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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