Page 269 - Mathematical Techniques of Fractional Order Systems
P. 269

258  Mathematical Techniques of Fractional Order Systems


               For the considered second order (n 5 2) plant, (9.34) becomes,
                                        s 5 λe 1 _ e                  ð9:35Þ
               Here, λ is a constant and error e 5 θ r 2 θ, where θ r is the desired angular
            position and θ is the current angular position of end points of the links in
            radian. On differentiation (9.35) becomes,

                                       _ s 5 λ_ e 1 € e               ð9:36Þ
                         €
               Putting € e 5 θ r 2 θ €
                                             €   €
                                     _ s 5 λ_ e 1 ðθ r 2 θÞ           ð9:37Þ
               The system output is forced to track this surface with the help of a reach-
            ing law. The reaching law is to be designed in such a way that it guarantees
            the stability of the closed loop system. Generally, three reaching laws are
            widely used and have been reported in the literature namely exponential,
            constant rate, and power rate laws (Liu and Wang, 2012). In the present
            work, exponential law as given in (9.38) is utilized. According to this law,
                               _ s 52 E sgn sðÞ 2 ks; E . 0; k . 0    ð9:38Þ

            where E and k are constants.
               As SMC is a high gain switching controller, a fast oscillation phenomenon,
            called chattering, occurs at the controller output due to the discontinuity in
            sgn function in control action. To resolve this problem, normally saturation
            function (9.39) is employed rather than sgn function (Liu and Wang, 2012).
                                        8   11; s . Δ
                                        >   s
                                        <    ; jsj , Δ
                                  sat sðÞ 5  Δ                        ð9:39Þ
                                        >
                                           21; s ,2 Δ
                                        :
            where Δ 0 , Δ , 1Þ forms the boundary layer.
                   ð
               Now, from (9.38) and (9.39),
                               _ s 52 E sat sðÞ 2 ks; E . 0; k . 0    ð9:40Þ
               Equating (9.38) and (9.40),
                                                   €   €
                               2 E sat sðÞ 2 ks 5 λ_ e 1 ðθ r 2 θÞ    ð9:41Þ
                             €
               Now substituting θ from the dynamics of manipulator (9.30),in (9.41) then,
                                     €        21         _
                                         ½
                  2 E sat sðÞ 2 ks 5 λ_ e 1 ðθ r 2 M θðފ  τ 2 V θ;θ 2 G θðÞ Þ  ð9:42Þ
               This can also be expressed as,
                              _                                €
                                             h                  i
                                        ½
                      τ 5 V θ;θ 1 G θðÞ 1 M θðފ E satðsÞ 1 ks 1 λ_ e 1 θ r  ð9:43Þ
   264   265   266   267   268   269   270   271   272   273   274