4569846498
Modelling and assembly of the full vehicle 387 Vertical force (N) 10000.0 9000.0 8000.0 7000.0 6000.0 5000.0 4000.0 3000.0 2000.0 1000.0 0.0 Fig. 6.57 0.0 FRONT RIGHT TYRE – 100 km/LANE CHANGE Roll stiffness model Linkage model 1.0 _ _ _ _ _ _ _ __________ 3.0 2.0 Time (s) Vertical tyre force comparison – linkage and roll stiffness models 4.0 5.0 example, at the error measured between the experimental and simulated results for the peaks in the response or to sum the overall error from start to finish. On that basis it may seem desirable to somehow ‘score’ the models giving, say, the linkage model 8/10 and the roll stiffness model 7/10. In light of the above questions the validity of such an objective measure is debatable and it is probably more appropriate to simply state: For this vehicle, this manoeuvre, the model data, and the available benchmark test data the equivalent roll stiffness model provides reliable predictions when compared with the linkage model for considerably less investment in model elaboration. Clearly it is also possible to use an understanding of the physics of the problem to aid the interpretation of model performance. An important aspect of the predictive models is whether the simplified suspension models correctly distribute load to each tyre and model the tyre position and orientation in a way that will allow a good tyre model to determine forces in the tyre contact patch that impart motion to the vehicle and produce the desired response. Taking this a step further we can see that if we use the equivalent roll stiffness and linkage models as the basis for further comparison it is possible in Figures 6.57 and 6.58 to compare the vertical force in, for example, the front right and left tyres. The plots indicate the performance of the simple equivalent roll stiffness model in distributing the load during the manoeuvre. The weight transfer across the vehicle is also evident as is the fact that tyre contact with the ground is maintained throughout. It should also be noticed that in determining the load transfer to each wheel the equivalent roll stiffness model does not include the degrees of freedom that would allow the body to heave or pitch relative to the suspension systems. In Figures 6.59 and 6.60 a similar comparison between the two models is made, this time considering, for example, the slip and camber angles predicted in the front right tyre.
388 Multibody Systems Approach to Vehicle Dynamics 10000.0 FRONT LEFT TYRE – 100 km/h LANE CHANGE 9000.0 8000.0 Roll stiffness model Linkage model _ _ _ _ _ _ _ __________ Vertical force (N) 7000.0 6000.0 5000.0 4000.0 3000.0 2000.0 1000.0 0.0 0.0 1.0 2.0 3.0 4.0 5.0 Time (s) Fig. 6.58 Vertical tyre force comparison – linkage and roll stiffness models Slip angle (deg) 6.0 5.0 4.0 3.0 2.0 1.0 0.0 1.0 2.0 3.0 4.0 5.0 6.0 0.0 FRONT RIGHT TYRE – 100 km/h LANE CHANGE Roll stiffness model Linkage model 1.0 2.0 _ _ _ _ _ _ _ __________ Time (s) 3.0 4.0 5.0 Fig. 6.59 Slip angle comparison – linkage and roll stiffness models Although the prediction of slip angle agrees well it can be seen in Figure 6.60 that the equivalent roll stiffness model with a maximum value of about 1.5 degrees underestimates the amount of camber angle produced during the simulation when compared with the linkage model where the camber angle approaches 5 degrees. Clearly the wheels in the effective roll stiffness model do not have a camber degree of freedom relative to the rigid axle parts and the camber angle produced here is purely due to tyre deflection.
