The Trapping Region of the Lorenz equations

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Discussion Overview

The discussion revolves around the trapping region of the Lorenz equations, specifically how this region is defined and identified using Lyapunov functions and alternative methods. Participants explore the implications of different approaches to determining the trapping region and the characteristics of radial velocity within this context.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions the method of defining a trapping region using radial velocity, noting that their results differ from expected outcomes based on the Lyapunov function approach.
  • Another participant suggests that within the trapping region, the radial velocity (dr/dt) can be greater than zero, as particles may loop around the attractor.
  • A follow-up response affirms that at the edge of the trapping region, the velocity should point inward, implying dr/dt should be less than or equal to zero.
  • Some participants propose that different Lyapunov functions yield different trapping regions, raising questions about the uniqueness of these functions.
  • There is a challenge regarding the assumption that a minimal trapping region must be the same across different methods, with a participant arguing that different Lyapunov functions could define strictly smaller regions.
  • One participant expresses a belief that there is typically one Lyapunov function for a system, comparing it to a unique energy function in conservative systems, but acknowledges the possibility of multiple Lyapunov functions.
  • There is a suggestion that converting to polar coordinates should yield a minimal region, though this is not universally accepted.

Areas of Agreement / Disagreement

Participants express differing views on the uniqueness of Lyapunov functions and the implications of using different methods to define trapping regions. The discussion remains unresolved regarding the relationship between radial velocity and the characteristics of trapping regions.

Contextual Notes

Participants highlight limitations in their understanding of Lyapunov functions and the assumptions underlying their methods. The discussion reflects uncertainty about the implications of different approaches to defining trapping regions.

Oliver321
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I was dealing with nonlinear systems of differential equations like the Lorenz equations (https://en.wikipedia.org/wiki/Lorenz_system). Now there is a trapping region of this system defined by the ellipsoid ρx^2+σy^2+σ(z-2ρ)^2<R.
I wondered how this region is found and I found out that a Lyapunov function is used.
However, I tried to do it another way. I defined r=√(x^2+y^2+z^2). Now I thought: when d/dt r <0 the radial velocity points inward and so there is a trapping region. I calculated this but the result was completely different.
Why doesn’t it work with my way?

Thanks for every awnser!
 
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In the trapping region, isn't dr/dt often bigger than zero? The particles move around and make loops around the attractor, but dr/dt isn't constantly shrinking while doing this.
 
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Office_Shredder said:
In the trapping region, isn't dr/dt often bigger than zero? The particles move around and make loops around the attractor, but dr/dt isn't constantly shrinking while doing this.

Yes that’s right, but on the edge of the trapping region all arrows should point inward (or at least be tangential to the boundary), so dr/dt should be less or equal to zero?
 
If you use different Liapunov functions, you will get different trapping regions.
 
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pasmith said:
If you use different Liapunov functions, you will get different trapping regions.
But why? With both methods I can get a minimal region, which is a trapping region. Because it is minimal, it has to be the same?
 
Oliver321 said:
But why? With both methods I can get a minimal region, which is a trapping region. Because it is minimal, it has to be the same?

How do you know the region is minimal?

All you can conlcude from looking at a particular Liapunov function is that the attractor is in some region, because once trajextories enter it they cannot leave. But there's always the possibility that a different Liapunov function would give you a stirctly smaller region, and hence a closer bound on the attractor.
 
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pasmith said:
How do you know the region is minimal?

All you can conlcude from looking at a particular Liapunov function is that the attractor is in some region, because once trajextories enter it they cannot leave. But there's always the possibility that a different Liapunov function would give you a stirctly smaller region, and hence a closer bound on the attractor.

Thanks for the answer!
So I thought that there is only one Liapunov function for a system. Like if i have a conservative system I can use a energy function to do the same things (and the Energy function is unique?). A liapunov function is a generalised energy function (at least so I was told). But if there are a few, this would be plausible.
Nevertheless the method with converting to polar coordinates should give a minimal region?
 

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