin Φ +
(F.21)
E 2 sin 2 Φ
1
artanh( E sin Φ )+
.
= A (1 E 2 )
2 E
E sin Φ
E 2 sin 2 Φ
1
End of Corollary.
Proof.
For the proof, let us depart from the setup x = and y = f ( Φ )as special case of ( F.11 ) with
L ( Φ )=1and g ( Φ ) = 1 such that the equator is mapped equidistantly. The left Cauchy-Green
deformation tensor c AB is generated by c 11 = A 2 ,c 12 =0,and c 22 = f 2 ( Φ ) such that the left
principal stretches, following ( F.12 )-( F.14 ), amount to ( F.22 ), which leads by partial integration
(decomposition into fractions) subject to the condition f ( Φ = 0) = 0 directly to ( F.21 ).
N ( Φ )cos Φ , Λ 2 = f ( Φ )
A
Λ 1 =
M ( Φ ) ,
Λ 1 Λ 2 =1
(F.22)
d f = A 1 N ( Φ ) M ( Φ )cos Φ d Φ,
cos Φ
E 2 )
d f = A (1
E 2 sin 2 Φ ) 2 d Φ.
(1
End of Proof.
Corollary F.3 (Ellipsoidal equiareal projection of pseudo-sinusoidal type).
The ellipsoidal equiareal projection of pseudo-sinusoidal type (generalized Sanson-Flamsteed pro-
jection) in the class of pseudo-cylindrical projections is represented in terms of surface normal
longitude Λ and latitude Φ of
2
E
A,B by ( F.23 ) mapping a parallel circle equidistantly.
A cos Φ
x =
1
Λ,
E 2 sin 2 Φ
y ≈ A (1 − E 2 ) Φ + 3
8 E 2 (2 Φ − sin 2 Φ )+O( E 4 )
(F.23)
A Φ
8 E 2 (2 Φ +3sin2 Φ )+O( E 4 ) .
1
End of Corollary.
Proof.
For the proof, let us depart from the setup ( F.24 ), which leads under the postulate of an equiareal
mapping via ( F.8 ) of Corollary F.1 to ( F.25 ), expressing the arc length of the meridian, namely
in terms of the standard elliptic integral of second kind, here instead by series expansion.
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