For the critical valueI3.71 it appears as a phase transition of
the type “first-order” through a supercritical Andronov-Hopf
bifurcation as described in [24, 52], giving rise to a limit cycle,
periodic oscillations, and self-organizing system outside the ther-
modynamic equilibrium. It is further noted as the maximum con-
centration values of the population of proliferating tumor cells
increase significantly.
It is noteworthy, as can be seen in Fig.4, as far as it decreases
the value of the control parameterI, although the system exhibits8
7
6
5
mmol/ml^4mmol/ml mmol/mlmmol/mlmmol/ml mmol/ml3
2
1
0712108
642
06 5 4 3 2 1 0108642010864201281064
20050
CABD100
s150 2000
E F50 100
s150 200 0 50 100
s150 2000 50 100
s
150 2000 50 100
s
0 50 100 150 200
s
150 200Fig. 4Dynamical behavior of the proposed model (Eq.24) for different values of the control parameter
I(N¼5,H¼3): (a) stationary state (I¼4), (b) limit cycle (I¼3), (c) limit cycle (I¼2), (d) limit cycle
(I¼1), (e) limit cycle (I¼0.7), (f) chaos (I¼0.4);red(x),blue(y) andgreen(z). Reprinted from [83]
140 Sheyla Montero et al.