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Equilibrium existence

$\displaystyle \forall j, \left(x_{j} - \alpha \right) \left( 1+\Sigma_{i=1}^{n}x_{i}^\mathrm{c} \right)=\sigma x_{j}^{c}
$

If $ \forall j, x_{j} = \bar{x}$,

$\displaystyle n \bar{x}^{c+1} - \left( \sigma + n \alpha \right) \bar{x}^c +\bar{x}-\alpha=0$ (8)

There is at least one solution, maybe 3 (or 2 in degenerate cases) depending on the parameters. The solutions are noted $ \bar{x}_l$, $ \bar{x}_u$, and $ \bar{x}_h$, with $ \bar{x}_l<\bar{x}_i<\bar{x}_h$.

If $ f(x)=n x^{c+1} - \left( \sigma + n \alpha \right) x^c +x$, $ f'(x)=(c+1) n x^c - c (\sigma + n \alpha)x^{c-1} +1$, $ f''(x)=c(c+1)nx^{c-1} - c(c-1)(\sigma+n\alpha)x^{c-2}$. $ f''\left(\frac{c-1} {n(c+1)} \left(\sigma + n\alpha\right)\right)=0$. $ f'$ takes negative values iff $ f'\left(\frac{c-1} {n(c+1)} \left(\sigma + n\alpha\right)\right)<0$, which is a necessary condition for the existence of 3 equilibria with all variables on.

The dynamics of the system constrained to $ \forall i, x_i=x$ are defined by

$\displaystyle \dot{x}=-x + \frac{\sigma x^c}{1+nx^c} + \alpha
$

The sign of $ \dot{x}(t)$ is the opposite of that of $ f(x(t))$. Because $ \bar{x}_u$ is such that $ f'(\bar{x}_i)<0$, it is easy to see that the steady state $ \bar{x}_u$ is unstable for the constrained system, and thus for the full system.