01.05.2017 Views

4569846498

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Modelling and assembly of the full vehicle 351<br />

6.9 Modelling of vehicle braking<br />

In Chapter 5 the force and moment generating characteristics of the tyre were<br />

discussed and it was shown how the braking force generated at the tyre contact<br />

patch depends on the slip ratio as the wheel is braked from a free rolling<br />

wheel with a slip ratio of zero to a fully locked wheel where the slip ratio is<br />

unity. In this section we are not so much concerned with the tyre, given that<br />

we would be using a tyre model interfaced with our full vehicle model to<br />

represent this behaviour. Rather we now address the modelling of the mechanisms<br />

used to apply a braking torque acting about the spin axis of the road<br />

wheel that produces the change in slip ratio and subsequent braking force.<br />

Clearly as the vehicle brakes, as shown in Figure 6.26, there is weight<br />

transfer from the rear to the front of the vehicle. Given what we know about<br />

the tyre behaviour the change in the vertical loads acting through the tyres<br />

will influence the braking forces generated. As such the braking model<br />

may need to account for real effects such as proportioning the braking pressures<br />

to the front and rear wheels or the implementation of anti-lock braking<br />

systems (ABS). Before any consideration of this we need to address the<br />

mechanism to model a braking torque acting on a single road wheel.<br />

If we consider a basic arrangement the mechanical formulation of a braking<br />

torque, based on a known brake pressure, acting on the piston can be<br />

derived from Figure 6.27.<br />

The braking torque B T is given by<br />

B T npAR d (6.13)<br />

where<br />

n the number of friction surfaces (pads)<br />

the coefficient of friction between the pads and the disc<br />

p the brake pressure<br />

A the brake piston area<br />

R d the radius to the centre of the pad<br />

Note that depending on the sophistication of the model the coefficient of<br />

friction may be constant or defined as a run-time variable as a function<br />

of brake rotor temperature. Obtaining such data is usually relatively easy,<br />

but the calculation of rotor temperature can be a little more involved.<br />

Weight transfer<br />

Brake torque<br />

Deceleration<br />

x<br />

z<br />

Brake torque<br />

Fxbr<br />

Fxbf<br />

Fig. 6.26<br />

Fzr<br />

Braking of a full vehicle<br />

Fzf

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!