2023
DOI: 10.1021/acs.langmuir.2c02925
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Effect of the Graphitization Mechanism on the Friction and Wear Behavior of DLC Films Based on Molecular Dynamics Simulations

Abstract: Whether a graphitization mechanism can control the low-friction behavior of DLC films is still controversial. In this paper, we establish the molecular dynamics model of the DLC film with graphene (DLC-GR-DLC) by LAMMPS and study the influence of the graphitization mechanism on the friction and wear behavior of the DLC film. The friction force of the DLC-GR-DLC model in the running-in stage is significantly smaller than that of the DLC film and then gradually increases to the same size as that of the DLC film.… Show more

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Cited by 21 publications
(13 citation statements)
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“…The P e is the minimum when the atomic spacing reaches equilibrium . The evolution of P e is helpful to determine when the system is in equilibrium to distinguish the friction state of the system . The left half of the P e curve has a significant decreasing trend (Figures S2j–l and S3j–l), indicating that the system is more compact with the decrease of the atomic spacing.…”
Section: Resultsmentioning
confidence: 99%
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“…The P e is the minimum when the atomic spacing reaches equilibrium . The evolution of P e is helpful to determine when the system is in equilibrium to distinguish the friction state of the system . The left half of the P e curve has a significant decreasing trend (Figures S2j–l and S3j–l), indicating that the system is more compact with the decrease of the atomic spacing.…”
Section: Resultsmentioning
confidence: 99%
“…41 The evolution of P e is helpful to determine when the system is in equilibrium to distinguish the friction state of the system. 42 The left half of the P e curve has a significant decreasing trend (Figures S2j−l and S3j−l), indicating that the system is more compact with the decrease of the atomic spacing. This corresponds to the sliding simulation gradually approaching the stable node (Figures S2a−f and S3a−f), which belongs to the pre-friction period.…”
Section: ■ Materials and Methodsmentioning
confidence: 94%
“…The friction force ( F f ) is obtained by summing the tangential forces of all of the Cr atoms in the upper rigid layer along the x direction. , Figure shows that the change of F f under different loadings and the water-lubricated friction of Cr and crystalline cellulose can be divided into three stages. In the beginning of sliding (stage I, S I ), F f and its fluctuation magnitude are quite high.…”
Section: Resultsmentioning
confidence: 99%
“…The friction generated by the relative sliding of Cr films and cellulose leads to a change of the temperature at contact interfaces, which varies at different loadings and sliding velocities, as shown in Figure . In this study, the temperature (Temp) is calculated by E k = 3 k B × Temp/2, where E k is the kinetic energy of atoms and is obtained by the mass and velocity of atoms and k B is the Boltzmann constant. , The temperature oscillates violently caused by high F f at the beginning and then rises to stabilize and fluctuate within a certain range. It is noticed that the temperature changes more drastically with increasing velocity at the beginning, with the largest value even higher than the stabilization.…”
Section: Resultsmentioning
confidence: 99%
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