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p 2 := X 2 + Y 2 , A 2 = A 1 (1 − E 2 ) , Z = (1 E 2 ) A 1 sin Φ
1
(19.21)
E 2 sin 2 Φ
A 1 cos Φ
1
p =
.
(19.22)
E 2 sin 2 Φ
We use the postulate of an equidistant mapping on the parallel circle-of-reference Φ 0 .
A 1 cos Φ 0
1
Λ = f ( Φ 0 ) α
E 2 sin 2 Φ 0
1 − E 2 cos 2 Δ 0 Λ = c 1+ E cos Δ 0
n
E/ 2
A 1 sin Δ 0
tan Δ 0
2
cos Δ 0 Λ
1
E cos Δ 0
(19.23)
1+ E cos Δ 0
1
−n
E/ 2
A 1 tan Δ 0
tan Δ 0
2
1
c =
E cos Δ 0
E 2 cos 2 Δ 0
α
r
=
,
f ( Δ )
tan 2
tan Δ 2
E/ 2 n
1 E cos Δ 0
1
A 1 tan Δ 0
1+ E cos Δ
1+ E cos Δ 0
f ( Δ )=
1 − E 2 cos 2 Δ 0
(19.24)
E cos Δ
E
1+ E sin Φ
1+ E sin Φ 0
1
tan 4
2
n
Φ
E 2 sin 2 Φ 0
A 1
tan 4
Φ 2
=
tan Φ 0 1
.
E 2 sin 2 Φ
1
E 2 sin 2 Φ 0
19-222 Conformal Mapping: The Variant of Type Equidistant on Two Parallel Circles (Lambert
Conformal Mapping)
We then consider the variant of type equidistant on two parallel circles . In this context, the
projection constant n is determined by the postulate of an equidistant mapping on two parallel
circles fixed by Δ 1 = 2 − Φ 1 and Δ 2 = 2 − Φ 2 .
 
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