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U 2 ( t l )= Λ ( t l )
= constant
.
constant
t r
= λ ( t r )
= u 2 ( t r ) .
(1.137)
Φ ( t l )
t l
φ ( t r )
End of Example.
r , respectively, we enter Box 1.21 . Here, we compute
Φ l and Φ r in parameterized form, namely ( Λ, Φ )
l and
With these parameterized curves in
M
M
3 and ( λ, φ )
X ( Λ, Φ )
R
x ( λ, φ )
3 , respectively. The left and the right displacement field is used to derive the tangent vectors
R
X 1 ,
X 2 }
{
of type “right”. The inner products vanish according to
our test computations in Example 1.3 . In consequence, Ψ l = Ψ r = π/ 2andΣ l r = 0, i.e. no
angular distortion appears.
of type “left” and
{
x 1 , x 2 }
Box 1.21 (Angular shear or angular distortion).
Left vector field:
Right vector field:
X ( Λ, Φ )= E 1 A 1 cos Φ cos Λ
1 −E 2 sin 2 Φ +
x ( λ, φ )= e 1 r cos φ cos λ +
(1.138)
1 −E 2 sin 2 Φ + E 3 (1 E 2 ) A 1 sin Φ
1 −E 2 sin 2 Φ . + e 2 r cos φ sin λ + e 3 r sin φ.
+ E 2 A 1 cos Φ cos Λ
Left displacement field:
Right displacement field:
(1.139)
d t r + ∂φ d φ
d X = ∂Λ d Λ
d t l + ∂Φ d Φ
d t l . d x = ∂λ d λ
d t r .
d t l
d t l
d t r
d t r
1st left parameterized curve: 1st right parameterized curve:
Λ =1 ,
(1.140)
Φ =0 , d d t l = ∂Λ .
λ =1 ,
φ =0 ,
d x
d t r
= ∂λ .
2nd left parameterized curve:
2nd right parameterized curve:
Λ =0 ,
Φ =1 , d d t l = ∂Φ .
λ =0 ,
φ =1 ,
d x
d t r
= ∂φ .
(1.141)
Left angular shear:
Right angular shear:
∂Φ =0 , 0= ∂λ |
∂φ =
= ∂Λ |
X 1
X 2
X
x
|
{
x 1
|
x 2
}
,
(1.142)
π
π
cos Ψ l =0
Ψ l =
±
2 ,
±
2 = Ψ r
cos Ψ r =0 ,
Σ l = Ψ l
Ψ r =0 .
Σ r = Ψ r
Ψ l =0 .
1-8 Relative Angular Shear
A third multiplicative measure of deformation: relative angular shear, Cauchy-Green defor-
mation tensor, Euler-Lagrange deformation tensor.
The third multiplicative measure of deformation is the ratio Q l and Q r , respectively. This ratio
is also called relative angular shear . In particular
 
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