Biomedical Engineering Reference
In-Depth Information
The type 1 cell proliferation rate is constant, while the type 2 cell proliferation
rate decreases with their local density number. As a consequence the nonnegative
function h
d
( .,
s
)
C b (R
)
,for s
S
, may be modelled in the following way:
h (
)) = λ 1 δ C i
1
Z i
X i
C i
h
(
(
t
)) =
(
t
) ,
(
t
+ λ 2
δ C i
,
(25)
(
t
) ,
1
(
t
) ,
2
Q [ 2 ]
N
+
(
)(
X i
(
))
1
N
K
t
where
λ 1 λ 2 and K is just a regularizing kernel.
The counting process N
λ 1 , λ 2 R + , with
d
(
t
)= Φ ([
0
,
t
] × R
× S)
has intensity given by
N
)
i = 1 h ( Z i
(
t
d
ν (
)= Λ
(R
× S)
=
(
))
d t
d t
t
d t
t
Cell State Evolution. The change of state of each cell is described via a continuous
time Markov chain. The associated time-dependent stochastic matrix for the i -th cell
is given by the following:
(
m 12 +
m 13 )
m 12
m 13
Z i
,
M
(
(
t
) ,
t
)=
m 21 (
m 21 +
m 23 )
m 23 ,
(26)
0
0
0
where
C i
C i
prob
{
(
t
+ Δ
t
)=
k
|
(
t
)=
h
}
Z i
m hk :
=
m hk (
(
t
)) =
lim
Δ
Δ
t
t
0
are given by
)= λ 12
u
λ 13
m 12 (
x
,
1
) ,
m 13 (
x
,
1
)=
,
(27)
(
,
Q [ 1 ]
N
x
t
(
K
)(
x
)
Q [ 2 N
m 21 (
x
,
2
)= λ 21 (
K
)(
x
) ,
m 23 (
x
,
2
)= λ 23 ,
(28)
for i
,
j
=
1
,
2
,
3,
λ ij >
0.
Evolution of the Fields. VEGF diffuses and naturally degrades; furthermore, as a
matter of modelling simplification, we assume that VEGF is produced at the front
of type 2 cells [ 19 ]. So, given a region of interest E
d
R
=
(for d
2 or 3), for
d , the concentration of VEGF g
(
,
) R + × R
(
,
)
any
t
x
x
t
is subject to the following
evolution equation:
j = 1 ε ( ·, C j ( t )) ( x , 2 ) K N ( X j
N ( t )
g
(
x
,
t
)
)+ α g 1
N
=
d g g
(
x
,
t
)+
D g Δ
g
(
x
,
t
(
t
)) .
(29)
t
 
Search WWH ::




Custom Search