Biomedical Engineering Reference
In-Depth Information
where t is the time at which N R is calculated and N 0 represents the number
of BMUs that are required to resorb the naturally timeworn osteocytes
and those that have been destroyed by microdamage. As proposed [2], the
resorption of osteocytes is activated by the microdamage. So the BMU acti-
vation frequency, f a (BMUs/volume/time), is assumed to be a function of the
existing state of damage
k
Φ
f
=
f
(1
e
)
(5.13)
R
a
a
(max)
where f a (max) = 0.8 BMU/mm 3 /day [2], and k R = −1.6 defines the shape of the
curve. Φ is defined here as an environmental stimulus:
q
(
)
e
(5.14)
Φ= ε+ +
CR CE
GB
f
ij
ij
L
i
i
i
i
Here, C ij , C i , and G i are the damage rate coefficients. ε ij , E i , and H i are strains,
electrical field, and magnetic field, respectively. The value for the exponent
q is set at a nominal 2/3. The mechanical loading rate, R L , is assumed to be
3,000 cpd, and f e is the frequency of the electromagnetic field.
The population N F in Equation (5.2) is found by multiplying the quantities
of resorbed osteocyte by k F :
N F = k F N R
(5.15)
where k F is the correlation coefficient of the refilling BMUs, indicating the
relation between the refilling and the resorbing process. k F is defined as a
piecewise function of Φ and p [2]:
c
Φ≤Φ≤Φ
0
L
U
(5.16)
k
=
c
Φ<Φ
F
1
U
n
p
p
(
)
cc
+ Φ<Φ
c
0
2
2
L
0
Considering that the quantity of growth factors retained in osteo-
cytes changes along with the environmental loads, as mentioned before,
Φ L and Φ U can be considered as MESr and MESm, respectively. When
Φ L  ≤  Φ  ≤  Φ U , the growth factors remain unchanged ( k F = c 0 ) and the bone
tissue is in the remodeling state. When Φ  <  Φ U , more growth factors
( k F = c 1 > c 0 ) are generated, which results in bone modeling. When Φ L  <  Φ
fewer growth factors ( k F = ( c 1 > c 0 )( p / p 0 ) n + c 2 < c 0 ) result in a disuse mode of
bone tissue.
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