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 333<br />

road will therefore be directly related to the roll angle of the vehicle. Spring<br />

and damper forces act between the suspensions and the body. Such suspensions<br />

have been used on early road vehicles, notably the Lancia<br />

Lambda (1908–1927), where it was termed ‘sliding pillar’.<br />

The front wheel knuckles are modelled as separate parts connected to the<br />

lumped suspension parts by revolute joints. The steering motion required<br />

for each manoeuvre is achieved by applying time dependent rotational<br />

motion inputs about these joints. Each road wheel is modelled as a part<br />

connected to the suspension by a revolute joint. The lumped mass model is<br />

shown schematically in Figure 6.7.<br />

6.4.3 Equivalent roll stiffness model<br />

This model is developed from the lumped mass model by treating the front<br />

and rear suspensions as rigid axles connected to the body by revolute<br />

joints. The locations of the joints for the two axles are their respective ‘roll<br />

centres’ as described in Chapter 4. A torsional spring is located at the front<br />

and rear roll centres to represent the roll stiffness of the vehicle. The determination<br />

of the roll stiffness of the front and rear suspensions required an<br />

investigation as described in the following section. The equivalent roll stiffness<br />

model is shown schematically in Figure 6.8.<br />

REV<br />

Torsional<br />

spring damper<br />

Rear axle<br />

Torsional spring<br />

damper<br />

REV<br />

Front axle and<br />

wheel knuckles<br />

Fig. 6.8<br />

Equivalent roll stiffness model approach

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

Saved successfully!

Ooh no, something went wrong!