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
−
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