Journal Home > Volume 1 , Issue 1

Computer simulations have been an integral part of the technical development process for a long time now. Industrial tribology is one of the last fields in which computer simulations have, until now, played no significant role. This is primarily due to the fact that investigating tribological phenomena requires considering all spatial scales from the macroscopic shape of the contact system down to the micro-scales. In the present paper, we give an overview of the previous work on the so-called method of reduction of dimensionality (MRD), which in our opinion, gives a key for the linking of the micro- and macro-scales in tribological simulations.

MRD in contact mechanics is based on the mapping of some classes of three-dimensional contact problems onto one-dimensional contacts with elastic foundations. The equivalence of three-dimensional systems to those of one-dimension is valid for relations of the indentation depth and the contact force and in some cases for the contact area. For arbitrary bodies of revolution, MRD is exact and provides a sort of “pocket edition” of contact mechanics, giving the possibility of deriving any result of classical contact mechanics with or without adhesion in a very simple way.

A tangential contact problem with and without creep can also be mapped exactly to a one-dimensional system. It can be shown that the reduction method is applicable to contacts of linear visco-elastic bodies as well as to thermal effects in contacts. The method was further validated for randomly rough self-affine surfaces through comparison with direct 3D simulations.

MRD means a huge reduction of computational time for the simulation of contact and friction between rough surfaces accounting for complicated rheology and adhesion. In MRD, not only is the dimension of the space reduced from three to one, but the resulting degrees of freedom are independent (like normal modes in the theory of oscillations). Because of this independence, the method is predestinated for parallel calculation on graphic cards, which brings further acceleration. The method opens completely new possibilities in combining microscopic contact mechanics with the simulation of macroscopic system dynamics without determining the “law of friction” as an intermediate step.


menu
Abstract
Full text
Outline
About this article

Method of reduction of dimensionality in contact and friction mechanics: A linkage between micro and macro scales

Show Author's information Valentin L. POPOV*( )
Berlin University of Technology, Berlin 10623, Germany

Abstract

Computer simulations have been an integral part of the technical development process for a long time now. Industrial tribology is one of the last fields in which computer simulations have, until now, played no significant role. This is primarily due to the fact that investigating tribological phenomena requires considering all spatial scales from the macroscopic shape of the contact system down to the micro-scales. In the present paper, we give an overview of the previous work on the so-called method of reduction of dimensionality (MRD), which in our opinion, gives a key for the linking of the micro- and macro-scales in tribological simulations.

MRD in contact mechanics is based on the mapping of some classes of three-dimensional contact problems onto one-dimensional contacts with elastic foundations. The equivalence of three-dimensional systems to those of one-dimension is valid for relations of the indentation depth and the contact force and in some cases for the contact area. For arbitrary bodies of revolution, MRD is exact and provides a sort of “pocket edition” of contact mechanics, giving the possibility of deriving any result of classical contact mechanics with or without adhesion in a very simple way.

A tangential contact problem with and without creep can also be mapped exactly to a one-dimensional system. It can be shown that the reduction method is applicable to contacts of linear visco-elastic bodies as well as to thermal effects in contacts. The method was further validated for randomly rough self-affine surfaces through comparison with direct 3D simulations.

MRD means a huge reduction of computational time for the simulation of contact and friction between rough surfaces accounting for complicated rheology and adhesion. In MRD, not only is the dimension of the space reduced from three to one, but the resulting degrees of freedom are independent (like normal modes in the theory of oscillations). Because of this independence, the method is predestinated for parallel calculation on graphic cards, which brings further acceleration. The method opens completely new possibilities in combining microscopic contact mechanics with the simulation of macroscopic system dynamics without determining the “law of friction” as an intermediate step.

Keywords: elastomers, contact mechanics, adhesion, sliding friction, static friction, rough surfaces, rolling, dynamic tangential contacts, reduction of dimensionality, scale linkage

References(60)

