Abstract

The paper investigates the variation of friction force (Fx) during reciprocating sliding tests on nanocrystalline diamond (NCD) films. The analysis of the friction behavior during the run-in period is the focus of the study. The NCD films were grown using microwave plasma-enhanced chemical vapor deposition (MW-PECVD) on single-crystalline diamond SCD(110) substrates. Reciprocating sliding tests were conducted under 500 and 2000 g of normal load using Si3N4 balls as a counter body. The friction force permanently varies during the test, namely Fx value can locally increase or decrease in each cycle of sliding. The distribution of friction force drops (dFx) was extracted from the experimental data using a specially developed program. The analysis revealed a power-law distribution f−µ of dFx for the early stage of the run-in with the exponent value (µ) in the range from 0.6 to 2.9. In addition, the frequency power spectrum of Fx time series follows power-law distribution f−α with α value in the range of 1.0–2.0, with the highest values (1.6–2.0) for the initial stage of the run-in. No power-law distribution of dFx was found for the later stage of the run-in and the steady-state periods of sliding with the exception for periods where a relatively extended decrease of coefficient of friction (COF) was observed. The asperity interlocking leads to the stick-slip like sliding at the early stage of the run-in. This tribological behavior can be related to the self-organized criticality (SOC). The emergence of dissipative structures at the later stages of the run-in, namely the formation of ripples, carbonaceous tribolayer, etc., can be associated with the self-organization (SO).

Highlights

  • Amonton’s law states that friction force is linearly related to the normal load: Fx = kFz (1)where Fx is friction force, k—coefficient of friction (COF) and Fz —normal load

  • The present study aims to investigate the distribution of the friction force drops obtained after sliding tests with Si3 N4 balls against nanocrystalline diamond (NCD) films grown on single-crystalline diamond SCD(110) substrates (NCD/SCD(110))

  • The distribution of friction force drops during reciprocating sliding on NCD/SCD(110) samples against Si3 N4 balls was analyzed

Read more

Summary

Introduction

Amonton’s law states that friction force is linearly related to the normal load: Fx = kFz (1). Where Fx is friction force, k—coefficient of friction (COF) and Fz —normal load. Friction is a complex phenomenon involving a number of processes, including deformation and fracture of surface asperities, adhesion, abrasion, chemical interactions, tribolayer formation, etc. Entropy 2019, 21, 1055 processes contribute to friction at different scales (nano-, micro- and macroscale) and hierarchy levels (molecular, surface asperity, component) [1]. The frictional systems are essentially not strictly linear, because the COF may depend on many factors including normal load. The energy (W) induced by external loading (mechanical work) is accumulated into the tribosystem (∆E) and converted into the heat (Q).

Methods
Discussion
Conclusion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.