Poincaré Section and Return Map for Rössler System
Consider the Rössler system (cf. Strogatz, ch. 12.3)
dxdt
=
-y-z,
(1)
dydt
=
x+ay,
(2)
dzdt
=
b+z(x-c).
(3)
Write a Matlab program to solve (1,2,3)
numerically (using simply forward Euler).
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.
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.
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?
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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