By Robert Horigan Smith
ISBN-10: 0849381363
ISBN-13: 9780849381362
Taking a mechanistic strategy that emphasizes the actual habit of rubber because it slides, Analyzing Friction within the layout of Rubber items and Their Paired Surfaces integrates the engineering and clinical facts demonstrating that the legislation of steel friction don't follow to rubber. The e-book additionally offers a newly constructed, scientifically dependent unified idea of rubber friction that includes a fourth easy rubber friction strength: floor deformation hysteresis.
With purposes that phenomenologically deal with either static and dynamic rubber friction, the ebook bargains useful assistance for enforcing the unified concept within the research and layout procedures. using this conception permits entire calculations of rubber friction, thereby providing possibilities to reinforce public defense. whereas the idea applies to all elastomeric items the place friction is a controversy, the writer essentially specializes in:
• reading friction within the layout of rubber tires and their contacted pavements
• The geometric layout of roadways
• motorized vehicle coincidence reconstruction
• studying slip resistance within the layout of sneakers and their contacted strolling surfaces
Supported by way of large analytical proof, this publication info what rubber friction is and why it behaves how it does.
Read Online or Download Analyzing Friction in the Design of Rubber Products and Their Paired Surfaces PDF
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Additional info for Analyzing Friction in the Design of Rubber Products and Their Paired Surfaces
Example text
These were compressed against a glass plate on which a measuring scale had been engraved. The areas of apparent or nominal contact at various loads were determined. ) The radii r of the apparent contact areas between the three rubber hemispheres and the glass scale were found to be proportional to FN1/3. This suggested that the rubber friction force is proportional to FN1/3. Schallamach’s [3] compressed-rubber findings were consistent with Bowden’s [4] suggestion because the Hertz [5] relationship can also be expressed as r = c(FN)−1/3.
To avoid confusion with the metallic coefficient of friction, μm, μA will not be referred to as a coefficient. 10) where m is the exponent equaling the slope of the µA vs. FN plot when rectified on logarithmic coordinates. 10 plots when rectified will be downward, m is negative in both instances. Applying the conceptually straightforward Hertz [5] equation allows calculation of circular contact areas between surfaces with complex configurations that have been idealized. 6b). The hyperbolic form fits test data from processes in which something is decreasing while another something is increasing, such as the coefficient of rubber friction µ with FN.
The rubber then experienced elastic release as the rolling objects moved out of contact. Such compression or extension resulted in energy losses, constituting a hysteretic deformational friction component. Because a portion of the bulk of the rubber was involved, bulk deformation hysteresis was the operative mechanism. The bulk hysteretic losses elucidated by Tabor [9] constitute a basic friction force developed in rubber. When this rolling or sliding mechanism is experienced by rubber in contact with smooth surfaces, it is often seen that negligible permanent deformation occurs.
Analyzing Friction in the Design of Rubber Products and Their Paired Surfaces by Robert Horigan Smith
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