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Poincaré Map 📂Dynamics

Poincaré Map

Definition 1

Let us consider a vector field in Euclidean space $\mathbb{R}^{n}$ and open sets $U \subset \mathbb{R}^{n}$ defined in the function continuous $f : U \to \mathbb{R}^{n}$ as given by the following differential equation. $$ \dot{x} = f(x) $$ Represent the flow as $\phi_t \left( \cdot \right)$ and consider a $\left( n-1 \right)$-dimensional surface $\Sigma$ that intersects the vector field. For an open set $V \subset \Sigma$, we define the following map $P$ as the Poincaré map. $$ \begin{align*} P : V &\to \Sigma \\ x &\mapsto \phi_{\tau (x)} (x) \end{align*} $$ Here, $\tau (x)$ denotes the time it takes to return to $\Sigma$ after departing from $x$.


  • If at every point on $\Sigma$, $f(x) \cdot n (x) \ne 0$ holds, then we call $\Sigma$ the transverse surface to the vector field.

Explanation

book

Due to $P$, the flow $\phi$ on $\Sigma$ can be represented by wandering on $\Sigma$, skipping the intermediate steps.

denma

This is similar to the long-range attack prevention plane constraint in Denma2. The Poincaré map reduces the system represented by a vector field to $\Sigma$ by one dimension. Although much information is lost due to the dimension reduction, it is useful to apply in any problem focusing on the overall dynamics.

See Also


  1. Wiggins. (2003). Introduction to Applied Nonlinear Dynamical Systems and Chaos Second Edition(2nd Edition): p123. ↩︎

  2. https://comic.naver.com/webtoon/detail.nhn?titleId=119874&no=119 ↩︎