Elsevier

Tribology International

Volume 38, Issues 11–12, November 2005–December 2006, Pages 931-942
Tribology International

In situ analysis of the fragmentation of polystyrene films within sliding contacts

https://doi.org/10.1016/j.triboint.2005.07.018Get rights and content

Abstract

Fracture processes of thin (10–100 μm) polystyrene films on PMMA substrates have been investigated within macroscopic single-asperity sliding contacts with rigid spheres. Using the resources of in situ contact visualization, the development of cracks has been analyzed under both elastic and plastic conditions for various values of the ratio of the contact radius to the film thickness. Under elastic contact conditions, damage mechanisms were dominated by the formation of a network of regularly spaced cracks at the leading edge of the contact. These processes were analyzed in the light of a fragmentation model based on contact mechanics simulations of the stress field induced within the cracked films. It emerged from this contact mechanics analysis that the mean spacing between adjacent cracks can be correlated to the strength of the polymer coating.

Introduction

Polymeric coatings are largely used to improve contact mechanical and tribological performance of engineering materials and optical components. However, the development and selection of such films is a very complex and costly task. The number of parameters is huge, spanning from material, physical, mechanical and surface properties to the behaviour of complex films/substrate systems. In addition, there is a lack of data and understanding regarding the actual deformation and fracture mechanisms involved in such coatings.

Within this context, abrasion resistance remains one of the key issues regarding the lifetime of organic coatings. During abrasive wear damage, the initial stage is usually considered to be the process of contact and scratch between the polymer surface and a sharp asperity. The accumulation of the associated microscopic failure events eventually generates wear particles and gives rise to weight loss. Investigating such processes within macroscopic contacts between rough surfaces is, however, a difficult task due to the multiple interactions between individual sliding micro-asperities. In order to overcome these limitations, model experiments are often considered which attempt to simulate the damage induced by a single asperity contact [1]. Although the wear rate itself is not monitored, such experiments provide the opportunity of getting a more detailed insight into the deformation and fracture mechanisms involved in asperity engagements. In such experiments, the selection of different indentor geometries and loading conditions offers the possibility of exploring the viscoelastic/viscoplastic response and brittle failure mechanisms over a wide range of strains and strain rates. For bulk polymers, the observed damage evolves through a range of severity as the contact strain is increased: visco-elastic smoothing or ‘ironing’, plastic or viscoplastic grooving, extensive plastic flow and tearing, pronounced fracture or tearing and finally cutting or chip formation can be identified [2], [3], [4], [5], [6], [7], [8]. These approaches have been popularized for a variety of amorphous and glassy and semi-crystalline polymers by Briscoe and co-workers [9], [10] who put together in the form of ‘deformation maps’ the different deformation regimes.

Similar regimes can be identified in the case of polymeric coatings. Within the fracture domain, regular crack patterns are often observed at the leading edge of the contact under the action of predominantly tensile stresses [7], [8], [11], [12]. A critical normal force is often ascribed to the occurrence of such cracking processes, but the way it relates to known polymer failure properties such as fracture toughness is still a matter of debate [6]. In addition, the contribution of substrate deformation to the development of contact cracks within thin polymer films remains largely unknown. As a first approach, the magnitude of these effects may be assumed to depend largely on the ratio of the contact area, a, to the film thickness, h. In many contact situations, this a/h ratio can vary by orders of magnitude depending on whether the macroscopic or micro-asperity contact lengths are considered. There is therefore a need for a better understanding of coating fracture processes as a function of this characteristic a/h ratio.

Within the frame of this investigation, fracture mechanisms of thin (10–100 μm) polystyrene (PS) films on polymethacrylate (PMMA) substrates have been investigated within macroscopic sliding contacts with smooth spherical asperities. Using the resources of in situ contact visualization, the various stages of the development of crack networks within the PS film have been observed for a range of contact conditions which were characterized by different ratios of the contact radius, a, to the film thickness, h. The resulting crack patterns have been analyzed in the light of a fragmentation model which considers that failure is driven by the evolving tensile stress field induced within the cracked PS film at the leading edge of the contact. For that purpose, a contact mechanics analysis of the cracked coated systems has been developed which is able to simulate the film unloading/reloading processes associated with the propagation of successive cracks during sliding.

Section snippets

Elaboration of the film systems

The polymer systems investigated in this study consisted in a poly(methylmethacrylate) (PMMA) substrate coated with poly(styrene) (PS) films 10–100 μm in thickness. In order to promote an optimum stress transfer between the two polymer layers, a thin (about 40 nm) layer of a PS-b-PMMA block copolymer was inserted at the PS/PMMA interface during the processing of the specimens. Mode I fracture tests carried out by Brown et al. [13] indicated that such di-block polymers can dramatically improve the

In situ analysis of film cracking processes

The contact deformation behaviour and damage modes were at first investigated for moderate a/h ratios using the ‘microvisioscratch’ device. In order to vary the average contact strain, a/R, from elastic to plastic conditions, the normal load was incrementally increased during the lateral displacement of the tip. For each normal load step, in situ observations allowed to identify the nature of the contact loading from an analysis of the actual shape of the contact area. A typical example of the

Contact mechanics analysis of the fragmentation processes

The above detailed cracking mechanisms present close similarities with the fragmentation processes which are observed in many heterogeneous systems such as fibre reinforced composites [31], [32] paints or coatings [33], [34], where a brittle phase is intimately associated with a more ductile phase and loaded under tensile conditions. Independently on the system geometry, a saturation of the mean distance between adjacent cracks is often observed when the applied strain is increased. The value

Conclusions

The cracking processes of brittle polystyrene coatings on Polymethylmethacrylate substrates have been investigated within sliding contacts with rigid counterfaces under both elastic and viscoplastic contact conditions. For large contact strains (i.e. a/R>0.2), cracks convex to the wake of the indenter were nucleated at the front edge of the contact, in regions where a significant viscoplastic pile-up was observed. Under elastic and viscoelastic contact conditions (i.e. a/R<0.1), the damage of

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