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258 Multibody Systems Approach to Vehicle Dynamics<br />

<br />

SPIN<br />

AXIS<br />

OVERTURNING<br />

MOMENT<br />

(M x )<br />

TRACTIVE FORCE<br />

(F x )<br />

WC<br />

{X SAE } 1<br />

α<br />

P<br />

ROLLING RESISTANCE<br />

MOMENT (M y )<br />

SELF-ALIGNING<br />

MOMENT<br />

(M y )<br />

{Z SAE } 1<br />

{Y SAE } 1<br />

LATERAL FORCE<br />

(F y )<br />

NORMAL FORCE<br />

(F z )<br />

Fig. 5.12<br />

Tyre forces and moments shown acting in the SAE tyre axis system<br />

The use of the term stiffness can also add confusion to newcomers to the<br />

subject area. A traditional static force/displacement approach is used by<br />

Moore (1975) to define longitudinal, lateral and torsional stiffness of a<br />

tyre. In each case a non-rolling tyre is mounted on a plate and incrementally<br />

loaded as indicated in Figure 5.13 until complete sliding occurs.<br />

Plotting graphs of force or moment against displacement or rotation allows<br />

the stiffness parameters to be obtained from the slopes at the origin.<br />

We will see later that terms such as cornering stiffness and aligning moment<br />

stiffness are associated with a rolling tyre and should not be confused with<br />

the lateral and torsional stiffness defined here. The term longitudinal stiffness<br />

can be particularly misleading as another definition is commonly used<br />

when longitudinal tractive forces due to driving and braking are discussed.<br />

The explanations that follow will initially deal with each force mechanism<br />

in isolation, for example lateral forces arising due to slip angle and camber<br />

angle are considered separately with no simultaneous longitudinal tractive<br />

force. Following this, a more complex treatment involving combinations of<br />

the various force components will be addressed.<br />

5.4.2 Normal (vertical) force calculations<br />

The calculation of normal force in the tyre is relatively straightforward compared<br />

with the calculation of longitudinal or lateral forces. The normal force<br />

will, however, always be negative when computed using the SAE tyre axis<br />

system. This is not particularly elegant when presenting the dependencies of<br />

other force components on the normal force. To overcome this a positive<br />

value of this force component is often referred to as vertical force or tyre<br />

load. In SAE J670e (SAE Publication, 1976) vertical load is taken as the<br />

negative of normal force.

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