Biomedical Engineering Reference
In-Depth Information
the Adaptive QLV model in a single, large amplitude ramp-and-hold test. In the
incremental ramp-and-hold test, the variation of the relaxation function with tissue
length can be modeled. This precludes the use the exceptionally simple fitting
procedure from the single, large amplitude ramp-and-hold protocol (Eq. (
40
)) to
determine the k
i
functions at intermediate stains ((n-1)De \ e \ nDe).
3.4.2 Generalized Fung Model
Substituting the strain function from Eq. (
41
) into Eq. (
9
), stress history for the nth
relaxation test is:
8
<
r
o
ð
n
1
Þ
De
þ
D
T
t
R
ds
¼
r
Pn
ð
t
Þ;
þ
D
T
P
i
t
Þ
A
i
ð
n
1
Þ
De
þ
D
T
s
g
i
t
s
ð
0\t\T
0
r
n
ðÞ¼
:
r
o
nDe
ð
Þ
þ
D
T
P
i
R
ds
¼
r
Hn
ð
t
Þ;
T
Þ
A
i
ð
n
1
Þ
De
þ
D
T
s
g
i
t
s
ð
t [ T
0
ð
49
Þ
The nonlinear unknown functions A
i
(e) appear inside the convolution integral in
both the ramp-loading stress history r
Pn
(t) and the hold-relaxation stress history
r
Hn
(t). Therefore, both r
Pn
(t) and r
Pn
(t) depend on the functions A
i
(e) for all the
strains between (n-1) De and nDe. This complicates the optimization procedure as
in the case of the Fung model for the single large amplitude ramp-and-hold pro-
tocol. Similarly, the optimization protocol is based on several trial-and-error steps.
However, because in the incremental ramp-and-hold protocol the incremental
strain De is small, we may approximate the A
i
(e) functions as piecewise linear. For
the case of a stress-free, fully relaxed specimen at zero strain, we may assume all
A
i
(0) to be zero. In the nth ramp-and-hold test, A
i
may be written as a linear
function in terms of a single parameter, a slope m
ni
, as:
¼
A
i
ð
n
1
Þ
De
ð
n
1
Þ
De
þ
De
T
Þ þ
m
ni
De
T
A
i
t
ð
t
;
ð
50
Þ
where A
i
((n-1) De) was determined in the (n-1)th ramp-and-hold test. For known
shape functions, the parameters m
ni
may be determined from data in the nth ramp-
and-hold test by minimizing the integral I
n
given in Eq. (
47
). For parametric shape
functions, the parameters of the shape functions and all the m
ni
parameters may be
calibrated so that the integral I given by Eq. (
48
) is minimized.
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