vault backup: 2024-10-28 15:30:42
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@ -22,5 +22,22 @@ $$\text{dist}[x, c] = \min_{y \in C}|x-y|$$
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Where c is a curve.
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Where in the plane we're using the minimum of the 2 norm.
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## Summary
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Stable half-paths can be generally stable, approaching an equilibrium, or periodic.
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Unstable half-paths exceed the bound $\epsilon$ somewhere.
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Unstable half-paths exceed the bound $\epsilon$ somewhere.
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Poincare cannot handle the time dependency of systems. As a result, we can't really use Poincare to handle real systems. That leads us to.....
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# Lyapunov Stability
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Basically extend the 2D distance formula we talked about last time to include n dimensions. (May need to analyze complex solutions as well).
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Let's define Lyapunov Stability:
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>[!note] Lyapunov Stability Definition
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>Let $x^*$ be a real or complex solution of $x = X(x,t)$. Then,
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>1. $x^*$ is lyapunov stable iff for each value of $\epsilon>0$ however small there is a corresponding value of $\delta>0$ such that
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>![[Pasted image 20241028152704.png]]
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>2. If the system is autonomous, then we can disregard the idea of $t_0$ in 1.
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>3. Otherwise, we call the system unstable in the sense of Lyapunov.
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This stability definition defines that for an autonomous system, Lyapunov stability is sufficient for Poincare stability.
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