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b. Does the value of this limit change if the value of y(1) is modified,
                                   while r is kept fixed?
                             Pb. 2.22 Find the iterates of the logistic equation for the following values of
                             r: 3.1, 3.236068, 3.3, 3.498561699, 3.566667, and 3.569946, assuming the follow-
                             ing three initial conditions:

                                               y(1) = 0.2, y(1) = 0.5, y(1) = 0.7

                             In particular, specify for each case:
                                a. The period of the orbit for large N, and the values of each of the
                                   iterates.
                                b. Whether the orbit is super-stable (i.e., the periodicity is present for
                                   all values of N).



                              This section provided a quick glimpse of two types of nonlinear difference
                             equations, one of which may not necessarily converge to one value. We dis-
                             covered that a great number of classes of solutions may exist for different
                             values of the equation’s parameters. In Section 2.8 we generalize to 2-D. Sec-
                             tion 2.8 illustrates nonlinear difference equations in 2-D geometry. The study
                             of these equations has led in the last few decades to various mathematical
                             discoveries in the branches of mathematics called Symbolic Dynamical the-
                             ory, Fractal Geometry, and Chaos theory, which have far-reaching implica-
                             tions in many fields of engineering. The interested student/reader is
                             encouraged to consult the References section of this book for a deeper
                             understanding of this subject.






                             2.8  Fractals and Computer Art
                             In Section 2.4, we introduced a fractal type having a priori well-defined and
                             apparent spatial symmetries, namely, the Koch curve. In Section 2.7, we dis-
                             covered that a certain type of 1-D nonlinear difference equation may lead, for
                             a certain range of parameters, to a sequence that may have different orbits.
                             Section 2.8.1 explores examples of 2-D fractals, generated by coupled differ-
                             ence equations, whose solution morphology can also be quite distinct due
                             solely to a minor change in one of the parameters of the difference equations.
                             Section 2.8.2 illustrates another possible feature observed in some types of
                             fractals. We show how the 2-D orbit representing the solution of a particular
                             nonlinear difference equation can also be substantially changed through a
                             minor variation in the initial conditions of the equation.



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