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Tyre characteristics and modelling 285<br />

The measurements of forces and moments were taken using the SAE<br />

co-ordinate system for the following configurations:<br />

(i) Varying the vertical load in the tyre 200, 400, 600, 800 kg.<br />

(ii) For each increment of vertical load the camber angle is varied<br />

from 10 to 10 degrees with measurements taken at 2 degree intervals.<br />

During this test the slip angle is fixed at 0 degrees.<br />

(iii) For each increment of vertical load the slip angle is varied from 10<br />

to 10 degrees with measurements taken at 2 degree intervals. During<br />

this test the camber angle is fixed at 0 degrees.<br />

(iv) For each increment of vertical load the slip and camber angle are<br />

fixed at zero degrees and the tyre is gradually braked from the free<br />

rolling state to a fully locked skidding tyre. Measurements were<br />

taken at increments in slip ratio of 0.1.<br />

The test programme outlined here can be considered a starting point in the<br />

process of obtaining tyre data to support a simulation exercise. In practice<br />

obtaining all the data required to describe the full range of tyre behaviour<br />

discussed in the preceding sections will be extremely time consuming and<br />

expensive. The test programme described here does not, for example, consider<br />

effects such as varying the speed of the test machine, changes in tyre<br />

pressure or wear, changes in road texture and surface contamination by<br />

water or ice. The testing is also steady state and does not consider the transient<br />

state during transition from one orientation to another.<br />

Most importantly the tests do not consider the complete range of combinations<br />

that can occur in the tyre. The longitudinal force testing described is<br />

limited by only considering the generation of braking force. To obtain a<br />

complete map of tyre behaviour it would also, for example, be necessary to<br />

test not only for variations in slip angle at zero degrees of camber angle but<br />

to repeat the slip angle variations at selected camber angles. For comprehensive<br />

slip behaviour it would be necessary at each slip angle to brake or<br />

drive the tyre from a free rolling state to one that approaches the friction<br />

limit, hence deriving the ‘friction circle’ for the tyre.<br />

Extending a tyre test programme in this way may be necessary to generate<br />

a full set of parameters for a sophisticated tyre model but will significantly<br />

add to the cost of testing. Obtaining data requires the tyre to be set up at<br />

each load, angle or slip ratio and running in steady state conditions before<br />

the required forces and moments can be measured. By way of example the<br />

basic test programme described here required measurements to be taken<br />

for the tyre in 132 configurations. Extending this, using the same pattern of<br />

increments and adding driving force to consider combinations of slip angle<br />

with camber or slip ratio would extend the testing to 1452 configurations.<br />

In practice this could be reduced by judicious selection of test configurations<br />

but it should be noted the tests would still be for a tyre at constant<br />

pressure and constant speed on a given test surface. Examples of test results<br />

for a wider range of tyres and settings can be obtained by general reference<br />

to the tyre specific publications quoted in this chapter and in particular to<br />

the textbook by Pacejka (2002).<br />

For the tyre tests described here the following is typical of the series<br />

of plots that would be produced in order to assess the force and moment

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