Xref: utzoo sci.math:16046 comp.theory.dynamic-sys:208 Path: utzoo!utgpu!news-server.csri.toronto.edu!rpi!zaphod.mps.ohio-state.edu!pacific.mps.ohio-state.edu!linac!att!news.cs.indiana.edu!ariel.unm.edu!cie!scavo From: scavo@cie.uoregon.edu (Tom Scavo) Newsgroups: sci.math,comp.theory.dynamic-sys Subject: Re: Non-linear difference equation Summary: this is a quadratic equation Keywords: discrete dynamical systems, iterative mappings, chaos Message-ID: <1991Mar25.215710.10367@ariel.unm.edu> Date: 25 Mar 91 21:57:10 GMT References: <1991Mar25.183530.23916@athena.mit.edu> Reply-To: scavo@cie.uoregon.edu (Tom Scavo) Followup-To: sci.math Organization: University of Oregon Campus Information Exchange Lines: 32 In article <1991Mar25.183530.23916@athena.mit.edu> armann@athena.mit.edu (Armann Ingolfsson) writes: >I'm trying to find out something about the behavior of the sequence {x(t)} >determined by > >x(t) + a x(t-1) + b x(t-1)^2 = c, for t = 1,2,... > >with x(0) given. Any pointers about under what conditions the sequence >converges, what it converges to, and at what rate would be useful to me. Unless I'm misinterpreting your notation, this is just a quadratic equation. Since quadratics are conjugate to one another, it suffices to consider Q(x) = x^2 + c which in some sense is the "simplest" of all quadratics. Note the dependence on the *single* parameter c . For an elementary discussion of the dynamics of this map and its complex analogue, see Devaney, R.L. _Chaos, Fractals, and Dynamics_. Addison- Wesley, Menlo Park, CA, 1990. Another much studied quadratic is the logistic equation given by F(x) = r x (1-x) . Everything you ever wanted to know about this dynamical system will be found in Devaney, R.L. _An Introduction to Chaotic Dynamical Systems_ (second edition). Addison-Wesley, Redwood City, CA, 1989. For certain parameter values, these simple equations have very complicated dynamics including period-doubling and chaotic behavior. Tom Scavo scavo@cie.uoregon.edu