Page 356 - Automotive Engineering Powertrain Chassis System and Vehicle Body
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Tyre characteristics and vehicle handling and stability  C HAPTER 11.1

















           Fig. 11.1-31 On the stability of a trailer (Exercise 11.1.4).

           limit-cycle). This is an unfortunate, possibly dangerous  the introduction of this extra term will be beneficial
           situation!                                         particularly when the system to be modelled is more
                                                              complex.
           Exercise 11.1.4. Stability of a trailer              Assess the condition for stability for this fourth-order
                                                              system. Simplify the system by putting g ¼ f and
           Consider the trailer of Fig. 11.1-31 that is towed by  c 4 ¼ k 4 ¼ 0. Now find the explicit conditional state-
           a heavy steadily moving vehicle at a forward speed Valong  ment for the cornering stiffness C.
           a straight line. The trailer is connected to the vehicle by
           means of a hinge. The attachment point shows a lateral
           flexibility that is represented by the lateral spring with  11.1.3.7 Vehicle dynamics at more
           stiffness c y . Furthermore, a yaw torsional spring and  complex tyre slip conditions
           damper are provided with coefficients c 4 and k 4 .
             Derive the equations of motion of this system with  So far, relatively simple vehicle dynamics problems have
           generalised coordinates y and 4. Assume small displace-  been studied in which the basic steady-state cornering
           ments so that the equations can be kept linear. The  force vs slip angle characteristic plays the dominant role.
           damping couple k 4 _ 4 may be considered as an external  The situation becomes more complex when matters like
           moment acting on the trailer or we may use the dissi-  combined slip at hard braking, wheel camber, tyre tran-
                                 2
           pation function D¼ ½k 4 _ 4 and add þvD=v_ q to the left-  sient and vibrational properties and e.g. obstacle cross-
                                                i
           hand side of Lag range’s equation (11.1.25). Obviously,  ings are to be considered.




































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