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(iv)
If the relative eccentricity vanishes, E = 0, then we arrive at the special Hammer projection of
the sphere
A 1
S
subject to c 1 =2 ,c 2 =1 ,c 3 =1 / 2, and c 4 =1,namely
x =2 r ( Λ, Φ )cos α ( Λ, Φ ) , y = r ( Λ, Φ ) , sin α ( Λ, Φ ) ,
(H.93)
cos Φ sin Λ/ 2
sin Φ
1
1
cos α ( Λ, Φ )=
cos 2 Φ cos 2 Λ/ 2 , sin α ( Λ, Φ )=
cos 2 Φ cos 2 Λ/ 2 ,
(H.94)
r = A 2 1
cos Φ cos Λ/ 2 ,
(H.95)
x =2 A 1 2
1+cos Φ cos Λ/ 2 , y = A 1 2
cos Φ sin Λ/ 2
sin Φ
1+cos Φ cos Λ/ 2 .
(H.96)
End of Corollary.
As a visualization for the derived mapping equations for the ellipsoidal Hammer projection ,at
the beginning of this section, Fig. H.3 is given including the Tissot indicatrices .
Fig. H.3. The ellipsoidal Hammer projection, squared relative eccentricity E 2 =0 . 1
H-3 An Integration Formula
Equation ( H.28 ) may be written as an integration formula. The following relations ( H.97 )-( H.100 )
specify this integration formula. If the relative eccentricity approaches E = 0, then the radial
coordinate specializes to ( H.101 ) according to the L'Hopital Rule ( H.102 )and( H.103 ).
sin x 1+ p 2 sin 2 x d x =
2 cos x 1+ p 2 sin 2 x −
1
1+ p 2
2 p
p cos x
1+ p 2 ,
arcsin
(H.97)
subject to
 
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