Geography Reference
In-Depth Information
We depart from the representation of the meridian arc length as a function of the polar distance
Δ , the complement of the surface normal latitude Φ . Let us transform the integral kernel (which
is a function of Φ )to Φ (which is the circular reduced latitude). Such a polar coordinate is
generated by projecting a meridianal point P vertically onto a circle
A 1
of radius A 1 .Notethat
the geometrical situation is illustrated in Figs. 8.2 and 8.3 . Furthermore, note that the relations
Δ := π/ 2
S
Φ and Δ := π/ 2
Φ hold, and
E 2 ) Δ
0
d Δ
(1 −E 2 cos 2 Δ ) 3 / 2
f ( Δ )= A 1 (1
(8.25)
1
f ( Δ )= A 1 Δ
E 2 sin 2 Δ d Δ.
0
Φ and Φ
The transformatio n formula e Φ
Φ , respectively, are summarized in Box 8.4 ,
originating from X 2 + Y 2 = A 1 cos Φ and Z = A 2 sin Φ , taking reference to the semi-major
axis A 1 and the semi-minor axis A 2 . Here, we refer to
sin Φ
sin Φ =
1
E 2 cos 2 Φ
or
cos Δ
1
cos Δ =
,
E 2 sin 2 Δ
and
E 2 )
A 1 (1
A 1
E 2 sin 2 Δ ) 3 / 2 ,
1
E 2 cos 2 Δ ) 3 / 2 =
E 2 (1
(1
and
(8.26)
1
E 2
sin Δ
1
sin Δ =
E 2 sin 2 Δ
1
E 2
E 2 sin 2 Δ ) 3 / 2 cos Δ d Δ ,
cos Δ d Δ =
(1
1 − E 2
1 − E 2
d Δ = cos Δ
cos Δ
E 2 sin 2 Δ ) 3 / 2 d Δ =
d Δ ,
E 2 sin 2 Δ
(1
1
in order to have derived
E 2 sin 2 Δ ) 3 / 2 1
E 2 )
A 1 (1
A 1
E 2
1 − E 2 sin 2 Δ
d Δ ,
1 − E 2 (1
E 2 cos 2 Δ ) 3 / 2 d Δ =
(8.27)
(1
E 2 cos 2 Δ ) 3 / 2 d Δ = A 1 1 − E 2 sin 2 Δ d Δ .
A 1 (1 − E 2 )
(1
 
Search WWH ::




Custom Search