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Modelling and assembly of the full vehicle 353<br />

For the most common brake rotor material, cast iron, the specific heat versus<br />

temperature characteristic can be approximated in the working range<br />

(0–730°C) by the expression:<br />

c 320 0.15T 1.164 10 9 T 4 (6.15)<br />

Note that in the above expression, temperature T is in centigrade (Celsius)<br />

and not Kelvin. The brake torque and temperature models may be used easily<br />

within a multibody system model using a combination of design variables<br />

(declared in MSC.ADAMS using the ‘variable create’ command) and<br />

run-time variables (declared in MSC.ADAMS using ‘data_element create’<br />

variable) as shown in Table 6.1 where we are using for the first time here an<br />

input format that corresponds to a command language used in MSC.ADAMS.<br />

Note the need for an explicit iteration since the temperature depends on the<br />

heat capacity and the heat capacity depends on the temperature. When<br />

modelling such behaviour in a spreadsheet, it is sufficient to refer to the<br />

temperature of the preceding time step. Although this is possible within<br />

many multibody system packages, it can be awkward to implement and can<br />

also lead to models with some degree of numerical delicacy.<br />

Note also that it is common practice within brake manufacturers to separate<br />

the brake energizing event from the brake cooling event for initial design<br />

calculations, leading to a systematic overestimation of the temperature during<br />

fade/recovery testing. This conservative approach is unsurprising given<br />

the consequences of brake system underdesign. The example given is a relatively<br />

simple one, with convection characteristics that are independent of<br />

vehicle velocity and no variation of brake friction with brake temperature.<br />

Although in practice these simplifications render the results slightly inaccurate,<br />

they are useful when used for comparative purposes – for example, if<br />

the brake temperature model is used with an ESP algorithm it can rank<br />

control strategies in terms of the energy added to individual brake rotors.<br />

Similar modelling is of course possible for other frictional systems within<br />

Joules<br />

2.0E005<br />

1.5E005<br />

1.0E005<br />

50000.0<br />

brake_rotor_heat_in.Q<br />

brake_rotor_heat_out.Q<br />

degrees Celsius<br />

120.0<br />

100.0<br />

80.0<br />

60.0<br />

40.0<br />

rotor_temperature_estimate_2<br />

metres/second<br />

0.0<br />

0.0 0.5 1.0 1.5 2.0 2.5 3.0<br />

Analysis: Last_Run Time (sec) 2003-08-25 16:02:49<br />

30.0<br />

25.0<br />

vehicle_velocity.Q<br />

20.0<br />

15.0<br />

10.0<br />

5.0<br />

0.0<br />

0.0 0.5 1.0 1.5 2.0 2.5 3.0<br />

Analysis: Last_Run Time (sec) 2003-08-25 16:02:49<br />

Joules/kilogram/K<br />

20.0<br />

0.0 0.5 1.0 1.5 2.0 2.5 3.0<br />

Analysis: Last_Run Time (sec) 2003-08-25 16:02:49<br />

340.0<br />

335.0<br />

330.0<br />

325.0<br />

rotor_heat_capacity_estimate_2.Q<br />

320.0<br />

0.0 0.5 1.0 1.5 2.0 2.5 3.0<br />

Analysis: Last_Run Time (sec) 2003-08-25 16:02:49<br />

Fig. 6.29 Output from the brake temperature model shown in Table 6.1<br />

during a 60 mph–0 stop

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