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matrix of the right metric tensor of the plane generated by developing the circular cylinder C
2 R
of radius ( I.31 ), namely the unit matrix G r =I 2 .
End of Lemma.
Definition I.10 (Generalized polycylindric projection, Airy optimum).
The generalized polycylindric projection of conformal type of ( I.33 )and( I.34 ) of the ellipsoid-of-
revolution E
2 R of radius ( I.31 ) is called Airy optimal if
the deviation from an isometry ( I.35 ) in terms of the left principal stretches 1 2 } , in particu-
lar ( I.34 ), averaged over a mapping area of interest, namely the surface integral ( I.36 ), is minimal
with respect to the unknown dilatation factor ρ 0 .
A 1 ,A 2 onto the developed circular cylinder C
1) 2 +( Λ 2
1) 2 ] / 2 ,
[( Λ 1
(I.35)
1
2 S
[( Λ 1 1) 2 +( Λ 2 1) 2 ]d S =min
ρ 0
J l A :=
.
(I.36)
area
End of Definition.
Let us refer to the representation of the areal elements { d S, S} of the ellipsoid-of-revolution
of Sect. I-1 . With the next step, we move on to Lemma I.11 for a representation of J l A subject to
Λ 1 = Λ 2 , in particular ( I.34 ).
Lemma I.11 (Generalized polycylindric projection, Airy distortion energy).
In case of the generalized polycylindric projection of conformal type, the left Airy distortion
energy J l A is the quadratic form in terms of the dilatation factor ρ 0 , in particular
2 c 01 ρ 0 + c 02 ρ 0 ,
J l A ( ρ 0 )= c 00
(I.37)
such that
c 00 =1 ,
c 01 = c 1 cos Φ 0 / 1
E 2 sin 2 Φ 0 ,
(I.38)
c 02 = c 2 cos 2 Φ 0 / (1
E 2 sin 2 Φ 0 )
hold .
End of Lemma.
Once we start from the proof of Lemma I.4 , the extension to the result of ( I.37 )and( I.38 ) with
respect to ( I.34 ) into Lemma I.11 is straightforward.
Question: “Where, with respect to the dilatation factor
ρ 0 , is the Airy distortion energy minimal?” Answer: “The
detailed answer is given in Lemma I.12 .”
 
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