Abstract
This brief introductory article summarizes key findings from experiments and from computer simulations concerning the dramatic changes that commonly occur adjacent to sliding interfaces. We conclude that a wide range of observed features depends on a few basic processes (plastic deformation, interactions with the environment (including the counterface) and mechanical mixing) and that sliding leads to flow patterns similar to those expected in fluid flow.
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It is now widely recognized that sliding dramatically changes the material adjacent to the sliding interface. The modified material, simply called ‘tribomaterial’ here, has been given many other names, including the following: amorphous layer, Beilby layer, transfer layer, fragmented layer, highly deformed layer, glaze layer, white-etching layer, nanocrystal layer, third body [1] and mechanically mixed material. Sliding commonly produces tribomaterial that is both structurally and chemically different from the bulk material [2, 3]. The development of this tribomaterial influences both friction and wear and suggests that simple models, e.g., familiar adhesion, delamination, fatigue and oxidation models, are not adequate for understanding and controlling sliding behavior.
Experimental observations during and after sliding, combined with computer simulations [2–16], show why our understanding of sliding processes has been elusive. In contrast to abrasion, which can be described in terms of geometry, relative hardness, indentation and microcutting [17], sliding commonly involves all of the following: large plastic strains and strain gradients, high strain rates and strain rate gradients, mechanical mixing of components from both contacting solids and from the environment, and various recovery processes, some of which may occur after sliding has ceased [3, 14, 16]. Sliding can drive the affected material very far from equilibrium, allowing levels of solubility and the appearance of phases not expected from experience with systems that are closer to equilibrium [2, 18]. Similar processes and products have been observed when mechanical alloying occurs in high-energy ball mills [2].
A wide range of observed features depends on a few basic processes: plastic deformation, interactions with the environment (including the counterface) and mechanical mixing. These processes are not adequately incorporated in traditional models [19, 20] of friction and wear. The composition and properties of the mixed material can vary widely for different materials and sliding conditions, so there can be a broad range of sliding behavior despite the involvement of the same basic processes. Special cases, e.g., effects of phase transformations, particle cracking, degradation of lubricants, etc., contribute to sliding behavior, but within the same broad framework.
Molecular dynamics (MD) simulations suggest for both crystalline and amorphous materials that sliding leads to flow patterns similar to those expected in fluid flow [6–16]. Mixing occurs when a Kelvin–Helmholtz shear instability [21, 22] leads to vorticity, and the size scale of the vortices is similar to that of grain sizes in nanocrystals. This correlation suggests that vorticity drives mechanical mixing and is at least partially responsible for the development of nanocrystalline material during sliding and during other processes involving severe plastic deformation. Recent results suggest that the formation of nanocrystals may be influenced by vorticity-driven dynamic recrystallization [16]. The disappearance of markers is also associated with vorticity. The simulations show dramatic rearrangements of structure when the normal load is removed or when sliding ceases [14, 16]. These observations raise important questions about conclusions based on even the most careful post-test observations of tribomaterial.
In all cases reported, the tribomaterial that develops during sliding is clearly different from the bulk material in the contacting materials. Therefore, a focus on the tribomaterial and its properties will be needed to develop friction and wear models that are physically reasonable and ultimately useful. In the case of wear models, the fracture characteristics of the tribomaterial need to be incorporated.
Figures 1, 2, 3, 4, 5, 6, 7 and 8 provide experimental and simulation examples of structures produced during the sliding of materials. The tribomaterial examples given here are in the regimes of nano- and micro-structure. However, similarities with structures produced in bubble rafts [23] and in structures observed after slip associated with earthquakes [24] suggest that the processes described here are quite general and may be important over a wide range of size scales, from the nanoscale to the macroscopic.
