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UWE Bristol Engineering showcase 2015

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Richard Thompson<br />

Motorsport <strong>Engineering</strong><br />

Project Supervisor<br />

Dr Benjamin Drew<br />

Improving the stability of three wheeled vehicles<br />

Preventing a three-wheeler from rolling over is very different to conventional cars. Unlike conventional cars where braking will make the system more stable,<br />

the nature of the geometry means it will actually be more likely to overturn. With this in mind, developing an ESP system for a three wheeler like a Reliant<br />

Robin needs to focused around torque vector control.<br />

Axis Title<br />

30<br />

25<br />

20<br />

15<br />

10<br />

5<br />

0<br />

0<br />

8.1<br />

Three Wheel Rollover Under Acceleration (0.25g)<br />

11.4<br />

13.9<br />

16.1<br />

18<br />

19.7<br />

0 20 40 60 80 100 120<br />

Axis Title<br />

21.3<br />

22.7<br />

24.1<br />

25.4<br />

Accelerating through the corner is actually<br />

favourable for a delta three wheeler with regards<br />

to stability, the acceleration that can occur as a<br />

consequence of torque vectoring is beneficial.<br />

Three Wheel rollover under acceleration (0.5g)<br />

Project summary<br />

This study consists of an investigation into the<br />

rollover stability of three-wheeled vehicles with a<br />

single front wheel, and if the implementation of an<br />

electronic stability program could improve it.<br />

Project Objectives<br />

• To research and understand rollover of three<br />

wheeled vehicles<br />

• To develop a mathematical model for three wheel<br />

rollover .<br />

• Research into the functionality behind ESP<br />

systems.<br />

• To devise a method for increasing the rollover<br />

threshold of the vehicle.<br />

30<br />

This graph results from an input acceleration of<br />

0.5g. The additional longitudinal acceleration<br />

stabilises the vehicle round the corner compared<br />

to the graph above with a lesser value of a. This<br />

illustrates a small element of how controlling<br />

torques can stabilise a three-wheeler<br />

Image below is of a differential capable of<br />

supplying different torques to each wheel.<br />

Axis Title<br />

25<br />

20<br />

15<br />

10<br />

5<br />

0<br />

26.6<br />

25.2<br />

23.8<br />

22.2<br />

20.6<br />

18.8<br />

16.8<br />

14.6<br />

11.9<br />

8.4<br />

0<br />

0 20 40 60 80 100 120<br />

Axis Title<br />

Understeer gradiant<br />

0.05<br />

0.04<br />

0.03<br />

0.02<br />

0.01<br />

0<br />

-0.01<br />

-0.02<br />

Understeer gradiant vs length L1 and L2<br />

length L1/L2 (m)<br />

0 0.5 1 1.5 2 2.5<br />

Project Conclusion<br />

This study had success in discovering that by creating<br />

a longitudinal inertia force through short bursts of<br />

acceleration; the rollover threshold for a delta threewheeler<br />

could be increased resulting in a more stable<br />

system. This study also yielded useful data as to why<br />

differential braking as an option for a stability<br />

program did not suit the geometry of the problem<br />

and in fact had a detrimental effect on the cornering<br />

stability by reducing the rollover threshold.<br />

understeer gradiant vs L1<br />

Understeer gradiant vs L2<br />

The graph above maps the steady state cornering of the<br />

three wheeler assuming no roller, neutral steer occurs<br />

where the lines cross the x-axis. From table 7, neutral steer<br />

occurs when L1 = 1.439333 = 2L/3. So the neutral steer point<br />

occurs when the centre of gravity is closer to the rear axle<br />

then the front. A useful design recommendation to assist<br />

rollover mitigation would be to move the centre of mass<br />

back towards the rear axle towards the neutral steer point.

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