Biomedical Engineering Reference
In-Depth Information
Fig. 7 Elastic part of the stress (a) and three nonlinear functions k
1
(b), k
2
(c) and k
3
(d) for the
fitted Adaptive QLV model [
55
]. Gray circles are calibrated values based on experimental data
and black curves are cubic spline interpolations
e
t
=
s
i
X
3
Þ þ
0
:
0667
20
e
T
=
s
i
1
r
Hn
ð
t
Þ¼
r
o
0
:
0667n
ð
A
i
0
:
0667
ð
n
1
Þ
ð
Þ
s
i
i
¼
1
2
e
t
=
s
i
:
X
3
þ
0
:
0667
20
1
e
T
=
s
i
þ
T
m
ni
s
i
s
i
e
T
=
s
i
ð
60
Þ
i
¼
1
Because stress is zero at zero strain, we may assume A
i
(0) = 0. Thus, using Eq.
(
50
), we may write:
Þ¼
De
X
n
A
i
nDe
ð
m
ni
:
ð
61
Þ
m
¼
1
This allowed Eq. (
60
) to be rewritten in terms of s
i
and m
ni
.
These parameters were calibrated so that the integral I given by Eq. (
48
) was
minimized. The fitted curves for the Generalized QLV model with pricewise linear
approximations of the A
i
functions (Fig.
8
) again produced an excellent fit to the
hold stress in all four tests (Fig.
9
); optimum time constants and slopes are listed in
Table
3
. The optimum time constants were very close to those found for the
Adaptive QLV model. Indeed, one may use a different fitting procedure (that
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