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Modelling and analysis of suspension systems 199<br />

1.0E00<br />

60 mph<br />

120 mph<br />

Road amplitude (m)<br />

1.0E02<br />

1.0E04<br />

1.0E06<br />

0.1 1 10 100<br />

Frequency (Hz)<br />

Fig. 4.63<br />

Road surface frequency content<br />

where R and K are constants of 2.5 and 5 10 5 respectively. The value of<br />

K varies with the nature of the road being studied. For novel applications or<br />

for previously unknown markets, some measurement of road profiles is<br />

desirable; for the developed western world the values given are generally<br />

appropriate. For military applications, a value of 1 for R may be appropriate.<br />

The very smoothest roads are unlikely to have R higher than 4.<br />

It can be seen that the spectral content as seen by the car varies with vehicle<br />

speed. Gillespie (1992) gives a ‘rational’ argument to suggest that spectral<br />

content rises with speed squared. However, Hales (1989) gives a different<br />

view, reproduced in essence here. The road surface is a process that may be<br />

approximated by a straight line on a log–log plot and represented by<br />

log[u(n)] log[K] R log[n] (4.89)<br />

implying that<br />

K<br />

un ( ) <br />

(4.90)<br />

n R<br />

This is a spatial representation of the road profile, with n defined in<br />

cycles/metre. It appears under the car at frequency of V n Hz, where V is<br />

the forward speed of the car, thus<br />

Vn ⇒ n<br />

(4.91)<br />

2<br />

2V<br />

We can write<br />

gn ( ) 2V<br />

un ( ) gn<br />

( ) <br />

n<br />

u( ) 2 V<br />

(4.92)<br />

if we acknowledge that g(n) g() – i.e. that the process is unchanged<br />

whatever we choose to express it as a function of. Hence:<br />

1 K 1 K<br />

u( )<br />

<br />

m<br />

<br />

2 V n 2 U ( / 2V<br />

)<br />

m<br />

K( 2V)<br />

<br />

m<br />

<br />

m1<br />

(4.93)

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