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Simulation output and interpretation 403<br />

So it can be seen that above a limiting speed, given by<br />

V<br />

lowlimit <br />

gL<br />

(( )/ 2)( / 180)<br />

i<br />

o<br />

(7.7)<br />

it is the surface grip that determines the limiting yaw rate and hence path<br />

curvature. For typical passenger cars, the region in which geometry dominates<br />

steering behaviour is small – up to about 15 mph. This is the speed<br />

that may be counted as ‘low’ and in which Figure 7.5 is a reasonable<br />

description of the behaviour of the vehicle. For vehicles such taxis and<br />

heavy goods vehicles, the low speed region is of more importance simply<br />

because these vehicles make more low speed, minimum radius manoeuvres.<br />

However, they rarely perform these manoeuvres at speeds exceeding walking<br />

pace and so the yaw rates remain low.<br />

The steer angles required to avoid scrubbing at the inner and outer road<br />

wheels, o and i are:<br />

L<br />

<br />

⎛180⎞<br />

o<br />

( R 0.5 t)<br />

⎝ ⎠<br />

(7.8)<br />

L<br />

<br />

⎛180⎞<br />

i<br />

( R 0.5 t)<br />

⎝ ⎠<br />

(7.9)<br />

The angle of a notional ‘average’ wheel on the vehicle centre line, , is the<br />

‘Ackermann’ angle – the approximate form is in common usage:<br />

LR<br />

<br />

⎛180⎞<br />

L 180<br />

( 0.25<br />

2<br />

R t ) ⎝ ⎠ ≈ ⎛ ⎞<br />

R ⎝ ⎠<br />

(7.10)<br />

In 1817, Rudolph Ackermann patented geometry similar to this as an<br />

improvement over a steered axle as was common on horse-drawn vehicles.<br />

That the geometry we today call ‘Ackermann’ was in fact a modification<br />

proposed by the Frenchman Charles Jeantaud in 1878 has been lost in the<br />

mists of time. Some measure of how accurately the steering geometry corresponds<br />

to the Ackermann/Jeantaud description is often quoted although<br />

rarely defined. The authors use a description as given in Figure 7.7, which<br />

in turn uses the simplified form of equation (7.10).<br />

The Ackermann/Jeantaud angles are calculated as given in equations (7.8)<br />

and (7.9). These are compared with the angles actually achieved by the<br />

front wheels. A fraction of the compensation is expressed for the outer<br />

wheel using mean for the mean of the actual angles:<br />

Ackermann fraction <br />

o<br />

_ actual − mean<br />

L/ ( 180/ )( L/ ) 0.5 t (180/ )<br />

<br />

[ [ mean ]]<br />

mean<br />

(7.11)<br />

This is the quantity graphed in Figure 7.7 as ‘% Ackermann’. The values<br />

shown (around 40%) are typical for road cars. There exists some confusion<br />

over the significance of Ackermann geometry. For ride and handling work,

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