Path: utzoo!utgpu!news-server.csri.toronto.edu!rpi!zaphod.mps.ohio-state.edu!samsung!noose.ecn.purdue.edu!news.cs.indiana.edu!ariel.unm.edu!cie.uoregon.edu!scavo From: scavo@cie.uoregon.edu (Tom Scavo) Newsgroups: comp.theory.dynamic-sys Subject: Re: Can Chaos Be Predictable? Keywords: chaos, predictability Message-ID: <1991Jun22.195653.26004@ariel.unm.edu> Date: 22 Jun 91 19:56:53 GMT References: <1991Jun20.203628.14343@alchemy.chem.utoronto.ca> <1991Jun21.003436.28578@cunews.carleton.ca> <1991Jun21.064503.8325@netcom.COM> Distribution: comp.theory.dynamic-sys Organization: Campus Information Exchange, University of Oregon Lines: 53 [Sorry if this is a repeat, but I have reason to believe it didn't get through the first time.] In article <1991Jun21.064503.8325@netcom.COM> kmc@netcom.COM (Kevin McCarty) writes: [much of an excellent article deleted] >So tell us, what happens to precision when you increment t by 1? You >*double* the argument value of the sine. In order to get an answer >with one bit of accuracy (e.g., whether the result is closer to 1.0 >than 0.0) you need one additional bit of input precision per unit time >step. Another way to look at it is that the absolute output error >roughly *doubles* with each passing unit of time. In this respect >it is no different from f(x) = 2x mod 1. Points initially close >together diverge exponentially over time. In fact, D(x) = 2x mod 1 is (semi-)conjugate to F(x) = 4x(1-x) via the two-to-one map S(x) = [sin(pi x)]^2 . I believe this is where the closed form solution to F^n(x) (where F^n is the nth iterate of F ) comes from since D^n(x) = 2^n x mod 1 . ... >Compare this with your other example, f(x) = sqrt(x) (on the unit >interval [0,1] say). Note that you need hardly any precision at all >in the initial condition in order to predict to a pretty good precision >the result of iterating f(x) a number of times. In fact, sqrt(x) has >an attracting fixed point for almost all initial values. The fixed point x = 1 attracts the orbits of ALL points in the function's domain of definition. ... >Consider three different dynamical laws described by >f(x) = sin**2( 2x ) >g(x) = (x + a) mod 1, (0 < a < 1) >h(x) = x/2 >Analyze the precision to which the n'th iterate is known, as a function >of the precision in the initial value of x and the number of iterates. >Only f(x) has chaotic behavior. Can you prove this? Can you find a conjugacy from f to some other map (like D , F , Q(x) = x^2 - 2 , or the tent map) that is known to be chaotic? The map g has quite interesting (but atypical) dynamics which I've yet to completely analyze, and of course h has the origin as a globally attracting fixed point. -- Tom Scavo scavo@cie.uoregon.edu