Biomedical Engineering Reference
In-Depth Information
Consider the case of an activator as in Eq. (
2.11
) and change the time variable to
τ
=
γ
P
t
, to obtain:
d
dτ
A
m
θ
A
+
γ
γ
P
=
κ
0
γ
P
+
κ
1
A
m
−
M,
γ
P
(2.14)
dP
dτ
=
κ
2
γ
P
M
−
P.
For a fixed value of
A
, Tikhonov's theorem can now be applied with
y
=
M
,
x
=
P
,
ε
=
γ
P
/γ
M
and with
f
(
x, y, ε
)=
κ
2
γ
P
A
m
θ
A
+
A
m
x
,
g
(
x, y, ε
)=
κ
0
γ
M
+
κ
1
y
.
Substituting the quasi steady state expression for mRNA into the protein Eq. (
2.14
),
and rewriting the system in the original time variable, obtains the reduced system:
y
−
−
γ
M
A
m
θ
A
+
A
m
−
P
=
κ
0
+
κ
1
γ
P
P,
(2.15)
where
κ
0
=
κ
2
κ
0
/γ
M
and
κ
1
=
κ
2
κ
1
/γ
M
. This yields a dynamical equation for
the protein concentration, directly dependent on the amount of activator (
A
). From
now on, all the intermediate steps (the binding of
A
to the promoter and synthesis
of mRNA) can be left out of the model.
The expression
h
+
(
x, θ, m
)=
x
m
/
(
θ
m
+
x
m
) (or
Hill function
) is known to
fit well to synthesis and activity rates. Similarly, the inhibition function can be
represented as:
h
−
(
x, θ, m
)=1
−
h
+
(
x, θ, m
)=
θ
m
/
(
θ
m
+
x
m
). For gene
regulatory networks, the exponent
m
is considered to be “large” (
m
≥
2), according
to experimental data [
40
]. Note that the qualitative form of
h
+
(
x, θ, m
) remains
essentially unchanged for
m
≥
2, with the same maximal and half-maximal values
(max(
h
−
)=1and
h
±
(
θ,θ,m
)=1
/
2), the only difference being the steepness
of the function around the value
θ
.Forlarge
m
, the parameter
θ
has therefore a
special meaning: it is a threshold value below which there is practically no activity
and above which activity is (almost) maximal. In the limit as
m
tends to infinity, the
Hill function becomes a step function, as described in Sect.
2.2.3.3
.
2.2.3.2
Continuous Differential Systems for Genetic Network Models
To illustrate the modeling and analysis of complex GRN, consider a regulatory motif
that appears frequently in genetic networks: two genes that mutually inhibit them-
selves or, more precisely, the protein
A
encoded by gene
a
represses transcription of
gene
b
, and vice-versa (Fig.
2.4
). The concentration of each protein can be described
by
x
j
=
κ
j
M
j
−
γ
j
x
j
, and each mRNA by an expression as in Eq. (
2.12
):
M
j
=
κ
j
0
+
κ
j
1
h
−
(
x
i
,θ
i
,m
i
)
−
γ
Mj
M
j
,
for
j, i
∈{
1
,
2
}
and
j
=
i.
(2.16)
Using the quasi-steady state assumption for the protein and mRNA equations,
the system can be reduced to the dynamics of the protein concentrations,
x
i
=
f
i
(
x
1
,x
2
) with (renaming constants):
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