Global entrainment of transcriptional systems to periodic inputs
- PMID: 20418962
- PMCID: PMC2855316
- DOI: 10.1371/journal.pcbi.1000739
Global entrainment of transcriptional systems to periodic inputs
Abstract
This paper addresses the problem of providing mathematical conditions that allow one to ensure that biological networks, such as transcriptional systems, can be globally entrained to external periodic inputs. Despite appearing obvious at first, this is by no means a generic property of nonlinear dynamical systems. Through the use of contraction theory, a powerful tool from dynamical systems theory, it is shown that certain systems driven by external periodic signals have the property that all their solutions converge to a fixed limit cycle. General results are proved, and the properties are verified in the specific cases of models of transcriptional systems as well as constructs of interest in synthetic biology. A self-contained exposition of all needed results is given in the paper.
Conflict of interest statement
The authors have declared that no competing interests exist.
Figures
-axis. The Figure shows the behavior of (9) for
(blue),
(green),
(red). Notice that an increase of
, causes an increase of the contraction rate, hence trajectories converge faster to the system unique periodic attractor. The other system parameters are set to:
, 
and gives as output the concentration of protein
. The downstream transcriptional module takes as input the concentration of protein
.
-axis. The state of the system (green),
, is entrained to both
and to a repeating
sequence. System parameters are set to:
,
= 1,
.
-axis. The system state (green),
, is entrained to the periodic input (blue):
. The zoom on
min highlights that trajectories starting from different initial conditions converge towards the attracting limit cycle. System parameters are set to:
,
,
,
,
.
-axis. Outputs
(top) and
(bottom) of two transcriptional modules driven by the external periodic input
. The parameters are set to:
,
,
,
for module
and
,
,
for module
.
-axis. Behavior of
when the input
is applied. Notice that when no forcing is present
converges to a non oscillatory regime behavior. System parameters are tuned in order to satisfy (72). Specifically:
,
,
,
,
,
,
.
-axis. Behavior of
when: (i) the input
is applied; (ii) no forcing is present. System parameters are the same as that used in Figure 10, except
.
-axis. Behavior of
when the input
is applied. Notice that when no forcing is present, the steady state behavior is non-oscillatory. System parameters are:
,
,
,
,
,
.
-axs. Notice that all the circuits synchronize with a steady-state evolution having the same period as
. System parameters are chosen as in Figure 11, with
.
,
,
,
,
. Green: inputs are
(left panel) and
(randomly picked, right panel). Blue:
. Note chaotic-like behavior in response to periodic input, but steady state in response to constant input.References
-
- Tyson JJ, Csikasz-Nagy A, Novak B. The dynamics of cell cycle regulation. Bioessays. 2002;24:1095–1109. - PubMed
-
- Kuznetsov YA. Elements of applied bifurcation theory. 2004. Springer-Verlag (New York)
-
- Sontag ED. An observation regarding systems which converge to steady states for all constant inputs, yet become chaotic with periodic inputs. 2009. Technical report, Dept. of Mathematics, Rutgers University. http://arxiv.org/abs/0906.2166.
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