Page 599 - Mathematical Techniques of Fractional Order Systems
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Control and Synchronization Chapter | 19  569


             1996. It is basically an extended version of the famous Lorenz system. Further
             investigations and analysis were made in Zhou et al. (1997). The integer order
             Lorenz Stenflo system can be described by following expressions.
                                  _ xðtÞ 5 ayðtÞ 2 axðtÞ 1 dwðtÞ
                                  _ yðtÞ 5 cxðtÞ 2 yðtÞ 2 xðtÞzðtÞ
                                                                      ð19:15Þ
                                  _ zðtÞ 5 xðtÞyðtÞ 2 bzðtÞ
                                  _ wðtÞ 52 xðtÞ 2 awðtÞ
             where x, y, z, and w are the system states and a, b, c, and d are the system
             parameters. The hyperchaotic behavior of the above system is shown in
             Fig. 19.1. The system parameters are taken as a 5 1, b 5 0:5, c 5 26, and
             d 5 1:5. The simulation has been carried out for 200 seconds for the initial
             conditions x 0ðÞ; y 0ðÞ; z 0ðÞ; wð0ÞÞ 5 ð2 0:592; 0:04; 0:72; 0:5Þ.
                      ð
                The dynamic analysis of fractional order version of the hyperchaotic
             Lorenz Stenflo system was first discussed in Wang et al. (2014). System
             dynamics of fractional order Lorenz Stenflo system are as follows:

                                  q 1
                                D t xðtÞ 5 ayðtÞ 2 axðtÞ 1 dwðtÞ
                                  q 2
                                D t yðtÞ 5 cxðtÞ 2 yðtÞ 2 xðtÞzðtÞ
                                                                      ð19:16Þ
                                  q 3
                                D t zðtÞ 5 xðtÞyðtÞ 2 bzðtÞ
                                  ðq 4 Þ
                                D t wðtÞ 52 xðtÞ 2 awðtÞ
             where q 1 ; q 2 ; q 3 , and q 4 are the orders of the fractional derivatives. The
             hyperchaotic behavior of the above system is depicted in Fig. 19.2 for the
             system parameters as a 5 1, b 5 0:5, c 5 26, and d 5 1:5. The order of deri-
             vatives is taken as q 1 5 q 2 5 q 3 5 q 4 5 0:98 and the simulation time is 200
             seconds. The initial conditions are chosen as ð x 0ðÞ; y 0ðÞ; z 0ðÞ; wð0ÞÞ 5
             ð1; 0:2; 0:2; 2 0:2Þ.

             19.4 CONTROL AND SYNCHRONIZATION VIA
             BACKSTEPPING TECHNIQUE
             As the dynamics of the fractional order Lorenz Stenflo system given in
             (19.16), are not in strict-feedback form, a simple transformation has to be
             carried out. For, w 5 x 1 , x 5 x 2 , y 5 x 3 , z 5 x 4 and q 1 5 q 2 5 q 3 5 q 4 5 q, the
             system is transformed to:
                                   q
                                  D t x 1 52 x 2 2 ax 1
                                   q
                                  D t x 2 5 ax 3 2 ax 2 1 dx 1
                                   q                                  ð19:17Þ
                                  D t x 3 5 cx 2 2 x 2 x 4 2 x 3 1 u
                                   q
                                  D t x 4 5 x 2 x 3 2 bx 4
                where, u is the controller to be designed. As the above system is in the
             desired form, two different strategies can be applied for control and synchro-
             nization. In this section, the backstepping strategy is presented and in the
             next section active backstepping technique will be described.
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