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Modelling and assembly of the full vehicle 361 The purpose of the STEP FUNCTION is to define a change of state in the expression that is continuous. The step function can be used to factor a force function by ramping it on over a set time period. In this case the driving torque is being switched on between time 0 and time 1 second. This is important because it is necessary to perform an initial static analysis of the vehicle at time 0 when Va 0 and the torque must not act. As can be seen a ‘reference’ (desired) state is needed, an error term is defined by the difference between the current state and the reference state and finally, responses to that in terms of throttle or brake application to adjust the speed back towards the reference value. There are two possible approaches; the simplest provides a speed ‘map’ for the track, similar to the curvature map description of it. More elaborately, it is possible to examine the path curvature map locally and decide (through a knowledge of the ultimate capabilities of the vehicle, perhaps) whether or not the current speed is excessive, appropriate or insufficient for the local curvature and use brakes or engine appropriately. For the development of vehicles, open loop throttle or brake inputs may be preferable and are sometimes mandated in defined test manoeuvres, rendering the whole issue of speed control moot. In many ways the skill of the competition driver lies entirely in this ability to judge speed and adjust it appropriately. It is also a key skill to cultivate for limit handling development and arguably for road driving too, so as not to arrive at hazards too rapidly to maintain control of the vehicle. For this functionality, some form of preview is essential. It is both plausible and reasonable to run a ‘here and now at the front axle’ model for the path follower and a ‘previewing’ speed controller within the same model, described in subsequent sections. 6.12 The steering system 6.12.1 Modelling the steering mechanism There are a number of steering system configurations available for cars and trucks based on linkages and steering gearboxes. The treatment in the following sections is limited to a traditional rack and pinion system. Space does not permit discussion of the modelling of power steering or steer-bywire here. For the simple full vehicle models discussed earlier, such as that modelled with lumped mass suspensions, there are problems when trying to incorporate the steering system. Consider first the arrangement of the steering system on the actual vehicle and the way this can be modelled on the detailed linkage model as shown in Figure 6.36. In this case only the suspension on the right-hand side is shown for clarity. The steering column is represented as a part connected to the vehicle body by a revolute joint with its axis aligned along the line of the column. The steering inputs required to manoeuvre the vehicle are applied as motion or torque inputs at this joint. The steering rack part is connected to the vehicle body by a translational joint and connected to the tie rod by a universal
362 Multibody Systems Approach to Vehicle Dynamics Steering column part MOTION Steering motion applied at joint REV Revolute joint to vehicle body COUPLER Steering rack part TRANS Translational joint to vehicle body Front suspension Fig. 6.36 Modelling the steering system. (This material has been reproduced from the Proceedings of the Institution of Mechanical Engineers, K2 Vol. 213 ‘The modelling and simulation of vehicle handling. Part 2: vehicle modelling’, M.V. Blundell, page 129, by permission of the Council of the Institution of Mechanical Engineers) joint. The translation of the rack is related to the rotation of the steering column by a coupler statement that defines the ratio. An example of a statement that would define the ratio is COUPLER/510502,JOINTS 501,502,TYPE T:R ,SCALES 8.45D,1.0 In this case joint 501 is the translational joint and 502 is the revolute joint. The coupler statement ensures that for every 8.45 degrees of column rotation there will be 1 mm of steering rack travel. Attempts to incorporate the steering system into the simple models using lumped masses, swing arms and roll stiffness will be met with a problem when connecting the steering rack to the actual suspension part. This is best explained by considering the situation shown in Figure 6.37. The geometry of the tie rod, essentially the locations of the two ends, is designed with the suspension linkage layout and will work if implemented in an ‘as-is’ model of the vehicle including all the suspension linkages. Physically connecting the tie rod to the simple suspensions does not work. During an initial static analysis of the full vehicle, to settle at kerb height, the rack moves down with the vehicle body relative to the suspension system.
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Modelling and assembly of the full vehicle 361<br />
The purpose of the STEP FUNCTION is to define a change of state in the<br />
expression that is continuous.<br />
The step function can be used to factor a force function by ramping it on<br />
over a set time period. In this case the driving torque is being switched on<br />
between time 0 and time 1 second. This is important because it is necessary<br />
to perform an initial static analysis of the vehicle at time 0 when<br />
Va 0 and the torque must not act.<br />
As can be seen a ‘reference’ (desired) state is needed, an error term is<br />
defined by the difference between the current state and the reference state<br />
and finally, responses to that in terms of throttle or brake application to<br />
adjust the speed back towards the reference value. There are two possible<br />
approaches; the simplest provides a speed ‘map’ for the track, similar to the<br />
curvature map description of it. More elaborately, it is possible to examine<br />
the path curvature map locally and decide (through a knowledge of the ultimate<br />
capabilities of the vehicle, perhaps) whether or not the current speed<br />
is excessive, appropriate or insufficient for the local curvature and use<br />
brakes or engine appropriately. For the development of vehicles, open loop<br />
throttle or brake inputs may be preferable and are sometimes mandated in<br />
defined test manoeuvres, rendering the whole issue of speed control moot.<br />
In many ways the skill of the competition driver lies entirely in this ability<br />
to judge speed and adjust it appropriately. It is also a key skill to cultivate<br />
for limit handling development and arguably for road driving too, so as not<br />
to arrive at hazards too rapidly to maintain control of the vehicle. For this<br />
functionality, some form of preview is essential. It is both plausible and<br />
reasonable to run a ‘here and now at the front axle’ model for the path follower<br />
and a ‘previewing’ speed controller within the same model, described<br />
in subsequent sections.<br />
6.12 The steering system<br />
6.12.1 Modelling the steering mechanism<br />
There are a number of steering system configurations available for cars and<br />
trucks based on linkages and steering gearboxes. The treatment in the following<br />
sections is limited to a traditional rack and pinion system. Space<br />
does not permit discussion of the modelling of power steering or steer-bywire<br />
here.<br />
For the simple full vehicle models discussed earlier, such as that modelled<br />
with lumped mass suspensions, there are problems when trying to incorporate<br />
the steering system. Consider first the arrangement of the steering system<br />
on the actual vehicle and the way this can be modelled on the detailed<br />
linkage model as shown in Figure 6.36. In this case only the suspension on<br />
the right-hand side is shown for clarity.<br />
The steering column is represented as a part connected to the vehicle body<br />
by a revolute joint with its axis aligned along the line of the column. The<br />
steering inputs required to manoeuvre the vehicle are applied as motion or<br />
torque inputs at this joint. The steering rack part is connected to the vehicle<br />
body by a translational joint and connected to the tie rod by a universal