vault backup: 2024-10-28 15:30:42

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Dane Sabo 2024-10-28 15:30:42 -04:00
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@ -22,5 +22,22 @@ $$\text{dist}[x, c] = \min_{y \in C}|x-y|$$
Where c is a curve.
Where in the plane we're using the minimum of the 2 norm.
## Summary
Stable half-paths can be generally stable, approaching an equilibrium, or periodic.
Unstable half-paths exceed the bound $\epsilon$ somewhere.
Unstable half-paths exceed the bound $\epsilon$ somewhere.
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.....
# Lyapunov Stability
Basically extend the 2D distance formula we talked about last time to include n dimensions. (May need to analyze complex solutions as well).
Let's define Lyapunov Stability:
>[!note] Lyapunov Stability Definition
>Let $x^*$ be a real or complex solution of $x = X(x,t)$. Then,
>1. $x^*$ is lyapunov stable iff for each value of $\epsilon>0$ however small there is a corresponding value of $\delta>0$ such that
>![[Pasted image 20241028152704.png]]
>2. If the system is autonomous, then we can disregard the idea of $t_0$ in 1.
>3. Otherwise, we call the system unstable in the sense of Lyapunov.
This stability definition defines that for an autonomous system, Lyapunov stability is sufficient for Poincare stability.

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