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Chaotic Properties of Various Types of Hidden Attractors Chapter | 17  507


                The same algebraic manipulation can be applied to a system of three frac-
             tional order differential equations
                                        α
                                      D x 5 fðx; y; zÞ;
                                        β
                                      D y 5 gðx; y; zÞ;                ð17:7Þ
                                        γ
                                      D z 5 hðx; y; zÞ;
             where 0 , α; β; γ # 1, to obtain the corresponding solutions. Discretized
             solutions to the systems could be obtained using (17.5) and NSFD.
             Nonlinear terms including the same state variable that is being calculated are
             replaced with the aid of the nonlocal discrete representations. For example,
                             β
             in the equation of D y, the following rules are used for replacement:
                2
               y   y n y n11 ;  xy   2x n11 y n 2 x n11 y n11 ; and zy   2z n y n 2 z n y n11 : ð17:8Þ
                The relations used for solving the systems will be given in Section 17.5.

             17.3 SURVEY OF SOME SYSTEMS
             WITH HIDDEN ATTRACTORS
             Fig. 17.1 shows the categorization of the hidden attractors, which are
             included in the selected papers (Jafari et al., 2013, 2015; Pham et al., 2015,
             2014), from the viewpoints of type of equilibrium points and nonlinearity.
             The selected systems are reviewed in this section by placing each of them in
             the category to which it belongs with the aid of Tables 17.1 and 17.2.
                The history of hidden attractors dates back to the early works by J.C.
             Sprott (1994) about two decades ago, which uncovered some simple chaotic
             flows. The case of a system of differential equations with no equilibria that
             exhibits chaotic behavior was first reported in the system which he called
             case A, however, it was not analyzed in this sense. On the other hand, the
             classification of such chaotic flows into flows with no equilibria, a
             stable equilibrium point, or line equilibria is a more recent topic and their
             handling in this sense of classification or grouping started around 5 years
             ago (Wang and Chen, 2012). Hidden attractors allow unexpected and poten-
             tially disastrous responses to perturbations in a structure like a bridge or an


                                         Hidden attractors





                       Equilibrium points                  Nonlinearity




                 No       A line of  Single stable  Quadratic  Exponential  Hyperbolic
              equilibrium  equilibrium points  equilibrium
             FIGURE 17.1 Categories of the reviewed hidden attractors.
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