Biomedical Engineering Reference
In-Depth Information
1
G1 sim
SG2M sim
G1 data
SG2M data
0.9
0.8
0.7
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0.5
0.4
0.3
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0.1
0
0
5
10
15
20
25
30
time (h)
Fig. 2
M
( green or light grey ) from biological data ( dashed line ) and from numerical simulations ( solid line ).
Our model results in a reasonably good fit to biological data
Time evolution of the percentages of cells in the phases G 1 ( red or deep grey )and S
/
G 2 /
the random variable corresponding to the time spent in G 1 and S
M .This
enabled us to determine the expression of the transitions rate according to the
formula ( 22 ). We then compared the solutions of the system with cell recordings
that had previously been synchronised “by hand”, i.e., all recordings were artificially
made to start simultaneously at the beginning of G 1 phase. The result is shown on
Fig. 2 . Note that using an inverse problem method—see Sect. 5 —instead of ours
could have consisted here in determining the parameters of the model, i.e., K i i + 1
transition functions, by minimising an L 2 distance between this experimental data
curve and a theoretical, parameter-dependent curve representing these data.
/
G 2 /
7.5
Optimising Eigenvalues as Objective and Constraint
Functions
We then used combined time-independent data on phase transition functions,
obtained from experimental identification of the parameter functions K i i + 1 (
t
,
x
)=
κ i (
x
)
in the uncontrolled model, with cosine-like functions representing the periodic
 
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