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14   Adaptive Identification and Control of Uncertain Systems with Non-smooth Dynamics


                        Lorentzian model
                        In [9], an improved model has been reported by replacing exponential term,
                        such that:
                                                               1
                                        T f = f c sgn(˙x) + (f s − f c )  + f v ˙x   (1.9)
                                                           1 + (˙x/˙x s ) 2
                        which shows a systematic dependence of ˙x s.

                        Dahl model
                        The Dahl model was introduced in [10], which is given by
                                                                  α

                                                         T f
                                              ˙
                                             T f = σ 1 −   sgn(˙x)  ˙ x             (1.10)
                                                         f c
                        where σ is the stiffness coefficient and α is a parameter that determines the
                        shape of the stress-strain curve.

                        LuGre model
                        The LuGre model is a dynamic model which can capture the dynamic
                        behaviors of the contacting surfaces [3], where friction is related to the de-
                        flection of bristles. In this model, the rate-dependent friction phenomenon
                        and the Stribeck effect are all considered. The LuGre model is given by

                                                T f = σ 0z + σ 1 ˙z + σ 2 ˙x
                                                        |˙ x|                       (1.11)
                                                 ˙ z =˙x −  z
                                                        g(˙x)
                        where σ 0 is the stiffness of the bristles, σ 1 is the damping coefficient and
                        σ 2 is the viscous coefficient, respectively. z represents the average bristle
                        deflection, and g(˙x) can be selected to model different friction effects.
                        A reasonable selection of g(˙x) which can characterize the Stribeck effect
                        is set as
                                              g(˙x) = f c + (f s − f c )e −(˙x/˙x s ) 2  (1.12)


                        1.2.3 Continuously Differentiable Friction Model
                        The above conventional friction models (e.g., [3], [11], [12]and [13]) are
                        discontinuous or piecewise continuous, which may be problematic for de-
                        riving smooth control actions [6] when they are used in the control designs.
                        Moreover, the identification of such friction models with non-smooth dy-
                        namics is not a trivial task. In [6], a new continuously differentiable friction
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