Page 166 - Tribology in Machine Design
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152   Tribology in machine design


                                4.14.1. Creep of an automobile tyre
                                An automobile tyre will tend to creep longitudinally if the circumferential
                                strain in the contact patch is different from that in the unloaded periphery.
                                In accordance with the theory of the membrane, there is a shortening in the
                                contact patch of the centre-line of the running surface. This is equal to the
                                difference between the chord AB and the arc AB (see Fig. 4.48). This leads to
                                a strain and consequently to a creep given here as a creep ratio:





                                The silent assumption regarding eqn (4.177) is that the behaviour of the
                                contact is controlled by the centre-line strain and that there is no strain
                                outside the contact. The real situation, however, is different.



                                4.14.2. Transverse tangential forces
                                Transverse frictional forces and moments are operating when the plane of
                                the tyre is slightly skewed to the plane of the road. This is usually called
                                sideslip. Similar conditions arise in the response to spin when turning a
                                corner. The usual approach to these problems is the same as that for solid
                                bodies. The analysis starts with the contact being divided into a stick region
                                at the front edge of the contact patch and a slip region at the rear edge. The
                                slip region tends to spread forward with the increase in sideslip or spin.
                                Figure 4.50 shows one-dimensional motion describing the resistance of the
                                tyre to lateral displacement. This displacement, k, of the equatorial line of
                                the tyre results in its lateral deformation. The displacement, k is divided into
                                displacement of the carcass, /c c, and the displacement of tread, /c t. The
                                carcass is assumed to carry a uniform tension R resulting from the internal
                                pressure. This tension acts against lateral deflection. The lateral deflection
                                is also constrained by the walls acting as a spring of stiffness G per unit
                                length. The tread also acts as an elastic foundation. Surface traction, g(x),
                                acting in the region — c^x ^ c deforms the tyre. The equilibrium equation
                                is of the form

















                      Figure 4.50
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