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Page 12 of 15                   Sun et al. Complex Eng Syst 2022;2:17  I http://dx.doi.org/10.20517/ces.2022.48


































                                          Figure 2. The exponential stability in    of system (30).
                                                                    6
               and


                                                 11  5     1   4  3  1  2  55  4  1  2 2
                                    L  (  ,   ,   , 2) =     (−   +    −    +    ) +     (    )
                                                  2        3   3     3      4   4
                                                     15037  8  2563  8  671  6  209  6
                                                 ≤ −         +        −      +       .
                                                     2688     2688     252     252
               Then, we obtain

                                                      407  8  169  8  671  6  67  6
                                        L  (  ,   ,   ,   ) ≤ −     +     −     +     ,
                                                      112     112    252     56
                                                           407     169     671    67          8          8
               whichmeansthatthecondition(9)holdswith    1 = − 112 ,    2 =  112 ,    3 =  252 ,    4 = ,   (  ) = |  | ,    (  ) = |  | ,
                                                                                  56
               and    = 6. Let J   1 = J   2 = 1   (i.e., the active period of each subsystem is 1 s) and    01 =    02 = 0.1. From
               (11) and (12), we can compute that the constant    should satisfy 0.0953 <    < 0.7883. Then, it follows from
               (10) that    = 0.4414. According to Theorem 1, the highly nonlinear SSS (30) has a unique global solution on
               [− , ∞) and is bounded. In addition, the system (30) is not only 6th moment exponentially stable but also
                  3
                  4
               almost surely exponentially stable. Figure 2 shows that the system (30) is exponentially stable in 6th moment.
               Figure 3 shows that the system (30) is exponentially stable in the sample path. Figure 4 shows the switching
               signal   (  ).



               5. CONCLUSIONS
               Inthis paper, the existenceofa uniqueglobal solution for a highly nonlinear SSS with a deterministic switching
               signal is examined by using the ADT method coupled with the MLF approach. The stability criteria of   th
               moment exponential stability and almost surely exponential stability of the highly nonlinear SSS are stated.
               Finally, a numerical example is presented to illustrate the effectiveness of the obtained results. Inspired by
               recent studies [7,20,33–36] , two further research directions have emerged: (1) Solving the problem of stability for
               highly nonlinear SSSs with impulsive effects under asynchronous switching, and (2) designing a control input
               function to stabilize a highly nonlinear SSS with a time-varying delay.
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