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Introduction 5<br />

Fig. 1.4 Linearity: more handwheel input results in proportionally more yaw<br />

rate (vehicle on left)<br />

2<br />

1<br />

3<br />

Fig. 1.5 A thought experiment comparing centripetal acceleration with linear<br />

acceleration<br />

acceleration – ‘centre seeking’. Note that speed is not the same as velocity;<br />

travelling in a curved path with a constant speed implies a changing direction<br />

and therefore a changing velocity. The centripetal acceleration definition<br />

causes some problems since everyone ‘knows’ that they are flung to<br />

the outside of a car if unrestrained and so there is much lax talk of centrifugal<br />

forces – ‘centre fleeing’. To clarify this issue, a brief thought experiment<br />

is required (Figure 1.5). Imagine a bucket of water on a rope being<br />

swung around by a subject. If the subject looks at the bucket then the water<br />

is apparently pressed into the bucket by the mythical ‘centrifugal force’<br />

(presuming the bucket is being swung fast enough). If the swinging is<br />

halted and the bucket simply suspended by the rope then the water is held<br />

in the bucket by the downward gravitational field of the earth – the weight<br />

of the water pulls it into the bucket. Imagine now a different scenario<br />

in which the bucket (on a frictionless plane) is pulled horizontally towards<br />

the observer at a constant acceleration in a linear fashion. It’s best not to

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