Nonlinear Dynamics and Chaos, Strogatz: 2.1.5

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Homework Help Overview

The discussion revolves around a mechanical system described by the equation \(\dot{x} = \sin(x)\). Participants are tasked with identifying a suitable mechanical system and analyzing the stability of fixed points within that context.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • One participant suggests a pendulum as a potential mechanical system but expresses uncertainty about solidifying this choice. Another participant proposes the idea of an inverted pendulum in a viscous medium. Additional questions arise regarding the interpretation of potential energy in relation to the system's dynamics.

Discussion Status

Participants are exploring various interpretations of the problem, with some offering suggestions for diagrams and physical models. There is a focus on understanding stability through visual representation and physical intuition, though no consensus has been reached regarding the best approach.

Contextual Notes

There is mention of constraints such as the need for a mechanical system that aligns with the given equation and the implications of energy conservation in the analysis. The original poster has not returned to the discussion, leaving some questions open-ended.

Niteo
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Homework Statement


a) Find a mechanical system that is approximately governed by [itex]\dot{x}=sin(x)[/itex]
b) Using your physical intuition, explain why it now becomes obvious that x*=0 is an unstable fixed point and x*=[itex]\pi[/itex] is stable.

Homework Equations



[itex]\dot{x}=sin(x)[/itex] (?)

The Attempt at a Solution


I'm thinking a pendulum can be used as a mechanical system that varies with sinθ, but I'm not sure how to solidify my answer.

Could it possibly be an inverted pendulum in a very viscous medium?
 
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Consider a particle sliding over terrain y=f(x). Assuming conservation of energy (and some convenient total) what is the PE at x? What does that yield for f?
 
Question of understanding what they want. I think all you need to do is draw a diagram of the given function (familiar!) extending a little further on both sides than the points mentioned; xdot is the ordinate, but more important, with little horizontal arrows show which way x Is moving on each side of the named points, and you will soon see what they mean about stability/instability. Just explain this in your own words.
 
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Immerse your pendulum in honey and evolve your equations. When you finish, you're going to get a second order differencial equation. At this point, you got to be audacious and destroy the second order term. Voilà.
 
velkhaliliB said:
Immerse your pendulum in honey and evolve your equations. When you finish, you're going to get a second order differencial equation. At this point, you got to be audacious and destroy the second order term. Voilà.
The OP never came back, and this is years old.
But for what it's worth, I believe my suggestion in post #2 gives a very easy model, no approximations needed.
 

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