[1]
Bowden F P, Tabor D. The Friction and Lubrication of Solids. Oxford: Clarendon Press, 1986.
[2]
Archard J F. Elastic deformation and the laws of friction. Proc R Soc A 243:190-205 (1957)
[3]
Archard J F. Contact and rubbing of flat surfaces. J of Appl Phys 24:981-988 (1953)
[4]
Persson B N J. Contact mechanics for randomly rough surfaces. Surf Sci Rep 61:201-227 (2006)
[5]
Popov V L. Contact Mechanics and Friction: Physical Principles and Applications. Berlin: Springer-Verlag, 2010.
DOI
[6]
German-Russian Workshop on "Numerical simulation method in tribology: possibilities and limitations", TU Berlin, March 14–17, 2005. Contributions published in the special issue of "Tribology International", (Trib Int, 40, No. 6, Guest editors Popov V and Ostermeyer G-P).
[7]
Popov V L, Psakhie S G. Numerical simulation methods in tribology. Tribology International 40:916-923 (2007)
[8]
Barber J R. Bounds on the electrical resistance between contacting elastic rough bodies. Proc R Soc Lond A 495:53-66 (2003)
[9]
Geike T, Popov V L. Mapping of three-dimensional contact problems into one dimension. Phys Rev E 76:036710 (2007)
[10]
Geike T, Popov V L. Reduction of three-dimensional contact problems to one-dimensional ones. Tribology International 40:924-929 (2007)
[11]
Kürschner S, Filippov A E. Normal contact between a rigid surface and a viscous body: Verification of the method of reduction of dimensionality for viscous media. Phys Mesomech 15:270-274 (2012)
[12]
Popov V L, Filippov A E. Force of friction between fractal rough surface and elastomer. Tech Phys Lett 36:525-527 (2010)
[13]
Popov V L, Dimaki A. Using hierarchical memory to calculate friction force between fractal rough solid surface and elastomer with arbitrary linear rheological properties. Tech Phys Lett 37:8-11 (2011)
[14]
Benad J. On the dependence of the static friction force between a rigid, randomly rough fractal surface and a viscoelastic body on the normal force. Phys Mesomech 15:300-302 (2012)
[15]
Li Q. Dependence of the kinetic force of friction between a randomly rough surface and simple elastomer on the normal force. Phys Mesomech 15:303-305 (2012)
[16]
Heise R. Multiscale simulation of friction with normal oscillations in the method of reduction of dimensionality. Phys Mesomech 15:316-318 (2012)
[17]
Teidelt E, Willert E, Filippov A E, Popov V L. Modeling of the dynamic contact in stick-slip microdrives using the method of reduction of dimensionality. Phys Mesomech 15:287-292 (2012)
[18]
Stracevic J, Filippov A E. Simulation of the influence of ultrasonic in-plane oscillations on dry friction accounting for stick and creep. Phys Mesomech 15:330-332 (2012)
[19]
Wetter R. Shakedown and induced microslip of an oscillating frictional contact. Phys Mesomech 15:293-299 (2012)
[20]
Popov M. Contact force resulting from rolling on a self- affine fractal rough surface. Phys Mesomech 15:342-344 (2012)
[21]
Heß M. Über die Abbildung ausgewählter dreidimensionaler Kontakte auf Systeme mit niedrigerer räumlicher Dimension. Göttingen: Cuvillier-Verlag, 2011.
[22]
Heß M. On the reduction method of dimensionality: The exact mapping of axisymmetric contact problems with and without adhesion. Phys Mesomech 15:264-269 (2012)
[23]
Johnson K L. Contact Mechanics. Cambridge: Cambridge University Press, 1987.
[24]
Sneddon I N. The relation between load and penetration in the axisymmetric boussinesq problem for a punch of arbitraryprofile. Int J Eng Sci 3:47-57 (1965)
[25]
Ejike U B C O. The stress on an elastic half-space due to sectionally smooth-ended punch. Journal of Elasticity 11:395-402 (1981)
[26]
Griffith A A. The phenomena of rupture and flow in solids. Phil Trans R Soc Lond A 221:163-198 (1921)
[27]
Johnson K L, Kendall K, Roberts A D. Surface energy and the contact of elastic solids. Proc R Soc A 324:301-313 (1971)
[28]
Popov V L. Kontaktmechanik und Reibung: Von der Nanotribologie bis zur Erdbebendynamik. Berlin: Springer, 2010.
DOI
[29]
Prandtl L. Ein Gedankenmodell für den Zerreißvorgang spröder Körper. ZAMM 13:129-133 (1933)
[30]
Maugis D. Contact, Adhesion, and Rupture of Elastic Solids. Berlin: Springer Verlag, 2000.
DOI
[31]
Popov V L. Basic ideas and applications of the method of reduction of dimensionality in contact mechanics. Physical Mesomechanics 15:254-263 (2012)
[32]
Popov V L, Filippov A E. Adhesive properties of contacts between elastic bodies with randomly rough self-affine surfaces: A simulation with the method of reduction of dimensionality. Phys Mesomech 15:324-329 (2012)
[33]
Cattaneo C. Sul contatto di due corpi elastici: distribuzione locale degli sforzi. Rendiconti dell'Accademia nazionale dei Lincei 27:342-348, 434-436, 474-478 (1938)
[34]
Mindlin R D. Compliance of elastic bodies in contact. Journal of Applied Mechanics 16:259-268 (1949)
[35]
Jäger J. Axi-symmetric bodies of equal material in contact under torsion or shift. Archive of Applied Mechanics 65:478-487 (1995)
[36]
