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
A m
θ A +
γ γ P
= κ 0
γ P + κ 1
A m
M,
γ P
(2.14)
dP
= 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 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 M and κ 1 = κ 2 κ 1 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 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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