References
Berthier, Y.: Maurice Godet’s third body. In: Dowson, D., Taylor, C.M., Childs, T.H.C., Dalmaz, G., Berthier, Y., Flamand, L., Georges, J.-M., Lubrecht, A.A. (eds.) The Third Body Concept: Interpretation of Tribological Phenomena, Proceedings of 22nd Leeds-Lyon Symposium on Tribology. Elsevier, Amsterdam (1996)
Rigney, D.A., Chen, L.H., Naylor, M.G.S., Rosenfield, A.R.: Wear processes in sliding systems. Wear 100, 195–219 (1984)
Rigney, D.A.: Transfer, mixing and associated chemical and mechanical processes during the sliding of ductile materials. Wear 245, 1–9 (2000)
Hammerberg, J.E., Holian, B.L., Zhou, S.J.: Studies of sliding friction in compressed copper. In: AIP Conference Proceedings, Seattle, Washington, 13–18 August 1995, vol. 370, p. 307 (1996)
Hammerberg, J.E., Holian, B.L., Röder, J., Bishop, A.R., Zhou, S.J.: Nonlinear dynamics and the problem of slip at material interfaces. Physica D123, 330–340 (1998)
Rigney, D.A., Hammerberg, J.E.: Unlubricated sliding behavior of metals. MRS Bull. 23(6), 32–36 (1998)
Fu, X.Y., Falk, M.L., Rigney, D.A.: Sliding behavior of metallic glass. Part II. Computer simulations. Wear 250, 420–430 (2001)
Rigney, D.A., Fu, X.Y., Hammerberg, J.E., Holian, B.L., Falk, M.L.: Examples of structural evolution during sliding and shear of ductile materials. Scr. Mater. 49, 977–983 (2003)
Subramanian, K., Wu, J.-H., Rigney, D.A.: The role of vorticity in the formation of tribomaterial during sliding. In: Materials Research Society Proceedings, San Francisco, CA, 13–16 April 2004, vol. 821, pp. 9.6.1–9.6.6 (2004)
Wu, H.H., Karthikeyan, S., Falk, M.L., Rigney, D.A.: Tribological characteristics of diamond-like carbon (DLC) based nanocomposites coatings. Wear 259, 744–751 (2005)
Kim, H. J., Emge, A., Subramanian, K., Rigney, D.: An experimental and theoretical study of microstructure evolution during sliding. In: Rohrer, G.S., Karma, A.S., Wynblatt, P.P., Rollett, A.D., Srolovitz, D.J., Farkas, D., Chatain, D., Woodward, C.F. (eds.) Symposium on Integration of Theoretical, Computational and Experimental Studies of Interfaces and Microstructural Evolution. Materials Science and Technology 2005. ASM, ACerS, AIST, AWS, TMS, Pittsburgh, PA (2005)
Karthikeyan, S., Kim, H.J., Rigney, D.A.: Velocity and strain-rate profiles in materials subjected to unlubricated sliding. Phys. Rev. Lett. 95, 1–4 (2005)
Kim, H.J., Windl, W., Rigney, D.A.: Structure and chemical analysis of aluminum wear debris: experiments and ab initio simulations. Acta Mater. 55, 6489–6498 (2007)
Kim, H.J., Kim, W.K., Falk, M.J., Rigney, D.A.: MD simulations of microstructure evolution during high-velocity sliding between crystalline materials. Tribol. Lett. 28, 299–306 (2007)
Kim, H.J., Karthikeyan, S., Rigney, D.: A simulation study of the mixing, atomic flow and velocity profiles of crystalline materials during sliding. Wear 267, 1130–1136 (2009)
Karthikeyan, S., Agrawal, A., Rigney, D.A.: Molecular dynamics sliding simulations in an Fe-Cu Tribopair System. Wear 267, 1166–1176 (2009)
Samuels, L.E.: Metallographic Polishing by Mechanical Methods, 3rd edn. American Society for Metals, Metals Park, OH (1982)
Bellon, P., Averback, R.S.: Peface to viewpoint set on: materials under driving forces. In Viewpoint Set No. 32. Scr. Mater. 49, 921–925 (2003)
Rabinowicz, E.: Friction and Wear of Materials. Wiley, New York (1965)
Bowden, F.P., Tabor, D.: The Friction and Lubrication of Solids, Part II. Clarendon Press, Oxford (1964)
Kelvin, W.: Hydrokinetic solutions and observations. Philos. Mag. 42, 362–377 (1871)
Von Helmholtz, H.L.F.: On discontinuous movements of fluids. Philos. Mag. 36, 337–346 (1868)
Mazuyer, D., Georges, J.M., Cambou, B.: Shear behavior of an amorphous film with bubble soap raft model. J. Phys. France 49, 1057–1067 (1989)
Little, T.A., Holcombe, R.J., Ilg, B.R.: Ductile fabrics in the zone of active oblique convergence near the alpine fault, New Zealand: identifying the neotectonic overprint. J. Struct. Geol. 24, 193–217 (2002)
Acknowledgments
The authors are pleased to acknowledge the contributions of J.E. Hammerberg (Los Alamos National Laboratory), M.L. Falk (University of Michigan and Johns Hopkins University, W.K. Kim (University of Michigan), W. Windl (Materials Science and Engineering (MSE), The Ohio State University (OSU)) and recent members of the tribology research group in MSE at OSU, especially X.Y. Fu, T. Kasai, J.H. Wu, H.J. Kim and A. Emge. We are also grateful to the following research sponsors: The National Science Foundation (NSF), U. S. Civilian Research and Development Foundation (CRDF), Dayton Area Graduate Studies Institute (DAGSI), U. S. Department of Energy (DOE/NNSA/SSAA), Los Alamos National Laboratory, Ohio Supercomputer Center and the Michigan Center for Parallel Computing.
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Rigney, D.A., Karthikeyan, S. The Evolution of Tribomaterial During Sliding: A Brief Introduction. Tribol Lett 39, 3–7 (2010). https://doi.org/10.1007/s11249-009-9498-3
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DOI: https://doi.org/10.1007/s11249-009-9498-3