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- Newsgroups: sci.fractals
- Path: sparky!uunet!utcsri!helios.physics.utoronto.ca!alchemy.chem.utoronto.ca!mroussel
- From: mroussel@alchemy.chem.utoronto.ca (Marc Roussel)
- Subject: Re: phase space
- Message-ID: <1992Dec15.040911.21587@alchemy.chem.utoronto.ca>
- Organization: Department of Chemistry, University of Toronto
- References: <FARID.92Dec14141233@gradient.cis.upenn.edu>
- Date: Tue, 15 Dec 1992 04:09:11 GMT
- Lines: 41
-
- In article <FARID.92Dec14141233@gradient.cis.upenn.edu>
- farid@gradient.cis.upenn.edu (Hany Farid) writes:
- >Excuse the ignorance but in James Gleick's book title "Chaos" on page
- >50 he shows signals in a 'traditional time space' and in a 'phase
- >space'. Can anyone explain in lay terms how to translate a signal
- >from time space to phase space, and perhaps what exactly phase space
- >is.
-
- The idea of a phase space is contained in most elementary books on
- differential equations. Let's take a simple example. Suppose you have
- a pair of autonomous differential equations
-
- dx
- -- = f(x,y)
- dt
-
- dy
- -- = g(x,y)
- dt
-
- Because of the existence and uniqueness theorem for systems of
- autonomous differential equations, there is one and only one solution
- curve (trajectory) of this system passing through every point (x0,y0) of
- the xy phase plane. There are different ways to think about this
- result, but the upshot is that you can simply disregard time and think
- of this system as defining trajectories in the phase plane rather than
- solutions in an (x,y,t) space. You can convince yourself that the
- trajectories satisfy the equation
-
- dy g(x,y)
- -- = ------
- dx f(x,y)
-
- so that time can be formally eliminated from the equations themselves.
-
- Marc R. Roussel
- mroussel@alchemy.chem.utoronto.ca
-
-
- P.S., to Hany: There is no such newsgroup as sci.chaos so I'm posting
- this to sci.fractals.
-