By T. A. Stolarski, S. Tobe
This publication offers a common advent to the basics of rolling friction with the emphasis on vital engineering functions of rolling contacts. Rolling friction is an age-old engineering challenge, with friction and wear-related difficulties leading to huge, immense expenditures to world-wide. This publication provides the basics of rolling contacts of every kind, emphasizing very important engineering purposes, together with rolling bearings, gears, road-tire and rail-wheel interactions, cam-tappet structures, and roll-forming of fabrics. strategies and strategies of research constructed through the ebook improve figuring out of this complicated topic and aid to enhance the engineer’s skill to layout and choose rolling contacts for mechanical units and platforms. this may be useful to working towards designers, researchers, and postgraduate scholars. Engineering measure direction scholars also will reap the benefits of this book’s thorough advent to rolling contacts conventional in perform.
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Additional resources for Rolling Contacts
6 illustrates the contact of two identical cylinders under conditions of plane strain. Utilizing the symmetry of the contact, it can be l p I Fig. e. to produce a plane contact zone [Fig. 6(a)]. Although this is not strictly true for a cylinder in contact with a plane, the error is small and can be neglected. Thus, a plane contact zone may be assumed. When two identical elastic cylinders are in contact under a normal load P per unit axial length, the resulting plane contact zone has a width of 2a [Fig.
The left-hand side parameter decreases as the surface roughness, defined by cr, increases. 38) The plasticity index is indicative of the onset of plastic deformations within the contact zone. It is large when the contact is basically plastic, and small, less than unity, when the contact is essentially elastic. 1 Surface plastic deformations In this section, a heavy, rigid roller moving steadily over the surface of an elastic-plastic half-space is considered. Resulting deformations of the roller are assumed to be in plane strain.
In the immediate proximity of the ends of the gap, the stress o,, at the points of the x axis becomes positive. This means that the elastic half-planes must exert a tensile traction on each other in order to maintain contact. In the present case, as in the classic statement of the contact problem of the theory of elasticity, a tensile traction between contacting bodies is not admitted. Thus, the case a < 1 is impossible. Now, let it be assumed that a > l . e. for 1x1 > a and y = 0, the stress o,,is negative and, consequently, the elastic half-planes are pressed against each other.