Search arXiv⌕ Search

arXiv · 2503.22307

Analytical Model of the Evolution of Surface Topography During Sliding Wear

Abstract

During the wear process of surfaces in sliding friction, there is a running-in period during which the topography of surfaces changes with time before reaching the steady wear regime. In the steady wear regime, the statistical parameters used to describe the topography of the surfaces remain almost constant. Some experimental studies have shown that starting friction tests with different surface finish levels leads to the same final topography of surfaces in the regime of steady wear. This article proposes an analytical model to describe the evolution of the topography of surfaces during sliding wear. First of all, the Greenwood and Williamson approach is used to describe the contact between nominally flat rough surfaces. The asperities in contact may undergo plastic deformation or adhesion with the opposing surface. Using a plasticity criterion and an adhesion criterion, it is possible to obtain a differential equation for the evolution of the standard deviation of the asperities of the surfaces. This equation has an analytical solution that is in good agreement with experimental results from the literature. It is shown that the final surface topography is the result of the competition between abrasive wear and adhesive wear. The model is then used to describe different wear processes from polishing to galling.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Noël Brunetière. 2025-03-28. Analytical Model of the Evolution of Surface Topography During Sliding Wear. https://doi.org/10.1115/1.4068176

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

3D modelling of strain concentration due to PCI within the fuel code ALCYONE

In this paper, the 3D scheme of the fuel code ALCYONE is applied to a database consisting of more than 50 base irradiations and ramp tests performed on rods with UO 2 , MOX or Cr-doped UO 2 fuels and Zy4 or M5__ cladding tubes with burn-ups up to 70 GWd/tU. The ability of the 3D scheme to predict the behaviour of a single fuel pellet -cladding element situated at the maximum Linear Heat Rate (LHR) during ramp testing is demonstrated by comparing the following experimental and calculated data: residual clad diameter after base irradiation and ramp test, height of inter-pellet and mid-pellet ridges after base irradiation and ramp test, dish filling after ramp test. In the second part of the paper, 3D simulations that catch the stress -strain localization at the triple point are presented. It is shown that the stress-strain concentration occurs only at the end of the power transient and is quickly relaxed by pellet and clad creep.

physics.class-ph↗

Repeated Binary Direct Collinear Impacts Under Incremental Contact Laws With Permanent Indentation: A Hybrid Systems Formulation

Incremental contact laws specify the normal contact force through a differential equation carrying an internal state, driven by the indentation and its rate. In some, the force is extinguished at a nonzero indentation, whether by plastic deformation or by an elastic aftereffect, so that a residual deformation remains at the separation. Such laws sit uneasily within rigid body dynamics, which admits no deformation. The tension is tolerable when the indentation is small relative to the bodies, so that it may be carried constitutively rather than geometrically. Even then, the contact law alone does not determine the interaction of the bodies. Because force and indentation no longer vanish together, conditions for the commencement and termination of contact must be supplied separately. So must the fate of the deformation and internal state at separation, neither of which the equations of motion contain. This article formulates the repeated direct collinear impact of two convex bodies under external forces as a hybrid dynamical system. The contact interface is modeled as a massless element carrying the contact law and its state, coupled to the bodies through relative velocity and an interaction force dictated by the contact state. Consequently, all switching and resets are confined to the interface, leaving the geometry and the equations of motion of the bodies unaltered. The principal analytical properties of the resulting formulations are established, among them passivity and completeness; the branching of solutions at the onset and termination of contact is also examined. The framework is demonstrated through numerical simulations.

physics.class-ph↗

Characterizing the Carnot cycle at absolute zero: a reply to "Comment on `Proof of the Nernst theorem' "

This reply addresses a recent comment concerning the proof of the Nernst theorem. I clarify how a Carnot engine can consistently operate at $T=0$ through a continuous deformation of a cycle operating at $T>0$. By examining the limit where heat exchange with the cold reservoir vanishes, I show that the Nernst theorem ensures that the concept of temperature remains physically consistent at the absolute zero limit.

physics.class-ph↗