Page 25 - Adaptive Identification and Control of Uncertain Systems with Nonsmooth Dynamics
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16   Adaptive Identification and Control of Uncertain Systems with Non-smooth Dynamics


                        h 1 (v) is introduced to represent the reversal behavior while h 2 (v) depicts
                        the Stribeck effect, which are defined as


                                                       2f s ,  ˙ x ≥ 0
                                             h 1 (˙x) =                             (1.15)
                                                       0,     ˙ x < 0

                        and

                                                  h 2 (˙x) = e −(˙x/˙x c ) 2        (1.16)

                        where ˙x c is the critical velocity at which the friction torque is minimum.
                           The above friction model (1.14) is developed based on the fact that
                        any arbitrary continuous piecewise linear function can be effectively rep-
                        resented by using a discontinuous piecewise parametric representation
                        (DPPR) as shown in [14]. However, different to standard DPPR, the static
                        friction has a jumping behavior at zero velocity where the direction of mo-
                        tion changes. Moreover, in the low velocity regime, the Stribeck effect and
                        the Coulomb friction force mainly contribute to the friction, which makes
                        the friction highly non-linear and non-smoothing in low-speed especially
                        near zero crossings. In order to address the Stribeck effect and the jumping
                        behavior at zero velocity, two additional terms are introduced in DPPR:
                        1) A jump term h 1 (˙x) related to the maximum static force, which is used to
                        represent the reversal behavior of friction force when the motion direction
                        is changed; 2) An exponential component h 2 (˙x) to denote the Stribeck
                        effect. As for an example, Fig. 1.2 provides theprofileofDPPR friction
                        model.




                        1.3 CONCLUSION
                        This chapter describes different friction dynamics and several friction mod-
                        els, which will be used in the control designs to be presented in this book.
                        Classical models are developed to show the dominant friction components,
                        among which LuGre model is able to represent most dynamic behaviors
                        of friction. Moreover, a continuously differentiable friction model is re-
                        cently proposed to facilitate continuous control designs. The introduced
                        discontinuous piecewise parametric representation (DPPR) friction model
                        is particularly suitable for model parameter identification.
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