- Page 360 and 361: Modelling and assembly of the full
- Page 362 and 363: Modelling and assembly of the full
- Page 364 and 365: Modelling and assembly of the full
- Page 366 and 367: Modelling and assembly of the full
- Page 368 and 369: Modelling and assembly of the full
- Page 370 and 371: Modelling and assembly of the full
- Page 372 and 373: Modelling and assembly of the full
- Page 374 and 375: Modelling and assembly of the full
- Page 376 and 377: Modelling and assembly of the full
- Page 378 and 379: Modelling and assembly of the full
- Page 380 and 381: Modelling and assembly of the full
- Page 382 and 383: Modelling and assembly of the full
- Page 384 and 385: Modelling and assembly of the full
- Page 386 and 387: Modelling and assembly of the full
- Page 388 and 389: Modelling and assembly of the full
- Page 390 and 391: Modelling and assembly of the full
- Page 392 and 393: Modelling and assembly of the full
- Page 394 and 395: Modelling and assembly of the full
- Page 396 and 397: Modelling and assembly of the full
- Page 398 and 399: Modelling and assembly of the full
- Page 400 and 401: Modelling and assembly of the full
- Page 402 and 403: Modelling and assembly of the full
- Page 404 and 405: Modelling and assembly of the full
- Page 406 and 407: Modelling and assembly of the full
- Page 408 and 409: Modelling and assembly of the full
- Page 412 and 413: Modelling and assembly of the full
- Page 414 and 415: Modelling and assembly of the full
- Page 416 and 417: Modelling and assembly of the full
- Page 418 and 419: 7 Simulation output and interpretat
- Page 420 and 421: Simulation output and interpretatio
- Page 422 and 423: Simulation output and interpretatio
- Page 424 and 425: down and even more difficult to asc
- Page 426 and 427: Simulation output and interpretatio
- Page 428 and 429: Simulation output and interpretatio
- Page 430 and 431: Simulation output and interpretatio
- Page 432 and 433: Simulation output and interpretatio
- Page 434 and 435: Simulation output and interpretatio
- Page 436 and 437: Simulation output and interpretatio
- Page 438 and 439: Simulation output and interpretatio
- Page 440 and 441: Simulation output and interpretatio
- Page 442 and 443: Simulation output and interpretatio
- Page 444 and 445: Simulation output and interpretatio
- Page 446 and 447: Simulation output and interpretatio
- Page 448 and 449: Simulation output and interpretatio
- Page 450 and 451: Simulation output and interpretatio
- Page 452 and 453: Simulation output and interpretatio
- Page 454 and 455: Simulation output and interpretatio
- Page 456 and 457: Simulation output and interpretatio
- Page 458 and 459: Simulation output and interpretatio
388 Multibody Systems Approach to Vehicle Dynamics<br />
10000.0<br />
FRONT LEFT TYRE – 100 km/h LANE CHANGE<br />
9000.0<br />
8000.0<br />
Roll stiffness model<br />
Linkage model<br />
_ _ _ _ _ _ _<br />
__________<br />
Vertical force (N)<br />
7000.0<br />
6000.0<br />
5000.0<br />
4000.0<br />
3000.0<br />
2000.0<br />
1000.0<br />
0.0<br />
0.0<br />
1.0<br />
2.0<br />
3.0<br />
4.0<br />
5.0<br />
Time (s)<br />
Fig. 6.58<br />
Vertical tyre force comparison – linkage and roll stiffness models<br />
Slip angle (deg)<br />
6.0<br />
5.0<br />
4.0<br />
3.0<br />
2.0<br />
1.0<br />
0.0<br />
1.0<br />
2.0<br />
3.0<br />
4.0<br />
5.0<br />
6.0<br />
0.0<br />
FRONT RIGHT TYRE – 100 km/h LANE CHANGE<br />
Roll stiffness model<br />
Linkage model<br />
1.0<br />
2.0<br />
_ _ _ _ _ _ _<br />
__________<br />
Time (s)<br />
3.0<br />
4.0<br />
5.0<br />
Fig. 6.59<br />
Slip angle comparison – linkage and roll stiffness models<br />
Although the prediction of slip angle agrees well it can be seen in Figure<br />
6.60 that the equivalent roll stiffness model with a maximum value of about<br />
1.5 degrees underestimates the amount of camber angle produced during the<br />
simulation when compared with the linkage model where the camber angle<br />
approaches 5 degrees. Clearly the wheels in the effective roll stiffness model<br />
do not have a camber degree of freedom relative to the rigid axle parts and<br />
the camber angle produced here is purely due to tyre deflection.