Team:Duke/Modeling/3

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Contents

Mathematical Modeling of Bistable Toggle Switch

Kinetic Model of Bistable System

Following Gardner's Work...

Tim Gardner from Jim Collins' Lab of Boston Univeristy published one of the first major papers on genetic toggle switch. In his work, he used a kinetic approach to model the stability of a genetic toggle switch. His equations involved two equations expressing the change in the level of two mutually repressive repressors with respect to time.

Gardner model.png
Figure 1. Equation Used in Gardner's Model


Gardner variables.png
Figure 2. Variables Used in Gardner's Model



Using this model, Gardner produced the two graphs shown below. The first is a graph of nullclines. Nullcline, also called zero-growth isocline, is a line that represents the set of points at which the rate of change is zero. In this example, the two nullclines shown are where rate of change of repressor 1 (U) and repressor 2 (V) are zero. It is clear that at the intersection of these two nullclines are steady-state points of the system because these are points where the change of both repressor levels with respect to time is zero.

The difference between the two figures with nullclines on left and right is that the system on the left is bistable with the system on the right is mono-stable. Figure (a) shows that there are two stable steady-states where only one of the two repressors exists at a high level, inhibiting the production of the other repressor. There exists a third intersection in the middle, however, this point can be mathematically shown to be unstable using the eigenvalue of the Jacobian matrix involving U and V (workings not included here). The value of U and V doesnt change exactly at this unstable steady-state, however, the level of repressors will quickly diverge from this point even at the smallest perturbation. The figure on the right, figure (b), shows that at a different combination of parameters, a system can be mono-stable where the nullclines only intersect once at a stable steady-state solution.


Gardner trajectory.png
Figure 3. Nullclines for Gardner's Model



Another set of graphs from Gardner's work is shown below. The two plots are bifurcation diagrams of a system, again, with two mutually repressive genes. Bifurcation is a mathematical term that describes a phenomena "when a small smooth change made to the parameter values (the bifurcation parameters) of a system causes a sudden 'qualitative' or topological change in its behavior" (Blanchard). In terms of this system in question, bifurcation occurs when the system changes its stability (Change between monostability and bistability).

The graphs below shows the effect of change in cooperativity on the bifurcation region. On the two axes are rate of synthesis of the two repressors, which can be translated as the strengths of the two promoters. According to the graphs, the bifurcation increases as cooperativity increases. In other words, increasing cooperativity of mutual repression allows a set of two weaker promoters to have bistability.



Gardner bifurcation.png
Figure 4. Gardner's Bifurcation Region Plots



explain the effect of changing hill coeff on bifurcation region. explain nullcline

reproduce nullcline and trajectory (explain trajectory)

Kinetic nullcine.png
Figure 5. Bifurcation Region and Trajectory


Development of Our Kinetic Model

moving on, we have developed another kinetic model using the results of the thermodynamic model. gardner = effect of hill coeff on bistability of a system (bifurcation region) new model = effect of various parameters on bistability (highlight and number Kd, pr_Str, basal rate.

as mentioned before, key assumption is is (du/dt , dv/dt = proportional to p_bound)

show equation

Thermo rates.png
Figure 6. Our Kinetic Model


explain

show values for variables like degradation rate

Results from Our Kinetic Model

show graph

Thermo prstrength.png
Figure 7. Bifurcation Region with Different Promoter Strengths


Thermo binding.png
Figure 8. Bifurcation Region with Different Repressor Binding Strengths


Thermo leaky.png
Figure 9. Bifurcation Region with Different Basal Transcription Rate


explain



show nullcline

Thermo nullcline.png
Figure 10. Nullcines and Trajectories Using Our Model



confirm bistability of the system (thermodynamic model incorporated into kinetic model)

References

  1. Gardener, T. et al. Construction of a genetic toggle switch in Escherichia coli. Nature. 403, 339-342 (2000).
  2. Blanchard, P.; Devaney, R. L.; Hall, G. R. (2006). Differential Equations. London: Thompson. pp. 96–111.