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e 22
;
K 1 G 22
×
(1.115)
( e 12
K 1 G 12 )
2nd left eigencolumns ,K 2 :
F 12
F 22
=
1
G 22 ( e 11
K 2 G 12 ) 2 ×
K 2 G 11 ) 2
2 G 12 ( e 11
K 2 G 11 )( e 12
K 2 G 12 )+ G 11 ( e 12
;
( e 12
K 2 G 12 )
e 11 − K 2 G 11
×
(1.116)
1st right eigencolumns 1 :
f 11
f 21
=
1
g 11 ( E 22
κ 1 g 12 ) 2 ×
(1.117)
κ 1 g 22 ) 2
2 g 12 ( E 12
κ 1 g 12 )( E 22
κ 1 g 22 )+ g 22 ( E 12
E 22
;
κ 1 g 22
×
( E 12
κ 1 g 12 )
2nd right eigencolumns, κ 2 :
f 12
f 22
=
1
g 22 ( E 11
κ 2 g 12 ) 2 ×
(1.118)
κ 2 g 11 ) 2
2 g 12 ( E 11
κ 2 g 11 )( E 12
κ 2 g 12 )+ g 11 ( E 12
( E 12 − κ 2 g 12 )
E 11 − κ 2 g 11
.
×
End of Lemma.
The proof of these relations follows the line of thought of the proof of Lemma 1.6 . Accordingly,
we skip any proof here.
The canonical forms of the scale difference (d s ) 2
(d S ) 2 and (d S ) 2
(d s ) 2 , respectively, have been
interpreted as
1
1
left Euler-Lagrange circle
S
right Euler-Lagrange circle
S
versus
versus
left Euler-Lagrange ellipse
right Euler-Lagrange ellipse
(1.119)
1
K 1 , K 2
1
κ 1 , κ 2
E
( K i > 0
i =1 , 2) , and
E
( κ i > 0
i =1 , 2) ,
left Euler-Lagrange hyperbola
right Euler-Lagrange hyperbola
1
K 1 , K 2
1
K 1 , K 2
H
( K 1 > 0 ,K 2 < 0) ,
H
( κ 1 > 0 2 < 0) ,
r , respectively. A deforma-
tion portrait with a positive eigenvalue K (E l , G r )or κ (E r , G l ) is referred to as extension , with
a negative eigenvalue K (E l , G r )or κ (E r , G l )as compression . Obviously, Cauchy-Green deforma-
tion and Euler-Lagrange deformation are related as outlined in Corollary 1.9 . The four cases of
the eigenspace analysis of the left and the right Euler-Lagrange deformation are illustrated in
Figs. 1.12 , 1.13 , 1.14 ,and 1.15 .
l and the right tangent space T u R
on the left tangent space T U M
M
 
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