next up previous
Next: Steady-state analysis: variables on Up: Analysis of the bHLH Previous: Analysis of the bHLH

Dynamical analysis

0 is a stable steady state. If $ x_i(0)=0$, then $ \forall t>0, x_i(t)=0$. If $ x_i(0)>0$, then $ \forall t>0, x_i(t)>0$. One can thus suppose that $ \forall i,\forall t\ge 0, x_i(t)>0$. Consider a state in which there is one variable strictly superior to all others (ie, a state not belonging to the line $ x_1=x_2=..=x_n$). Suppose without loss of generality that the variable in question is $ x_1$. Consider the function

$\displaystyle f_{1}(x)=\frac{x_1^2}{\alpha D^2 + x_1^2}
$

$\displaystyle \dot{f_{1}(x)}=2\alpha D x_1\frac{\dot{x_1}\left( D-x_1 \right) - x_1 \Sigma_{i=2}^n \dot{x_i}}{\left( \alpha D^2 + x_1^2 \right)^2}
$

$\displaystyle \frac{\left( \alpha D^2 + x_1^2 \right)^2}{2\alpha D x_1}\dot{f_{1}(x)}=\dot{x_1} +$    
$\displaystyle \sigma \Sigma_{i=2}^n \frac{x_1 x_i \left( x_1 - x_i \right)\left...
...i \right)} {\left(\alpha D^2 + x_1^2 \right) \left( \alpha D^2 + x_i^2 \right)}$    

For $ \alpha \ge 1/2$, the second term is positive.

We have

$\displaystyle \frac{\mathrm{d}x_1(t)}{\mathrm{d}t}= \sigma f_{1}(x) - x_1
$

We first consider the case in which $ \forall t\ge 0,\forall n\ge j>1, x_1>x_j$.

Suppose that $ \sigma f_{1}(0) \ge x(0)$. In this case, $ \dot{f_1}\left( 0 \right) > 0$, and $ x_1$ and $ f$ are strictly increasing functions of time. If $ \sigma f_{1}(0)<x_1(0)$, then $ \dot{f_1}\left( 0 \right)$ can be negative or positive. In the first case, $ x_1$ is decreasing as long as $ f_1$ is. If at some time $ t_0$ $ \sigma f_{1}(t_0) \ge x(t_0)$, then for $ t>t_0$, $ x_1$ and $ f_1$ are increasing functions of time. Thus there can be at most one change in the monotony of $ x_1$. Thus $ \lim_{t\rightarrow \infty} x_1(t)$ exists. Since $ \ddot{x_1}$ exists and is bounded on any trajectory, $ \lim_{t\rightarrow \infty} \dot{x_1}(t)=0$. All trajectories thus converge to a steady state where $ \forall j>1, x_j=x_1 \mathrm{or} x_j=0$.

If $ \exists t \mathrm{st} \forall  n>j>1, x_1(t)=x_j(t)$, the system is brought back to one dimension. Note that it is impossible for any variable to outgrow $ x_1$.


next up previous
Next: Steady-state analysis: variables on Up: Analysis of the bHLH Previous: Analysis of the bHLH