Page 435 - Mathematical Techniques of Fractional Order Systems
P. 435

420  Mathematical Techniques of Fractional Order Systems


              Phase synchronization: Happens when the phases of both systems are
               locked while the dependency of the amplitudes is weak.
              Lag synchronization: When outputs of both systems are identical except
               for a constant time shift.
              Antisynchronization: Is similar to complete synchronization except the
               amplitudes are additive inverses to each other (Srivastava et al., 2014).
              Projective synchronization: When both responses are the same except for
               a constant factor (Jiang et al., 2017; Ouannas et al., 2017i,h).
              Impulsive synchronization: When the coupling is forced to be on/off
               according to some condition.
              Incomplete synchronization: When the difference between the responses
               of the synchronized systems occasionally differs from zero.
              Complete desynchronization: It occurs when both systems differ in every
               detail.

               Another important form of synchronization is between two different sys-
            tems: different dimensions (Ouannas et al., 2017k,f) or even integer and frac-
            tional (Ouannas et al., 2017e). The following subsections discuss three
            examples of synchronization of FOCS.



            14.4.1 Synchronization of Fractional Order Modified
            Van der Pol-Duffing Circuit

            The system is given as (Matouk, 2011):
                                   α
                                            3
                                  D x 52 vðx 2 μx 2 yÞ;              ð14:30aÞ
                                      α
                                     D y 5 x 2 γy 2 z;              ð14:30bÞ
                                         α
                                        D z 5 βy;                    ð14:30cÞ
            where the original integer order system ðα 5 1Þ exhibits chaotic behavior at
            parameter values: β 5 200, μ 5 0:1, v 5 100 , and γ 5 1:6. The system has
            three equilibrium points: E 0 5 ð0; 0; 0Þ and E 1;2 5 ð 6 μ; 0; 6 μÞ. The equilib-
            rium point E 0 is a saddle point of index 1 while the other two equilibrium
            points E 1;2 are saddle points of index 2. If the eigenvalues at any equilibrium
            point are given (in general) by the polynomial:
                                           2
                                     3
                              PðλÞ 5 λ 1 a 1 λ 1 a 2 λ 1 a 3 5 0;    ð14:31Þ
            then, the discriminant is given as (Matouk, 2011):
                                               3
                                                               2
                                                       3
                                      2
                 DðPÞ 5 18a 1 a 2 a 3 1 ða 1 a 2 Þ 2 4a 3 ða 1 Þ 2 4ða 2 Þ 2 27ða 3 Þ :  ð14:32Þ
               Based  on the discriminant, the authors derived the fractional
            Routh Hurwitz conditions for stability then they proposed two schemes for
            synchronization of this system: unidirectional linear error feedback coupling
   430   431   432   433   434   435   436   437   438   439   440