Page 252 - Adaptive Identification and Control of Uncertain Systems with Nonsmooth Dynamics
P. 252

Hysteresis Dynamics and Modeling  253



















                            Figure 16.4 Backlash-like model of hysteresis.


                                                                  _
                            where γ α,β [u(t),ζ]∈ C([0,T]),ζ ∈[−1,1], t = lim ε→0 t − ε. Similar to the
                            Preisach model, the KP model can be described as:


                                        y(t) =     μ(α,β)γ α,β [u,ζ(α,β)](t)dαdβ       (16.7)
                                                 P 0
                            16.2.4 Backlash-Like Model

                            Different from the previously discussed models, the backlash model does
                            not belong to the Preisach type model. The Backlash-like hysteresis model
                            is simpler than Preisach models in terms of its expression, where the ex-
                            plicit solution can be obtained [11]. Backlash exists in a wide range of
                            physical systems and devices, such as biological optics, electro-magnetism,
                            actuators, electronic relay circuits, and others. Many scholars are interested
                            in the identification and control of systems with Backlash-like hysteresis,
                            e.g., [12]. As shown in Fig. 16.4 and explained in [12], the Backlash-like
                            hysteresis model can be described by using the following continuous-time
                            dynamic model:

                                            ˙ u(t) = α|˙v(t)|(cv(t) − u(t)) + b˙v(t)   (16.8)

                            where α, c, b are constants satisfying c > b > 0.
                               Then the explicit solution of (16.8) can be easily obtained as [12]:

                                                  u(t) = cv(t) + h[v(t)]               (16.9)

                            where h[(v(t))]=[u 0 − cv 0 ]e −α(v(t)−v 0 )sgn(˙v)  + e −αsgn(˙v)     v(t) [b − c]e αδsgn(˙v) dδ for
                                                                         v 0
                            constant u 0 = u(v 0 ).
   247   248   249   250   251   252   253   254   255   256   257