Elsevier

Wear

Volume 308, Issues 1–2, 30 November 2013, Pages 186-192
Wear

Wear equation for adhesive wear established through elementary process of wear

https://doi.org/10.1016/j.wear.2013.06.016Get rights and content

Highlights

  • Wear process was observed from the origin of wear elements for adhesive wear.

  • Generation of wear elements was discussed from slip systems at sliding surface in the elementary wear process.

  • Wear model of adhesive wear from the generation of wear elements to wear particles was presented.

  • Wear equation for adhesive wear was proposed.

Abstract

The research covers the wear processes of adhesive wear from the origin of wear elements (the unitary debris of wear) with a size from a few nanometers to a few tens of nanometers to form transfer particles and lastly wear particles. These particles and wear phenomenon were observed by means of atomic force microscopy (AFM). Furthermore, the formation process of wear particles between the sliding surfaces was optically observed by means of an in situ observation system. From the results of observation of the wear process, we propose a basic wear model of the adhesive wear mechanism and present a wear equation for adhesive wear including physical properties of the sliding surfaces as well as the chemical effect of surrounding gas molecules to the surfaces.

Introduction

Investigation into the mechanism of adhesive wear was undoubtedly triggered by the concept of real contact area (i.e. junction) introduced by Holm [1], [2]. Wear is occurred at the junction fractured by the shear force in frictional motion through the removal of debris of wear. Holm attributed the wear to the removal of atomic level particles or layers at the junction, and afterwards Rabinowicz [3] and Archard [4] proposed that the mechanism for the formation of wear particles stemmed from the removal of the junction itself after fracture of the junction. However, the observation revealed that the size of wear particles was not neither atomic level nor junction itself, but it depended on the mode of adhesive wear after the formation process of transfer and further processes [5], [6]. Of course, severe wear has a particle size from a few tens to a few hundreds μm, while mild wear has a size less than a few μm. Their wear models for adhesive wear and their equations for adhesive wear could not explain the difference in the two modes of adhesive wear. Furthermore, it was most uncertain in their proposed wear equations that both of the wear equations included the factor of probability of removal of wear debris from the junction described as a wear coefficient. However, we suppose the removal of wear debris is not decided by probability but it is absolutely decided by the physical, chemical and mechanical properties of the substances in the tribological processes. The further progressive precise wear equation including the physical and chemical properties of the surfaces for adhesive wear has not proposed after their equations. Therefore, at present we have no wear equations for adhesive wear to explain physical and chemical properties in the wear mechanism.

We recently reported adhesive wear process from the origin of elemental debris of wear particles, which we refer to as “wear elements”; with the size ranges from a few nanometers to a few tens of nanometers observed by means of atomic force microscopy (AFM) to explain elementary process of adhesive wear process [7], [8], [9]. The aim of this investigation is to clarify the progressive process from the origin of wear elements to the formation of wear particles that subsequently disengage from the sliding surfaces as examined by AFM and in situ optical imaging. Furthermore, we propose a basic wear model and present an equation for adhesive wear including the physical and chemical properties in tribological processes according to the characteristics from the origin of elemental debris to the formation process of wear particles on the sliding surfaces.

Section snippets

Experimental

Friction and wear experiments were performed using a pin−on−disk tribotester. The disk specimen (diameter 40 mm) was rotated at a sliding speed of 1.0 mm/s. The pin specimen (diameter 5 mm) was subjected to a normal load of 5.0 N and the sliding surface of the pin was hemispherical in shape. The wear track of the pin specimen on the disk surface was set at 22 mm in diameter. All experiments were performed under dry conditions in air at room temperature and ambient relative humidity (about 40%). At

Observation of pre-sliding surface and the first contact

Fig. 1(a) shows the pre-sliding surface after the steel pin came into contact with the steel disk and tangential force was applied under a load of 5.0 N. At this stage, the pin did not slide on the disk surface in macro scale. Then, the surfaces were separated and the disk surface was observed by AFM. The circle with a diameter of about 30 μm drawn with a broken line on the surface image is the Hertz contact area determined by calculating the ball-flat contact. We can see the real contact area in

Conclusion

In this investigation, we examined the adhesive wear process by means of AFM and in situ optical imaging. The wear process was clarified as originating from wear elements of a few nanometers to a few tens of nanometers in size, which accumulated and formed wear particles. From the observations, we proposed a model for adhesive wear from the origin of wear elements to the formation of wear particles, and we presented an equation for adhesive wear V=(1/3)×(nλ)×(ba)3×(P×ℓpm) considering the

Acknowledgements

This research was supported by the Ministry of Education, Culture, Sports, Science and Technology of Japan [Grant-in-Aid for Scientific Research (B), 22360066, 2010].

References (18)

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    Here, assuming that n corresponds to the number of wear elements present in the area of πa2, n is expressed by n ≈ πa2nunit. As previously described, the wear element is the unitary debris of an adhesive wear particle, and the size of wear element was ranging from a few nanometers to a few tens of nanometers by AFM observation [3–6,8]. With respect to the size of the wear elements, it has previously been discussed this is comparable to the size of single-magnetic-domain particles when the metal is a ferromagnetic metal (Ni, Fe, or Co) [5,6].

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