ESAM 438

Interdisciplinary Nonlinear Dynamics
Fall 2000
Hermann Riecke

Problem Set 8


For Discussion Section November 29


  1. Poincaré Section and Return Map for Rössler System

    Consider the Rössler system (cf. Strogatz, ch. 12.3)
    dx
    dt
    =
    -y-z,
    (1)
    dy
    dt
    =
    x+ay,
    (2)
    dz
    dt
    =
    b+z(x-c).
    (3)
    Write a Matlab program to solve (1,2,3) numerically (using simply forward Euler).

    1. Pick a = 0.2 and b = 0.2. Scan c through the range 5 < c < 7.5 and plot the projection of the attractor on the (x,y)-plane. To get a reasonable impression of the attractor you have to run at least to t = 500 for each value of the parameters.
    2. Obtain the Poincaré section (surface of section) of the attractor in the (y,z)-plane for increasing values of x, i.e. plot the points (yn,zn) at which the attractor pierces the (y,z)-plane with increasing x. Thus, whenever x changes sign (with x increasing) determine y and z by linear interpolation for the time at which x = 0. Plot this discrete sequence of yn and zn as a function of n.
    3. Since the points on the Poincaré section obtained in * lie on a line which can be characterized by taking only the yn-values (or the zn-values), obtain the return map yn+1 = f(yn) by plotting the points (yn,yn+1). The return map is similar in spirit to the Lorenz map for the maxima discussed in class. Plot the function f for increasing values of c (with a = b = 0.2). This sequence of maps should give you an idea of what the dynamics of the Rössler system is in this regime. How does it compare to that of the logistic map?

  2. Universality of Unimodal Maps

    From Strogatz do problems 10.6.1 and 10.6.2 (note the introductory paragraph on p. 394).


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On 19 Nov 2000, 18:49.