The Hertzian contact surface (original) (raw)
Abstract
It is tempting to accept the predictions regarding indentation depth and radius of circle of contact between two elastic bodies in contact given by the well-known Hertz equations at face value. However, it is nevertheless of interest to examine these predictions either by experiment or by independent computation. Indentation depth may be readily compared using standard experimental apparatus but in this paper, attention is given to the radius of curvature of the indented surface for a condition of full load. The conclusion arising from the Hertz equations, that contact between a flat surface and a non-rigid indenter of radius R is equivalent to that between the flat surface and a perfectly rigid indenter of a larger radius, has not thus far been examined in detail in the literature, possibly because of the difficulty in measuring such a radius of curvature in situ while load is applied to the indenter. This feature of contact between two solids is of interest since it has been often used as the basis for various hardness theories which involve an elastic–plastic contact. This paper addresses the issue by utilizing the finite-element method to compute the radius of curvature of the contact surface for both elastic and elastic–plastic contacts. It is shown that indentations involving elastic–plastic deformations within either or both the specimen and the indenter are equivalent to indentations with a perfectly rigid spherical indenter whose radius is somewhat smaller than that calculated using the Hertz equations for elastic contact. An experimental compliance response is used to indirectly validate the finite-element results.
Access this article
Subscribe and save
- Starting from 10 chapters or articles per month
- Access and download chapters and articles from more than 300k books and 2,500 journals
- Cancel anytime View plans
Buy Now
Price excludes VAT (USA)
Tax calculation will be finalised during checkout.
Instant access to the full article PDF.
Similar content being viewed by others
References
- H. Hertz, J. Reine Angew. Math. 92 (1881) 156; Translated and reprinted in English in "Hertz's Miscellaneous Papers" (Macmillan & Co, London, 1896) Ch. 5.
Google Scholar - H. Hertz, Verhandlungen des Vereins zur Bef¨orderung des Gewerbe Fleisses 61 (1882) 410; Translated and reprinted in English in "Hertz's Miscellaneous Papers" (Macmillan & Co, London, 1896) Ch. 6.
Google Scholar - F. Guiberteau, N. P. Padture, H. Cai and B. R. Lawn, Philos. Mag. A 68 (1993) 1003.
Google Scholar - M. Barquins and D. Maugis, J. Mec. Theor. Appl. 1 (1982) 331.
Google Scholar - K. L. Johnson, in "Contact Mechanics" (Cambridge University Press, 1985).
- D. A. Spence, J. Elast. 5 (1975) 297.
Google Scholar - A. C. Fischer-cripps and R. E. Collins, J. Mater. Sci. 29 (1994) 2216.
Google Scholar - J. S. Field and M. V. Swain, J. Mater. Res. 8 (1993) 297.
Google Scholar - A. C. Fischer-cripps, J. Mater. Sci. 32 (1996) 727.
Google Scholar - M. C. Shaw and D. J. Desalvo, Trans. ASME, J. Eng. Ind. 92 (1970) 469.
Google Scholar - G. Car`e and A. C. Fischer-cripps, J. Mater. Sci. 32 (1997) 5653–5659.
Google Scholar
Authors
- A. C. Fischer-Cripps
Rights and permissions
About this article
Cite this article
Fischer-Cripps, A.C. The Hertzian contact surface.Journal of Materials Science 34, 129–137 (1999). https://doi.org/10.1023/A:1004490230078
- Issue date: January 1999
- DOI: https://doi.org/10.1023/A:1004490230078