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. 2010 Apr 15;6(4):e1000739.
doi: 10.1371/journal.pcbi.1000739.

Global entrainment of transcriptional systems to periodic inputs

Affiliations

Global entrainment of transcriptional systems to periodic inputs

Giovanni Russo et al. PLoS Comput Biol. .

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.

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Conflict of interest statement

The authors have declared that no competing interests exist.

Figures

Figure 1
Figure 1. Entrainment of (9) to .
Time (minutes) on the formula image-axis. The Figure shows the behavior of (9) for formula image (blue), formula image (green), formula image (red). Notice that an increase of formula image, causes an increase of the contraction rate, hence trajectories converge faster to the system unique periodic attractor. The other system parameters are set to: formula image, formula image
Figure 2
Figure 2. A schematic diagram of the transcriptional system modeled in (12).
As explained in , the transcriptional component takes as input the concentration of protein formula image and gives as output the concentration of protein formula image. The downstream transcriptional module takes as input the concentration of protein formula image.
Figure 3
Figure 3. Entrainment of the transcriptional module (12).
Time in minutes on the formula image-axis. The state of the system (green), formula image, is entrained to both formula image and to a repeating formula image sequence. System parameters are set to: formula image, formula image = 1, formula image.
Figure 4
Figure 4. Entrainment of the transcriptional module (26).
Time in minutes on the formula image-axis. The system state (green), formula image, is entrained to the periodic input (blue): formula image. The zoom on formula image min highlights that trajectories starting from different initial conditions converge towards the attracting limit cycle. System parameters are set to: formula image, formula image, formula image, formula image, formula image.
Figure 5
Figure 5. Multiple driven transcriptional modules.
A schematic diagram of the transcriptional modules given in (12).
Figure 6
Figure 6. Entrainment of two-driven transcriptional modules.
Time in minutes on the formula image-axis. Outputs formula image (top) and formula image (bottom) of two transcriptional modules driven by the external periodic input formula image. The parameters are set to: formula image, formula image, formula image, formula image for module formula image and formula image, formula image, formula image for module formula image.
Figure 7
Figure 7. Transcriptional cascade discussed in the text.
Each box contains the transcriptional module described by (12).
Figure 8
Figure 8. The Repressilator circuit.
A schematic representation of the three-genes Repressilator circuit.
Figure 9
Figure 9. Modular addition to the Repressilator circuit.
This module is used for forcing the original circuit with some external signal (represented by an extra-cellular molecule in the bottom panel).
Figure 10
Figure 10. Simulation of the Repressilator model described by (53), (54), (55).
Time (minutes) on the formula image-axis. Behavior of formula image when the input formula image is applied. Notice that when no forcing is present formula image converges to a non oscillatory regime behavior. System parameters are tuned in order to satisfy (72). Specifically: formula image, formula image, formula image, formula image, formula image, formula image, formula image.
Figure 11
Figure 11. Increasing the amplitude of oscillations for the model described by (53), (54), (55).
Time (minutes) on the formula image-axis. Behavior of formula image when: (i) the input formula image is applied; (ii) no forcing is present. System parameters are the same as that used in Figure 10, except formula image.
Figure 12
Figure 12. Simulation of the Repressilator forced by some extra-cellular molecule.
Time (minutes) on the formula image-axis. Behavior of formula image when the input formula image is applied. Notice that when no forcing is present, the steady state behavior is non-oscillatory. System parameters are: formula image, formula image, formula image, formula image, formula image, formula image.
Figure 13
Figure 13. Synchronization of Repressilators.
Behavior of a population of Repressilator modeled as in (80). Time (minutes) on formula image-axs. Notice that all the circuits synchronize with a steady-state evolution having the same period as formula image. System parameters are chosen as in Figure 11, with formula image.
Figure 14
Figure 14. Simulation of counter-example.
The following randomly-chosen input and initial conditions are used: formula image, formula image formula image, formula image, formula image, formula image. Green: inputs are formula image (left panel) and formula image (randomly picked, right panel). Blue: formula image. Note chaotic-like behavior in response to periodic input, but steady state in response to constant input.

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