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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
{Λ
1
,Λ
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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