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