Mindlin R D, Mason W P, Osmer J F, Deresiewicz H. Effects of an oscillation tangential force on the contact surfaces of elastic spheres. Pros.1st US National Congress of Applied Mechanics: 203–226 (1952)
[37]
Landau L D, Lifschitz E M. Lehrbuch der Theoretischen Physik, Band 7: Elastizitätstheorie. Berlin: Akademie-Verlag, 1965.
[38]
Landau L D, Lifschitz E M. Lehrbuch der Theoretischen Physik, Band 6: Hydrodynamik. Berlin: Akademie-Verlag, 1991.
[39]
Radok J R M. Viscoelastic stress analysis. Q Appl Math 15:198-202 (1957)
[40]
Greenwood J A, Williamson J B P. Contact of nominally flat surfaces. Proc R Soc A 295:300-319 (1966)
[41]
Hyun S, Robbins M O. Elastic contact between rough surfaces: Effect of roughness at large and small wavelengths. Tribol Intern 40:1413-1422 (2007)
[42]
Campana C, Müser M H. Practical Green's function approach to the simulation of elastic semi-infinite solids. Phys Rev B 74:075420 (2006)
[43]
Akarapu S, Sharp T, Robbins M O. Stiffness of contacts between rough surfaces. Phys Rev Lett 106:204301 (2011)
[44]
Campana C, Persson B N J., Müser M H. Transverse and normal interfacial stiffness of solids with randomly rough surfaces. J Phys: Condens Matter 23:085001 (2011)
[45]
Pohrt R, Popov V L. Normal contact stiffness of elastic solids with fractal rough surfaces. Phys Rev Lett 108:104301 (2012)
[46]
Pohrt R, Popov V L, Filippov A E. Normal contact stiffness of elastic solids with fractal rough surfaces for one- and three-dimensional systems. Phys Rev E 86:026710 (2012)
[47]
Pohrt R, Popov V L. Contact mechanics of randomly rough self-affine surfaces. Tribology International, 2013, in press.
[48]
Popov V L, Heß M. Methode der Dimensionsreduktion in der Kontaktmechanik und Reibung. Berlin: Springer, 2013.
DOI
[49]
Pohrt R. Private communication.
DOI
[50]
Heise R, Popov V L. Adhesive contribution to the coefficient of friction between rough surfaces. Tribology Letters 39:247-250 (2010)
[51]
Grosch K A. The relation between the friction and viscoelastic properties of rubber. Proc R Soc Lond A 274:21-39 (1963)
[52]
Ben-David O, Fineberg J. Static friction coefficient is not a material constant. Phys Rev Lett 106:254301 (2011)
[53]
Adams G G, Nosonovsky M. Contact modeling – forces. Tribology International 33:431-442 (2000)
[54]
Psakhie S G, Popov V L. Mesoscopic nature of friction and numerical simulation methods in tribology. Physical Mesomechanics 15:251-253 (2012)
[55]
Filippov A E, Popov V L. Fractal Tomlinson model for mesoscopic friction: From microscopic velocity-dependent damping to macroscopic Coulomb friction. Physical Review E 75:027103 (2007)
[56]
Prandtl L. Ein Gedankenmodell zur kinetischen Theorie der festen Körper. ZAMM 8:85-106 (1928). English translation: Popov V L, Gray J A T. Prandtl-Tomlinson model: History and applications in friction, plasticity, and nanotechnologies. ZAMM 92: 683–708 (2012)
[57]
Popov V L. A theory of the transition from static to kinetic friction in boundary lubrication layers. Solid State Commun 115:369-373 (2000)
[58]
Meyer E, Overney R M, Dransfeld K, Gyalog T. Nanoscience: Friction and Rheology on the Nanometer Scale. Singapore: World Scientific, 1998.
DOI
[59]
Geike T. Theoretische Grundlagen eines schnellen Berechnungsverfahrens für den Kontakt rauer Oberflächen. Ph.D thesis. Berlin: Berlin University of Technology, 2008.
[60]
Scaraggi M, Putignano C, Carbone G. Elastic contact of rough surfaces: A simple criterion to make 2D isotropic roughness equivalent to 1D one. Wear 297:811-817 (2013)
Publication history
Copyright
Acknowledgements
Rights and permissions

Publication history

Received: 27 October 2012
Revised: 31 January 2013
Accepted: 18 February 2013
Published: 26 March 2013
Issue date: March 2013

Copyright

© The author(s) 2013

Acknowledgements

I am grateful to my colleagues and guests at the Berlin University of Technology J. Benad, A. Dimaki, A.E. Filippov, T. Geike, R. Heise, M. Heß, S. Kürschner, Q. Li, R. Pohrt, M. Popov, S. G. Psakhie, J. Starcevic, E. Teidelt, R. Wetter, E. Willert for many valuable discussions of the fundamentals of the method of reduction of dimensionality and its extensions. I thank R. Pohrt for providing not yet published results and permission to use them in this review. I acknowledge the useful critical remarks by B. N. J. Persson and M. Müser, which contributed to the understanding of the region of applicability of the method. I acknowledge financial support of this research by the Deutsche Forschungsgemeinschaft (DFG) and the Deutscher Akademischer Austausch Dienst (DAAD) in the framework of several projects.

Rights and permissions

This article is published with open access at Springerlink.com

Open Access: This article is distributed under the terms of the Creative Commons Attribution Noncommercial License which permits any noncommercial use, distri- bution, and reproduction in any medium, provided the original author(s) and source are credited.

Return