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3.4 Behavioral Capabilities for Locomotion      97


              For the data mentioned, the lane change time is T LC  =  2.68 seconds, and  the
            maximum speed at the center of the idealized maneuver is v ymaxLCi  {t = T LC/2} =
            2.68 m/s. Since Ackermann steering is nonholonomic, real cars cannot perform this
            type of lane change maneuver; however, it is nice as a reference for realizable ma-
            neuvers to be discussed in the following. For a y = 4 m/s², lane change time would
            be 1.9 seconds and maximum lateral speed v y (T LC/2) = 3.8 m/s.

            Fifth-order dynamic model for lateral road vehicle guidance: The very busy
            Figure 3.23 shows the basic properties of a simple but full order (linear) bicycle

                                                 Inertial reference direction
                                Axle distance a
                       °
                      l ȥ      V r  Į r   cg  ȥ °  ȥ  Ȥ  F xf  f  l ȥ °
                      r
                       r       ¤          ¤                ¤  f
                                                      ȕ
                    F                          V                     Ȝ
                     xr
                                                      F
                      F yr        P                    yf      V
                                   l r           l f            f    Į f
                       R r      R r       Ȝ   steer angle (first integral of
                                              control variable)
                             l P          ȕ   side slip angle at cg
                                          °
                                          ȥ   yaw rate (inertial)
                                          l f  distance from cg to front axle
                                          l   distance from cg to rear axle
                                           r
                                          Į f  angle of attack at front wheel
                                          Į   angle of attack at rear wheel
                                           r
                                          V   velocity vector of cg
                                          V f  velocity vector of front wheel
                                          V   velocity vector of rear wheel
                                           r
                                          P   point on longitudinal axis of body
                                              where the velocity vector is
                              (effective      tangential to body
                              center of   R   turn radius of vehicle body
                              rotation)     r
                                          F ij  tire force components tangential
                                              (index x) and normal to wheel (y)
                        ¤ M 0  ¤ M
                            Figure 3.23. Bicycle model with rotational dynamics


            model, taking combined tire forces from both the left- and right-hand side as well
            as translational and rotational dynamics into account. [The full  model with all
            nonlinearities and separately modeled dynamics for the wheel groups and the body
            is too complex to allow analytical solutions; these are used in numerical simula-
            tions.] Here, interest lies in some major effects of lateral maneuvering for turns and
            lane changes.  More involved  models may  be found in  [Mitschke 1990; Giampiero
            2007].
              Side forces on the wheels (index y) are generated by introducing an angle of at-
            tack at the front wheel(s) through a steering angle Ȝ. Tires may be considered to act
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