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+ | The biological networks are highly nonlinear and exhibit interesting phenotypical be- | ||
+ | havior for certain operating conditions. One of such behaviour is the limit cycle in the | ||
+ | mathematical sense, which shows a sustained oscillations of protein levels in the cell. It | ||
− | + | is quite interesting as well important to look for topologies which can produce such os- | |
+ | cillations for different amplitude, oscillation and shape. Here, we have used a theoretical | ||
− | + | framework to begind with for identifying topology based on following theorem. | |
+ | Theorem:1 Consider a system ̇x = f(x), which is of ring in nature, and f is a monotone | ||
+ | function and in the form | ||
− | + | Then, if the Jacobian of f and x has no repeated eigenvalues and has any eigenvalue | |
+ | with positive real parts, then the system must have a consistent periodic orbit. | ||
+ | To design a squarewave oscillator, we used the theorem to idenify the biological system | ||
+ | which can satisfies such condition. One of classical example is Repressillator (Elowitz et | ||
+ | all) or 5n1 ring oscillator (Murray et al). This kind of oscillator is based on negative | ||
+ | feedback with delay and able to produce stable limit cycle in computation and as well as | ||
+ | experimentally. However, these oscillators are more of a phaselag oscillator matching the | ||
+ | sinusoidal umbrella behavior. As the the philosophy behind our work is to design towards | ||
+ | square wave, we exploit the system parameters to produce relaxation oscillations. The | ||
+ | relaxation oscillator typically works on the principle to level of concentration, where once | ||
+ | the level is reached it relaxes there for some additional time and falls back to another | ||
+ | level and resides there for some till till it jumps back (slowly). The time evolution of such | ||
+ | trajectories portray a square wave-sih in state-space. | ||
+ | The dynamical model of the five node oscillator can be written as; | ||
− | + | where i ∈ [0 = 5, 1, 2, 3, 4, 5], xmi is the mRNA concentration level, xpi is the protein | |
− | + | transcription level, βm0 is the leaky expression, βmi is the production rate of mRNA, βpi | |
+ | is the production rate of protein, γmi is the degradation/dilution of mRNA and γpi is | ||
+ | the degradation/dilution of protein for ith protein. The simulation results of the model | ||
− | + | presented in Fig. . It is evident the such system can exhibit a oscillation resembling a | |
− | + | squarewave. | |
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− | + | As the dynamical model comprises of two time-scale, one can use the singular pertur- | |
− | + | bation analysis to reduce the model in to smaller one, i.e. 5th order, as discussed earlier. | |
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+ | The simpler version of the model, where multiple constants product are clubbed into one, | ||
+ | can be reproduced as follows, | ||
+ | where αi can be considered as the protein production rate constant and γ as the degra- | ||
+ | dation constant. The simulation of 5th order comes model presented in FigX is almost | ||
+ | identical to the simulation for full order model. Both of the model can exhibit sustained | ||
+ | square wave like response of arbitrary initial conditions. | ||
Revision as of 17:01, 1 November 2017
Deterministic Model