vault backup: 2024-09-23 14:12:51

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Dane Sabo 2024-09-23 14:12:51 -04:00
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@ -88,4 +88,13 @@ For $\bf J$:
- $\Delta = \pm\omega^2$
Then:
- $\theta$ is 0, $\Delta = \omega^2 >0$, spiral. Stable
- $\theta = n \pi$, $\Delta = - \omega^2 <0$, saddle. Unstable
- $\theta = n \pi$, $\Delta = - \omega^2 <0$, saddle. Unstable
---
# Competing Species Problems
We have a Species X vs. Species Y.
$$\dot x = x(\beta-\delta x -\gamma y) = \beta x - \delta x^2 - \gamma xy$$
$$\dot y = y(b - d y - c x) = by - dy^2 -cxy$$
>[!note] Coupling Terms
>$\gamma x y$ and $c x y$ are coupling terms.
>These equations are coupled because of these. Without them x and y would just be doing their own thing.