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example of an equiareal pseudo-azimuthal mapping, category B. The special case
g
Λ
= 1 trans-
forms the pseudo-azimuthal mapping, category B, back to the azimuthal mapping, category A.
det [C
l
G
−
l
]=1; here:
ff
R
2
sin
Δ
g
Λ
=1
.
(5.145)
End of Proof.
5-4 The Wiechel Polar Pseudo-Azimuthal Projection
A special variant of Lambert's equiareal polar azimuthal projection: the Wiechel polar
pseudo-azimuthal projection.
A special variant of Lambert's equiareal polar azimuthal projection has been given by
Wiechel
(
1879
). The direct equations for mapping the “sphere to plane” are presented in Box
5.22
and are illustrated in Fig.
5.30
. Thanks to the azimuthal function
α
=
g
(
Λ, Δ
)
=
Λ
(in general,
here we consider
α
=
Λ
+
Δ/
2), the
Wiechel map
is pseudo-azimuthal. A quick view to Wiechel's
pseudo-azimuthal map of Fig.
5.30
motivates the following interpretation: we see the polar vortex
at the North Pole directed to the Earth's rotation axis, namely
e
3
. Indeed, we compute the curl
or vortex of the placement vector
x
(
Λ, Δ
)=
e
1
x
(
Λ, Δ
)+
e
2
y
(
Λ, Δ
):
curl
x
(
Λ, Δ
)=
e
3
(
D
Λ
y
−
D
Δ
x
)
=
e
3
2
cos
Λ
+
Δ
R
cos(
Λ
+
Δ
)+2
R
sin
Δ
−
=0
.
(5.146)
2
Consult the original contribution of
Wiechel
(
1879
) for a deeper understanding. In particular,
enjoy his arguments for “a rotational graticule”. To become familiar with such a special pseudo-
azimuthal mapping “sphere to plane”, let us ask the following question.
Question: “Is the Wiechel pseudo-azimuthal projection
“sphere to plane” equiareal?” Answer: “Yes.”
For the proof, follow the lines of the proof outlined in Box
5.22
. First, we compute the left Jacobi
matrix constituted by the partial derivatives
D
Λ
x, D
Δ
x, D
Λ
y
,and
D
Δ
y
. Second, we derive the
left Cauchy-Green matrix by computing C
l
=J
l
J
l
. Third, we derive the left principal stretches,
the left eigenvalues of the matrix C
l
G
−
l
,namely
Λ
1
and
Λ
2
, from the trace tr
C
l
G
−
l
and the
determinant det
C
l
G
−
l
. Fourth,
Λ
1
Λ
2
= 1 proves an equiareal mapping.
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