I Does the Hamilton-Jacobi equation exist for chaotic systems?

AI Thread Summary
The discussion centers on the applicability of the Hamilton-Jacobi equations to chaotic systems, questioning whether a canonical transformation exists that maintains constants of motion. It is noted that such transformations can exist locally outside equilibrium, but the sets where they are defined are not invariant, complicating the analysis of chaotic dynamics. The concept of dynamical chaos is highlighted as encompassing various effects, including ergodicity and separatrix splitting, which complicate trajectory behavior. Additionally, the presence of attractors in dissipative systems can lead to complex trajectory patterns that reflect the attractor's geometry. The conversation suggests that traditional analytical mechanics literature may not adequately address these complexities, particularly in the context of perturbation theory.
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TL;DR Summary
Does the Hamilton-Jacobi equation exist for chaotic systems?
Given a Hamiltonian ##H(\mathbf{q},\mathbf{p})##, in the time-independent Hamilton-Jacobi approach we look for a canonical transformation ##(\mathbf{q},\mathbf{p})\rightarrow(\mathbf{Q},\mathbf{P})## such that the new Hamiltonian is one of the new momenta $$H(\mathbf{q},\mathbf{p})=K(\mathbf{Q},\mathbf{P})=P_{1}=E.$$
If such transformation exists, all the momenta ##\mathbf{P}## are constant of the motion. And, since the transformation is canonical, we will have n constant of the motion in involution, i.e., ##\left\{ P_{i},P_{j}\right\} =0.## But this seems to be the requirement of the Liouville theorem for integrability. Chaotic systems don't have that many constants of motion in involution.
This seems to imply that the Hamilton-Jacobi equations cannot be even written for chaotic systems, so my reasoning has to be wrong somewhere. Where?
 
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andresB said:
TL;DR Summary: Does the Hamilton-Jacobi equation exist for chaotic systems?

Given a Hamiltonian H(q,p), in the time-independent Hamilton-Jacobi approach we look for a canonical transformation (q,p)→(Q,P) such that the new Hamiltonian is one of the new momenta H(q,p)=K(Q,P)=P1=E.
If such transformation exists, all the momenta P are constant o
Such a transformation exists locally outside an equilibrium. The set where this transformation is defined is not invariant. The system comes and goes away from there, while a dynamical chaos appears in invariant sets.
 
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wrobel said:
Such a transformation exists locally outside an equilibrium. The set where this transformation is defined is not invariant. The system comes and goes away from there, while a dynamical chaos appears in invariant sets.

Ok, I suspected the issue had to do with the new momenta not being defined globally.

Yet, I'm not sure I understand your answer. Can you give more details or point to a source with an example?
 
A dynamical chaos is an informal concept which expresses a complex of very different effects. The common feature for all these effects is a complicated behavior of trajectories of a dynamical system. Every time, one should specify what he means by saying “dynamical chaos”. For example, in Hamiltonian systems, ergodicity or separatrix splitting are commonly considered as a dynamical chaos, but there are a lot of other chaotic effects. Real life examples are really hard.
See for example this https://link.springer.com/book/10.1007/978-3-642-03028-4
or start from this https://www.mat.univie.ac.at/~gerald/ftp/book-ode/ode.pdf

UPD

Dissipative systems commonly have attractors. If an attractor is of complicated geometry, say has a fractional dimension, then trajectories which wind up on the attractor replicate its geometry and become complicated. That is another chaotic effect.
 
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Likes andresB and vanhees71
Fascinating and frustrating at the same time.

wrobel said:

My doubts started by studyng perturbation theory. In the book Canonical Perturbation Theories Degenerate Systems and Resonance, I find the following
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The usual books in analytical mechanics don't deal with this.
 
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