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Zhang et al. Intell Robot 2022;2(4):371­90  I http://dx.doi.org/10.20517/ir.2022.26  Page 375






















                                               Figure 2. 2-DOF vehicle lateral dynamics.

               is the steering angle for the front wheel of the vehicle.   ,    and       represent the sideslip angle, yaw rate, and
               longitudinal velocity of the ego vehicle, respectively. The vehicle lateral dynamics can be described in terms of
               the sideslip angle and yaw rate as follows:

                                            {
                                                  ¤
                                                   2   (  ) =          (  ) +         (  ) −      2   (  )
                                                                                                       (6)
                                                    ¤  (  ) =                (  ) −               (  ) +       (  )
               where       is the external yaw moment generated by the differences in the longitudinal tire/road forces among
               the four tires of the vehicle.


               2.3. Tire/road force model
               The vehicle lateral tire/road force is generated by contact between the vehicle tires and the road surface [30] .
               A tire operates in the linear region for a small vehicle lateral acceleration, which can be characterized by the
               cornering stiffness of the front and rear tires       and      , respectively, and the corresponding sideslip angles.
               The relationship between the tire lateral force and sideslip angle is

                                                   {
                                                              (  ) = 2            (  )
                                                             (  ) = 2            (  )
               where       and       are the slip angles of front and rear tire and can be given by:

                                               {
                                                                      (  )
                                                       (  ) =   (  ) −  −   (  )
                                                                  2       .
                                                       (  ) =          (  )  −   (  )
                                                            2
               However, at high lateral acceleration, the tire/road force may not be linearly proportional to the slip angle
               owing to differences in the road surface characteristics and cannot be simply expressed in terms of a constant
               cornering stiffness and sideslip angles. Therefore, we adopt an uncertain cornering stiffness, which varies over
               a range, to model the uncertainty in the tire/road force [31] :

                                                  {
                                                            (  ) = 2      + 2Δ      (•),
                                                                                                       (7)
                                                           (  ) = 2      + 2Δ      (•).

               where       =  max(      (•))+min(      (•))  , Δ      (•) ∈ [−Δ      , Δ      ], Δ      =  max(      (•))−min(      (•)) (   =    ,   ),       (•) denotes
                                                                            2
                                 2
               the uncertain cornering stiffness, and (•) represents all possible variables causing variations in the cornering
               stiffness.
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