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=
1
4
[(
f
2
)
]
2
h
2
=
=
1
4
[(
f
2
)
]
2
cos
2
Δg
2
(
Δ
) =
(18.16)
=
1
4
[(
f
2
)
]
2
cos
2
Δ
4
R
4
tan
2
Δ
[(
f
2
)
]
2
=
=
R
4
sin
2
Δ.
End of Proof.
Proof.
tr[C
l
G
−
l
]=
=
c
11
G
−
1
11
+
c
22
G
−
1
22
=
=
f
2
h
2
(
R
2
sin
2
Δ
)
−
1
+(
f
2
h
2
Λ
2
+
f
2
)(
R
2
)
−
1
=
1
1
R
2
sin
2
Δ
f
2
g
2
cos
2
Δ
+
R
2
[
f
2
(
g
cos
Δ
g
sin
Δ
)
2
Λ
2
+
f
2
] =
=
−
(18.17)
=4
R
2
f
2
[(
f
2
)
]
2
+
f
2
2
R
2
cos
Δ
(1 + tan
2
Δ
)
(
f
2
)
Λ
2
+
f
2
,
2
+
1
R
2
2
R
2
sin
Δ
2
R
2
sin
Δ
tan
Δ
(
f
2
)
[(
f
2
)
]
2
(
f
2
)
−
−
det[G
l
]=
R
4
sin
2
Δ.
(18.18)
End of Proof.
18-2 Special Pseudo-Conic Projections Based Upon the Sphere
The Stab-Werner mapping and the Bonne mapping. The mapping equations and the prin-
cipal stretches. Tissot indicatrix.
We use the setup (“Ansatz”)
r
(
Δ
)=
f
(
Δ
)=
aΔ
+
b, f
(
Δ
)=
a.
(18.19)
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