Abstract
The first goal of this chapter is to describe the kinematics of a wheel with tire, mainly under steady-state conditions. This leads to the definitions of slips as a measure of the extent to which the wheel with tire departs from pure rolling conditions. All aspects are discussed in detail and with a critical approach, showing that the use of the slips implies neglecting some phenomena. The slip angle is also defined and discussed. It is shown that a wheel with tire resembles indeed a rigid wheel because slip angles are quite small. The relationships between the kinematics and the forces/couples the tire exchange with the road are investigated by means of experimental tests. The Magic Formula provides a convenient way to represent these functions. Finally, the mechanics of wheels with tire is summarized with the aid of quite a number of plots.
Notes
- 1.
Only in competitions it is worthwhile to employ special (and secret) gas mixtures instead of air. The use of nitrogen, as often recommended, is in fact completely equivalent to air, except for the cost.
- 2.
A rigid wheel is essentially an axisymmetric convex rigid surface. The typical rigid wheel is a toroid.
- 3.
S is the system recommended by ISO (see, e.g., [14, Appendix 1]).
- 4.
- 5.
What is relevant in vehicle dynamics is the moment of (F,M O ) with respect to the steering axis of the wheel. But this is another story.
- 6.
More precisely, it is necessary to have a mathematical description of the shape of the road surface in the contact patch. The plane just happens to be the simplest.
- 7.
We have basically a steady-state behavior even if the operating conditions do not change “too fast”.
- 8.
However, in the brush model, and precisely at p. 294, the effect of the elastic compliance of the carcass on C is taken into account.
- 9.
In a toroidal rigid wheel with maximum radius r 0 and lateral radius s r we would have r r =r 0−s r (1−cosγ), c r =−tanγs r and ε r =0. It follows that \(\dot{c}_{r} \neq- \dot{\gamma}s_{r}\).
- 10.
Common definitions of the slip angle, like “α being the difference in wheel heading and direction” are not sufficiently precise.
- 11.
All other angles are positive angles if measured counterclockwise, as usually done in mathematical writing.
- 12.
In a step steer the steering wheel of a car may reach ω z =20∘/s=0.35 rad/s. At a forward speed of 20 m/s, the same wheels have about ω c =80 rad/s. The contribution of ω z to φ is therefore like a camber angle γ≈0.5∘.
- 13.
sin(Cπ/2)=sin((2−C)π/2), since 1<C<2.
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Guiggiani, M. (2014). Mechanics of the Wheel with Tire. In: The Science of Vehicle Dynamics. Springer, Dordrecht. https://doi.org/10.1007/978-94-017-8533-4_2
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