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I have the following system of ODEs that I am trying to find the equilibrium points to. I firstly begin by taking (2) and rearranging for $x$. I then insert this into (3) to find a relation for $z$. Then my strategy is to insert the newly found expressions for $x$ and $z$ into $(1)$ to generate an expression for $y$. However when I do this, everything cancels and I cannot generate my expression for $y$.

Where am I going wrong?

\begin{align} (1) \qquad \frac{dx}{dt} &= -\beta x(y + z) + \gamma y + \alpha z + \epsilon\eta '(1-\phi)y \\ (2) \qquad \frac{dy}{dt} &= \beta yx - \gamma y - \eta \epsilon y \\ (3) \qquad \frac{dz}{dt} &= \beta zx - \alpha z + \epsilon\eta \phi y \end{align}

The expression for $x$ is:

$$ x^* = \frac{1}{\beta}(\gamma + \eta\epsilon) $$

The expression for $z^*$ is:

$$ z = - \frac{\epsilon \eta\phi}{\gamma + \eta\epsilon - \alpha } y $$

Inserting these into (1) cancels everything out and I cannot obtain an independent expression for $y^*$! I am struggling to complete further analysis without this crucial step!

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  • $\begingroup$ Everything cancels in all three equations regardless of the value of $y^*$? In that case you have a whole line of equilibria, which is not that unusual of a situation. $\endgroup$
    – Ian
    Commented Oct 2, 2017 at 0:35
  • $\begingroup$ Yes there are many non-isolated equilibria in this system. I see another with $(x^*,0,0)$. $\endgroup$
    – Gregory
    Commented Oct 2, 2017 at 0:37
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    $\begingroup$ Noticed that $y = 0$ was a solution of the (2) equation and that $y$ and $z$ always appear in terms. $\endgroup$
    – Gregory
    Commented Oct 2, 2017 at 1:02
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    $\begingroup$ You are missing two critical points and I agree with the third you found. The two missing CPs are $$x = \dfrac{\alpha}{\beta}, y = 0, ~\mbox{and}~ y = 0, z = 0$$ $\endgroup$
    – Moo
    Commented Oct 2, 2017 at 1:08
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    $\begingroup$ When I show two values for the CP, it means the third can be anything, so yes, for example, the second CP I show is $$(x, y, z) = (x, 0, 0)$$ Substitute those two values into each of the 3-equations. Clear? $\endgroup$
    – Moo
    Commented Oct 2, 2017 at 1:22

1 Answer 1

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Equation $(2)$ gives $$ y^* = 0\, , \qquad\text{or}\qquad x^* = \frac{\gamma+\eta\epsilon}{\beta} $$ at equilibrium. Injecting these two possibilities in equation $(3)$ yields either $$ z^* = 0 \quad\text{or}\quad x^* = \frac{\alpha}{\beta}\, , \qquad\text{or}\qquad z^* = \frac{\epsilon\eta\phi\, y^*}{\alpha-\gamma-\eta\epsilon} . $$ Now, we use $(1)$ at equilibrium:

  • the case $y^* = 0 = z^*$ gives $x^* \in \mathbb{R}$. There is an equilibrium line;
  • the case $y^* = 0$, $x^* = {\alpha}/{\beta}$ gives $z^* \in \mathbb{R}$. There is a second equilibrium line;
  • the case $x^* = ({\gamma+\eta\epsilon})/{\beta}$, $z^* = {\epsilon\eta\phi\, y^*}/({\alpha-\gamma-\eta\epsilon})$ gives $y^*=0=z^*$.

The last equilibrium point is conditioned by $\alpha \neq \gamma + \eta\epsilon$, which was already assumed when writing $z^* = {\epsilon\eta\phi\, y^*}/({\alpha-\gamma-\eta\epsilon})$. This equilibrium point belongs to the first equilibrium line, and is therefore not isolated.

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  • $\begingroup$ Thank you!, in the third case doesn't $y^*=0$ then mean that $z^*=0$ too? $\endgroup$ Commented Oct 2, 2017 at 11:12
  • $\begingroup$ @AngusTheMan Yes, that's it! $\endgroup$
    – EditPiAf
    Commented Oct 2, 2017 at 11:53

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