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438 Multibody Systems Approach to Vehicle Dynamics<br />

Yaw acceleration (deg/s/s)<br />

1000<br />

800<br />

600<br />

400<br />

200<br />

0<br />

200<br />

400<br />

600<br />

Predicted CN – A y boundary<br />

Measured data 0–90 kph<br />

Measured data 90–130 kph<br />

Measured data 130–250 kph<br />

800<br />

1000<br />

2.0 1.5 1.0 0.5 0.0 0.5 1.0 1.5 2.0<br />

Lateral acceleration (g)<br />

Fig. 7.36 Yaw acceleration versus lateral acceleration for the Subaru WRC<br />

2002, Petter Solberg, Argentina<br />

Yaw acceleration (deg/s/s)<br />

1000<br />

800<br />

600<br />

400<br />

200<br />

0<br />

200<br />

400<br />

Predicted CN–A y<br />

boundary<br />

Measured data 0–90 kph<br />

Measured data 90–130 kph<br />

Measured data 130–250 kph<br />

600<br />

800<br />

1000<br />

2.5 2.0 1.5 1.0 0.5 0.0 0.5 1.0 1.5 2.0 2.5<br />

Lateral acceleration (g)<br />

Fig. 7.37 Yaw acceleration versus lateral acceleration for Subaru WRC 2002,<br />

Petter Solberg, Germany<br />

Examination of the recorded data shows there is little ‘steady state’ about<br />

the rally stage on loose surfaces and the character of the handwheel angle<br />

versus yaw rate trace for the entire stage has a distinctly ‘circular’ quality<br />

about it (Figure 7.38). This indicates that output (yaw) has a phase shift of<br />

around 90 degrees – an indication that the system is indeed at resonance. In

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