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Simulation output and interpretation 415<br />

K Tr<br />

RC rear<br />

Roll<br />

axis<br />

F ROy<br />

F ROz<br />

F RIy<br />

h<br />

A y<br />

K Tf<br />

F RIz<br />

RC front<br />

F FOy<br />

F FIy<br />

F FOz<br />

F FIz<br />

Fig. 7.19 Free-body diagram roll stiffness model during cornering<br />

Consider next the components of force and moment acting on the vehicle<br />

body in isolation.<br />

Using the roll stiffness model as the basis for the analysis we are treating<br />

the body as a single rigid axis with forces and moments transmitted from<br />

the front and rear suspensions (axles) at points representing the front and<br />

rear roll centres as shown in Figure 7.20. Consider the forces and moments<br />

acting on the vehicle body rigid roll axis. Note that we are ignoring the<br />

inclination of the roll axis. A roll moment (mA y h) acts about the axis and<br />

is resisted in the model by the moments M FRC and M RRC resulting from the<br />

front and rear roll stiffnesses K Tf and K Tr :<br />

FFRCy FRRCy mAy 0<br />

(7.17)<br />

MFRC MRRC mAy h 0<br />

(7.18)<br />

The roll moment causes weight transfer between inner and outer wheels<br />

(Figure 7.21). Taking moments for each of the front and rear axles shown<br />

gives:<br />

M<br />

⎛ K<br />

FRC<br />

Tf<br />

⎞<br />

FFzM<br />

may<br />

h<br />

t<br />

⎜<br />

f<br />

KTf K<br />

⎟ 1<br />

⎝<br />

Tr ⎠ tf<br />

(7.19)<br />

M<br />

⎛ K ⎞<br />

RRC<br />

Tr<br />

FRzM<br />

may<br />

h<br />

t<br />

⎜<br />

r<br />

KTf K<br />

⎟ 1<br />

⎝<br />

Tr ⎠ tr<br />

(7.20)<br />

It can be seen from equations (7.19) and (7.20) that if the front roll stiffness<br />

K Tf is greater than the rear roll stiffness K Tr there will be more weight transfer<br />

at the front (and vice versa). It can also be seen that an increase in track

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