(Under Construction : synchronisation and whole system)

Oscillations

Short System

• We wanted to see if, from a mathematical point of view, it was possible for the "short" system presented above to hover.

• Here are the equations we took into account :

• The equations are normalized (thus the degradation term set to 1), as well as the parameters :

• As introduced before, the goal of this model was to give us useful bases on which to work on. Then, we shall use the values of the parameters presented below as a "starting point". We shall present a double approach, composed of a theoretical and a simulation approach. Both approaches should interact so as to help us understand the way our system behaves.
• The obvious though process we propose consists in observing what happens with the simulation, then understand the source of these phenomenas. Finally, the ultimate goal consists in finding how we can pull the strings, hidden in the system, that control the behavior of the system.

Observations

---> petites oscillations + vérifier par le calcul ---> trop grande réactivité de flhDC

• First of all, let us see what the simulation gives, and what pieces of information we can get from it.
• Observation#1 :
  • By looking at this simulation, we could think that it is going to be hard to get oscillations...
    
  • However when we zoom, we get this more reassuring view :
    
  • Conclusion : some intrinsic oscillations actually occur, but they seem to be strongly attenuated. The mathematical study shall help us decide whether these are only artefact oscillations. For example we shall try to check if the period observed (~10 time units) can be linked to mathematical data.
• Observation#2 :
  • Here, we need to change parameters a little bit, so that it becomes more obvious//trop grande rapidité du system... voir atténuation mais eventuellemnt a dégager

Understanding the dynamics

• Theory introduction

The classical approach consists in finding the equilibrium state, by setting

Then, we evaluate the jacobian matrix, so as to put the system under its linearized form:

which gives :

Then, we want to find the eigenvalues of the jacobian matrix, because they make us understand the behavior of the system. Here is the theoretical explanation :

The λ and γ coefficients make the convergence. In our case they are negative terms, which explains the fact that we have a quick convergence for the system. Ideally, it could be convenient to find which parameter influence this coefficient, so as to play with it and be able to propose a better control of the convergence.
The μ coefficient is responsible for the oscillations. In fact, in another base, with only real matrix, this would beget cosinuses and sinuses terms. Furthermore, it is strongly linked to the period of the oscillations.

• Comparison of the simulation and theoretical periods

We obtained three solutions :

We are only interested in positive real solutions. We can note that 0.4764 corresponds well to the experimental equilibrium value. Then we evaluated the eigenvalues for the jacobian :

We can note that the λ and γ coefficient are negative, which corroborates the fact that we obtain a convergence.

• Understanding the attenuation

Furthermore, this theoretical study helps us understand that reducing the attenuation is tough. In fact, whatever the base in which you consider a matrix, the trace is conserved. Here, we obtain :

Since λ and γ are assumed (thanks to simulations) to be negative, we cannot avoid to have their sum to be (with absolute value) superior to 2. The only chance we have would be that the weight goes in the λ parameter because this parameter plays a role in the third dimension, in which we are not interested. However, for every simulation we made, we found the opposite. Trying to evaluate with non-numerical calculus does not provide relevant material.

However, we now know that β_FliA influences the attenuation. We ran a simulation with β_FliA=0.02

This confirms what we saw previously. Before, the system was hovering around the equilibrium at T=20. In this second case, the system is therefore less attenuated, and we have to wait until T=150 to observe the effect.

Last but not least, one should not forget that we chose a normalized interpretation of the system. Thus, even though the attenuation phenomenon remains unchanged, the tiny oscillations we see may indeed be observable.

Using these elements to improve the system and give directions to the wet-lab

• To what extent can this study help us improve our oscillations? We want to minimize the γ coefficient, and we know that the period is linked to the μ coefficient.

• Qualitative exploitation

First and foremost, the effect of β_FliA as a considerable influence over the

• Quantitative exploitation

• What can we do about that, ans how can we improve the behavior of the system? The ideal though process would be to get the equilibrium state, but not with numerical values, so as to understand the influence of each of the system parameter. However, we face a major problem. This requires ot solve an (n+1) degree equation, which explicit solutions are unusable. Yet, imagining that we can get the solution, we could evaluate the eigenvalues in the same way (since they are solution of a third degree equation, this could be possible). Consequently, we could understand the influence of each parameter, and we could find a way to minimize the λ and γ coefficients.
• However, we understand that even though we consider the short system, this process faces strong difficulties. Yet, it is possible to consider an algorithmic approach that meets the same ends. Let's say we want to otpimize the system for n and θ_FlhDC :
  • for n evolving between n_min and n_max
  • for θ_FlhDC evolving between θ_FlhDCmin and θ_FlhDCmax

Entire System

//biocham ici//+ comparaison avec le modele hillistique

FIFO

• The goal here is to present the results of the simulations we made concerning the FIFO part of the system.

Here is the system we implementated using Matlab (see the corresponding codes)

and the corresponding equations (for more detailed information see our establishment of the model).

where CFP, YFP, and RFP will be denoted below as respectively Z1,Z2 and Z3.

• We wanted to see if our predictions were accurate or not. We then solved the equations, forcing the behavior of FhlDC. In a first step, we imposed a constant production term of 1. Then, at a certain time, we set this production term to zero :

In fact we assumed that this behavior for FlhDC was acceptable regarding its estimated behavior in the whole system.

• We saw previously that without FliA, the FIFO would presumably not work. We then simulated a first system, where [FliA] stays to zero value.
  

We may see that there is a LIFO behavior rather than the FIFO we expect...

• Then, we simulated the entire system, to check if we had
  • the lasting burst due to FliA (more important for Z3 than for Z2, and more important for Z2 than Z1) in the increasing phase.
  • the effect of fliA which maintained the concentrations to their maximum (more important for Z3 than for Z2, and more important for Z2 than Z1) in the decreasing phase.
    

• We observe on these plots that the behavior is quite the one we expected, and that the FIFO is realized. FliA enables the curves to cross, and adds a delay on the genes that are most affected, with gives a better observability of the FIFO behavior.

Synchronization

Mathematical Analysis

Simulations and verification of the hypothesis