The Selkov model for glycolysis exhibits a Hopf bifurcation. As the b parameter increases from 0.25 to 0.95, the model switches from a stable equilibrium point to a limit cycle near b=0.41 and back to a stable equilibrium point near b=0.8.
Figure 1: The phase plane plots showing oscillatory behavior.
Description
This is a model showing oscillatory behavior in a chemical reaction with just two species.
PHASE PLANE PLOTS
Nullclines are plotted in dashed red (dx/dt=0) and dashed green (dy/dt=0).
Stable solutions are plotted in magenta (b=0.35, b=0.85)
Limit Cycles are plotted in blue (b=0.45, b=0.55, b=0.65).
Plow lower right corner: The standard deviation of the last half of the solutions were calculated for X and Y and the product, LC, was plotted as a function of b. Where LC is small, the solution has a stable steady state (Magenta circles). Where LC gets large, the solution is a limit cycle (Blue circles).
The appearance and disappearance of a periodic orbit through a local change in the stability properties of a steady point is known as a Hopf bifurcation. The Hopf bifurcations occur at approximately b=0.41 and b= 0.80 when a=0.1;
TIME COURSE PLOTS
There are 6 plots corresponding to 6 values of b. x is plotted in black, y in red.
Note that far away from the transition points the solutions converge rapidly (R=0.35, transition at 0.41). Close to the transition points the solutions converge more slowly (r=0.81, transition at 0.80). As the solution switches from stable solutions to Limit Cycles back to stable solutions, the size of the Limit cycles begins small, grows to a maximum and then shrinks back to zero. (r=0.42, r=0.55, r=0.65, and r=0.79).
Equations
Selkov model equations
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Selkov, E., Model of glycolytic oscillations, (1968) Eur. J. Biochem. 4, 79-86. Strogatz, SH, Nonlinear Dynamics and Chaos, Addison-Wesley, Reading, MA, (1994). (see pages 205-207)
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