Elsevier

Wear

Volume 262, Issues 11–12, 10 May 2007, Pages 1516-1521
Wear

Short communication
A modelling technique for predicting compound impact wear

https://doi.org/10.1016/j.wear.2007.01.032Get rights and content

Abstract

Wear problems are consistently arising as a result of the introduction of new or alternative materials to situations where components are impacting.

Impact wear has generally not been studied as extensively as other wear mechanisms and as a result information on the causes and actual impact wear data is quite scarce. There are also few impact modelling techniques and those that exist have not been extensively applied.

In this work, a new modelling technique for predicting compound impact wear was developed. This was found to give improvements when compared with existing models in terms of both usability and accuracy of results.

Introduction

Impact or percussive wear has been defined as: “the wear of a solid surface that is due to percussion, which is a repetitive exposure to dynamic contact by another body” [1].

Two modes of impact wear are apparent (as shown in Fig. 1). Normal impact wear occurs when the relative approach of the impacting bodies contains no tangential or rotational elements. Where a shear component is added, either when normal impact occurs with a component of sliding or the bodies impact at a tangent, the term compound impact wear is used. Most impact situations actually involve impact with a small amount of sliding. Compound impact wear has been shown to lead to much higher wear rates than normal impact alone [2], [3]. This is thought to be due to enhanced removal of wear debris that occurs with the introduction of a shear component.

There are many industrial situations in which impacting bodies are employed where failures due to wear can be costly and safety, reliability and quality reduced greatly. Excessive wear of impacting poppet valves in automotive engines can lead to loss of cylinder pressure and ultimately engine failure. Failure of tools used for drilling rock and other media raise cost concerns, not only associated with the need for frequent replacement of parts, but also in the down time incurred [4]. Impact wear of printer typefaces will lead to loss of definition and a subsequent reduction in print quality [5]. Unintentional impacts, such as the chattering of tubes carrying, for example, waste from nuclear reactors, can give rise to situations where safety and reliability are of critical concern [6]. Potential impact wear problems are also being found in dental implants and heart valves, where health and well-being are at stake.

Problems due to impact wear are starting to arise more when new or alternative materials are introduced in situations where components are impacting, usually in order to reduce costs or for environmental reasons. An example of this is the increasing use of sintered materials, ceramics and plastics in the production of automotive engines (see for example, [7]). These are being introduced to ease manufacture by increasing machinability or to reduce weight, etc. However, all have raised impact wear issues not previously apparent.

Impact wear generally has not been studied as extensively as other wear mechanisms and information on the causes and actual impact wear data is hard to find. There are also few dedicated impact wear modelling techniques and those that exist have not been extensively applied. In this work, extant impact wear models were assessed. A new improved modelling technique was then developed to predict compound impact wear, which was compared with experimental data to provide validation and with existing models to assess its relative performance.

Section snippets

Extant impact wear models

A compound impact wear modelling approach has been established based on two assumed stages of wear progression [8]. The first is an induction period (see Fig. 2), during which deformation occurs and a wear scar is formed, but there is no measurable material loss. The end of this stage is defined as the zero wear limit. This constitutes the initial point of the measurable wear region. As indicated in Fig. 2, the progression of wear in this region can take on a number of forms. These will depend

Model structure

There is a clear a need for an easy to apply model for predicting compound impact wear that is able to cope with any contact geometry. Such a model will now be outlined. It is simply comprised of two wear models; one for predicting impact wear and one for sliding wear.

A relationship of the same form as that used in erosion studies to model wear mass, W [8] (based on impact energy) (Eq. (4)), is used to model impact wear.

The equation for impact wear is combined with an equation for sliding wear

Conclusions

  • A technique for predicting compound impact wear rates (that involving impact and sliding) has been developed. Although requiring a number of empirical wear factors it is easy to use and can quickly give an idea of a likely wear rate given a contact geometry and a set of operating parameters.

  • The technique has been compared to existing experimental data and predictions using extant wear models. Good correlation exists with the experimental data, except at low numbers of cycles where plastic

Cited by (35)

  • A new predictive model for normal and compound impact wear

    2021, Wear
    Citation Excerpt :

    It is important to note that material hardness has not been directly and explicitly considered as a parameter controlling the wear loss of materials under repetitive normal impact. It is often indirectly included, as part of experimentally derived coefficients and constants, from line fitting [20] or in the case of Rabinowicz [17] discounted because in that experimental work stainless steel experienced more wear than the aluminium alloys tested, despite stainless steel having higher hardness than aluminium. Similar results were obtained by Fricke [19], who found that in a high carbon martensitic stainless steel (AISI 440C) with hardness of 710Hv there was more mass loss than in both austenitic stainless steel (AISI 304) (242Hv) and a high chromium martensitic stainless steel (AISI 431) (465Hv), leading to the same conclusion that hardness is not a primary parameter controlling the results of repetitive normal impact.

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