Friction coefficient evaluation using physically based viscoplasticity model at the contact region during high velocity sliding

Many physical systems require the description of mechanical interactions across interfaces if they are to be successfully analyzed. One of the well-known examples of such a system in the engineering world is the metal to metal friction. This is a complex process that needs to be adequately identified by a constitutive relation in order to better facilitate the design components in severe contact stress applications. In this paper, the formulation of Molinari et al.’s work (J Tribology Trans ASME 35–41, 1999) is revisited in order to investigate the coefficient of dry friction for steel on steel in the high velocity range using physically based viscoplastic constitutive relations. First some of the errors in the work are corrected, and their results are regenerated. The phenomenological constitutive relation used in Molinari et al. (J Tribology Trans ASME 35–41, 1999) is then replaced by the physically based viscoplastic model used in this paper. This constitutive model is implemented into ABAQUS (Analysis User’s Manual, 2008) as user-defined subroutine as VUMAT in order to obtain the stress–strain curves at different strain rates and various temperatures. It is shown that the material responses obtained from the simulation using the physically based constitutive viscoplastic model agree well with the real behavior of the metals. Comparing this proposed work with that of Molinari et al. (J Tribology Trans ASME 35–41, 1999) one observes that the proposed theory and constitutive model are superior to the one presented by Molinari et al. This is specifically the case for the artificial shape of softening in the curve.

[1]  Meir Shillor,et al.  A dynamic thermoviscoelastic contact problem with friction and wear , 1997 .

[2]  A. Molinari,et al.  Analytical Characterization of Shear Localization in Thermoviscoplastic Materials , 1987 .

[3]  E. Bisson,et al.  Friction at high sliding velocities , 1947 .

[4]  J. C. Simo,et al.  On the Variational Foundations of Assumed Strain Methods , 1986 .

[5]  A. Klarbring A mathematical programming approach to three-dimensional contact problems with friction , 1986 .

[6]  Robert S. Montgomery,et al.  Surface Melting of Rotating Bands , 1976 .

[7]  G. Voyiadjis,et al.  Mechanics of strain gradient plasticity with particular reference to decomposition of the state variables into energetic and dissipative components , 2009 .

[8]  Michael Ortiz,et al.  An analysis of a new class of integration algorithms for elastoplastic constitutive relations , 1986 .

[9]  U. F. Kocks Realistic constitutive relations for metal plasticity , 2001 .

[10]  Geoffrey Ingram Taylor,et al.  The Latent Energy Remaining in a Metal after Cold Working , 1934 .

[11]  Alain Molinari,et al.  Dependence of the Coefficient of Friction on the Sliding Conditions in the High Velocity Range , 1999 .

[12]  D. Rigney,et al.  Plastic deformation and sliding friction of metals , 1979 .

[13]  F. P. Bowden,et al.  The Nature of Sliding and the Analysis of Friction , 1939 .

[14]  Anders Klarbring,et al.  A model of damage coupled to wear , 2003 .

[15]  X. J. Wang,et al.  Sliding behavior of Pb-Sn alloys , 1995 .

[16]  G. Voyiadjis,et al.  Theoretical and Experimental Characterization for the Inelastic Behavior of the Micro-/ Nanostructured Thin Films Using Strain Gradient Plasticity With Interface Energy , 2009 .

[17]  M. Ashby,et al.  Wear-mechanism maps , 1990 .

[18]  J. Duffy,et al.  On critical conditions for shear band formation at high strain rates , 1984 .

[19]  R. D. Krieg,et al.  Accuracies of Numerical Solution Methods for the Elastic-Perfectly Plastic Model , 1977 .

[20]  A. Klarbring Examples of non-uniqueness and non-existence of solutions to quasistatic contact problems with friction , 1990, Ingenieur-Archiv.

[21]  P. W. Christensen,et al.  Formulation and comparison of algorithms for frictional contact problems , 1998 .

[22]  G. Voyiadjis,et al.  Effect of dislocation density evolution on the thermomechanical response of metals with different crystal structures at low and high strain rates and temperatures , 2005 .

[23]  Walter Noll,et al.  The thermodynamics of elastic materials with heat conduction and viscosity , 1963 .

[24]  Anders Klarbring,et al.  Study of Frictional Impact Using a Nonsmooth Equations Solver , 2000 .

[25]  A. Molinari Shear Band Analysis , 1991 .

[26]  H. Blok Fundamental Mechanical Aspects of Boundary Lubrication , 1940 .

[27]  D. Rigney,et al.  An energy-based model of friction and its application to coated systems , 1981 .

[28]  M. Gurtin,et al.  Thermodynamics with Internal State Variables , 1967 .

[29]  George Z. Voyiadjis,et al.  Plastic deformation modeling of AL-6XN stainless steel at low and high strain rates and temperatures using a combination of bcc and fcc mechanisms of metals , 2005 .

[30]  J. T. Oden,et al.  Existence and uniqueness results for dynamic contact problems with nonlinear normal and friction interface laws , 1987 .

[31]  George Z. Voyiadjis,et al.  Nonlocal Gradient-Dependent Thermodynamics for Modeling Scale-Dependent Plasticity , 2007 .

[32]  Seh Chun Lim,et al.  Overview no. 55 Wear-Mechanism maps , 1987 .

[33]  George Z. Voyiadjis,et al.  Multiscale Analysis of Multiple Damage Mechanisms Coupled with Inelastic Behavior of Composite Materials , 2001 .

[34]  A. Bragov,et al.  Determining dynamic friction using a modified Kolsky method , 2008 .

[35]  George Z. Voyiadjis,et al.  Microstructural based models for bcc and fcc metals with temperature and strain rate dependency , 2005 .

[36]  M. Ashby,et al.  The effects of sliding conditions on the dry friction of metals , 1989 .

[37]  George Z. Voyiadjis,et al.  Modeling of strengthening and softening in inelastic nanocrystalline materials with reference to the triple junction and grain boundaries using strain gradient plasticity , 2010 .