Page 485 - Automotive Engineering Powertrain Chassis System and Vehicle Body
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Modelling and assembly of the full vehicle   C HAPTER 15.1


                                                Weight transfer
                                                            z
                                              Deceleration
                                Brake torque
                                                       x                       Brake torque



                                                Fxbr                           Fxbf

                                          Fzr                             Fzf

           Fig. 15.1-26 Braking of a full vehicle.

             Clearly as the vehicle brakes, as shown in Fig. 15.1-26,  p ¼ the brake pressure
           there is weight transfer from the rear to the front of the  A ¼ the brake piston area
           vehicle. Given what we know about the tyre behaviour  R d ¼ the radius to the centre of the pad
           the change in the vertical loads acting through the tyres
           will influence the braking forces generated. As such the
           braking model may need to account for real effects such  Note that depending on the sophistication of the
           as proportioning the braking pressures to the front and  model the coefficient of friction m may be constant or
           rear wheels or the implementation of anti-lock braking  defined as a run-time variable as a function of brake rotor
           systems (ABS). Before any consideration of this we need  temperature. Obtaining such data is usually relatively
           to address the mechanism to model a braking torque  easy, but the calculation of rotor temperature can be
           acting on a single road wheel.                     a little more involved. Figure 15.1-28 shows typical
             If we consider a basic arrangement the mechanical  specific heat capacity versus temperature characteristics
           formulation of a braking torque, based on a known brake  for different brake rotor materials. Brake rotor temper-
           pressure, acting on the piston can be derived from  ature, T, can be calculated using the expression:
           Fig. 15.1-27.
             The braking torque B T is given by                 T ¼ T 0 þ  B T ut   hA c ðT   T env Þ  (15.1.14)
                                                                                  mc
             B T ¼ nmpAR d                        (15.1.13)
                                                              where
           where
                                                                T 0 ¼ initial brake rotor temperature (K)
                                                                                                      1
             n ¼ the number of friction surfaces (pads)         u ¼ brake rotor spin velocity (rads second )
             m ¼ he coefficient of friction between the pads and  t ¼ time (seconds)
                                                                                                        2  1
                 the disc                                        h ¼ brake rotor convection coefficient (Wm K )




                                                                       B T
                                                                                  F R
                                                              Brake         R
                                  Brake                       disc           d
                                  pad
                                                    P
                                               F N
                                                                                   A
                                Brake
                                piston






           Fig. 15.1-27 Braking mechanism.


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