Biomedical Engineering Reference
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and in matrix notation, respectively
2
4
3
5 h e i e j i
G 11
G 12
G 13
½¼
G 12
G 22
G 23
ð 3 : 71 Þ
G 13
G 23
G 33
with six independent coordinates
"
#
2
2
2
G 11 ¼ o u 1
oX 1
þ 1
2
ou 1
oX 1
þ o u 2
oX 1
þ o u 3
oX 1
"
#
2
2
2
G 22 ¼ o u 2
oX 2
þ 1
2
ou 1
oX 2
þ o u 2
oX 2
þ o u 3
oX 2
ð 3 : 72 Þ
"
#
2
2
2
G 33 ¼ o u 3
oX 3
þ 1
2
ou 1
oX 3
þ o u 2
oX 3
þ o u 3
oX 3
þ 1
2
G 12 ¼ G 21 ¼ 1
2
ou 1
oX 2
þ o u 2
oX 1
ou 1
oX 1
ou 1
oX 2
þ o u 2
oX 1
ou 2
oX 2
þ o u 3
oX 1
ou 3
oX 2
þ 1
2
G 13 ¼ G 31 ¼ 1
2
ou 1
oX 3
þ o u 3
oX 1
ou 1
oX 1
ou 1
oX 3
þ o u 2
oX 1
ou 2
oX 3
þ o u 3
oX 1
ou 3
oX 3
ð 3 : 73 Þ
þ 1
2
:
G 23 ¼ G 32 ¼ 1
2
ou 2
oX 3
þ o u 3
oX 2
ou 1
oX 2
ou 1
oX 3
þ o u 2
oX 2
ou 2
oX 3
þ o u 3
oX 2
ou 3
oX 3
Analogue to tensor representation ( 3.69 ), it can be seen using ( 3.72 ) and ( 3.73 )
that the elements of the principal diagonal G ii of G are dependent on the squares of
the displacement derivations, i.e. ð ou 1 = oX 1 Þ 2 and so on, and the elements of the
secondary diagonal G ij are dependent on the bilinear terms of the displacement
derivations, i.e. ð ou 1 = oX 1 Þð ou 1 = oX 2 Þ and so on.
Rigid Body Motion. Under the motion of a rigid body, the displacement vectors
of all material points are equal due to u ð X ; t Þ¼ u 0 . They are no longer position
dependent (cf. Fig. 3.8 b). According to ( 3.56 ), the displacement gradient vanishes
due to H ¼ u 0 0 : Using ( 3.57 ) this yields the deformation gradient to be
F ¼ I :
ð 3 : 74 Þ
Using ( 3.74 ) together with ( 3.65 ) and ( 3.69 ), the strain tensors yield
C ¼ B ¼ I
and
G ¼ 0
ð 3 : 75 Þ
where, in the case of no deformation (rigid body motion), only the GREEN-strain
tensor transforms into the zero tensor, and thus represents a ''true'' strain measure.
Furthermore, according to ( 3.70 ), ( 3.53 ) and ( 3.55 ) it remains dx ¼ dX and
dV ¼ dV 0 , which leads to constant edge lengths of a volume element and the
volume element itself remains unchanged in case of a rigid body motion. The body
thus does not experience any deformation.
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