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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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