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Tyre characteristics and vehicle handling and stability  C HAPTER 11.1


             The axle side force is the sum of the left and right  running, side forces are already present through the in-
           individual tyre side forces. We have:              troduction of e.g. opposite steer and camber angles. If these
                                                              anglesareabsent, theinfluenceofloadtransferispurelynon-
             F yiL ¼ð½C Fai þ z ai DF zi Þða i   j Þ          linear and is only felt at higher levels of lateral accelerations.
                                         io
                                                              In the next subsection, this non-linear effect will be in-
                    þð½C Fgi þ z gi DF zi Þðg   g Þ           corporated in theeffectiveaxlecharacteristic.
                                           io
                                       i
             F yiR ¼ð½C Fai   z ai DF zi Þða i þ j Þ  (11.1.19)
                                         io
                    þð½C Fgi   z gi DF zi Þðg þg Þ            Effective non-linear axle characteristics
                                           io
                                       i
                                                              To illustrate the method of effective axle characteristics
           where the average wheel slip angle a i indicated in the  we will first discuss the determination of the effective
           figure is:                                          characteristic of a front axle showing steering compli-
                                                              ance. The steering wheel is held fixed. Due to tyre side
             a i ¼ a ai þ j i                     (11.1.20)   forces and self-aligning torques (left and right) distor-
                                                              tions will arise resulting in an incremental steer angle j c1
           and the average additional steer angle and the average  of the front wheels (j c1 will be negative in Fig. 11.1-5 for
           camber angle are:                                  the case of just steer compliance). Since load transfer is
                                                              not considered in this example, the situation at the left
             j ¼ j þ j þ j   sfi                  (11.1.21)   and right wheels are identical (initial toe and camber
                   ri
                        ci
              i
             g ¼ g ri                                         angles being disregarded). The front tyre slip angle is
              i
                                                              denoted with a 1 . The ‘virtual’ slip angle of the axle is
             The unknown quantity is the virtual slip angle a ai
           which can be determined for a given lateral acceleration  denoted with a a1 and equals (cf. Fig. 11.1-5):
           a y . Next, we use the Eqs. (11.1.8), (11.1.9), (11.1.13)–                                 (11.1.24)
           (11.1.15) and (11.1.18), substitute the resulting ex-  a a1 ¼ a 1   j c1
           pressions (11.1.21) and (11.1.20)in(11.1.19) and add  where both a 1 and j c1 are related with F y1 and M z1 . The
           up these two equations. The result is a relationship  subscript 1 refers to the front axle and thus to the pair of
           between the axle slip angle a ai and the axle side force F yi .  tyres. Consequently, F y1 and M z1 denote the sum of the
           We obtain for the slip angle of axle i:            left and right tyre side forces and moments. The objec-
                                                              tive is, to find the function F y1 (a a1 ) which is the effective
                   F yi
             a ai ¼                                           front axle characteristic. Fig. 11.1-6 shows a graphical
                  C eff;i                                     approach. According to Eq.(11.1.24) the points on the

                   F yi       lð3 i C Fai þ s i C Fgi Þh 0    F y1 (a a1 ) curve must be shifted horizontally over a length
                ¼       1 þ                     0
                  C Fai    ðl   a i Þðc 41 þ c 42   mgh Þ     j c1 to obtain the sought F y1 (a a1 ). The slope of the curve
                    C Fai ðe i þ t i Þ                        at the origin corresponds to the effective axle cornering
                  þ             C Fai c sfi                   stiffness found in the preceding subsection. Although the
                       C ji
                                                              changes with respect to the original characteristic may be
                    2ls i                                     small, they can still be of considerable importance since it
                  þ     ðz ai j þ z gi g Þ       (11.1.22)
                                    io
                             io
                    l   a i                                   is the difference of slip angles front and rear which
                                                              largely determines the vehicle’s handling behaviour.
             The coefficient of F yi constitutes the effective axle
           cornering compliance, which is the inverse of the effec-
           tive axle cornering stiffness (11.1.17). The quantitative
           effect of each of the suspension, steering and tyre factors
           included can be easily assessed. The subscript i refers to
           the complete axle. Consequently, the cornering and
           camber stiffnesses appearing in this expression are the                                   V
           sum of the stiffnesses of the left and right tyre:
                                                                                                    a1
            C Fai ¼ C FaiL þ C FaiR ¼ C FaiLo þ C FaiRo
                                                  (11.1.23)                                       1
            C Fgi ¼ C FgiL þ C FgiR ¼ C FgiLo þ C FgiRo                                       1
                                                                         M
                                                                           z1
           in which (11.1.7)and (11.1.11) have been taken into ac-                F
           count. The load transfer coefficient s i follows from                    y1
           Eq.(11.1.10). Expression (11.1.22) shows thatthe influence  Fig. 11.1-5 Wheel suspension and steering compliance resulting
           oflateralloadtransferonlyoccursifinitially,atstraightahead  in additional steer angle j 1 .


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