Abstract:We use molecular dynamics (MD) simulations to characterize the tensile strength of contacts formed between various clean platinum surfaces with nanoscale asperities. Both commensurate contacts between (001) and (111) Commensurate contacts lead to stronger bridges than incommensurate ones but only during the initial closing events, after steady state is achieved commensurate and incommensurate (001) surfaces lead to bridges of similar strengths.
“…This leads to a decrease in hardness with decreasing contact length since dislocations are localized within the high-stress, thin contact regions. 16,17 The atomic mechanisms that govern size effects in asperity/asperity and flat/asperity are similar. However, the dislocation structures generated show some differences.…”
Section: Atomic Mechanisms Of Size Effects In Contact Hardnessmentioning
confidence: 94%
“…The transition from hardening to softening is reminiscent of the Hall-Petch maximum in nanocrystalline or nanolaminate materials [13][14][15] but is governed by very different mechanisms. The hardness of these nanoscale contacts is between 50% and 70% larger than their corresponding tensile strength, 16,17 and their size effects exhibit similarities and interesting differences.…”
Section: Introductionmentioning
confidence: 90%
“…This external force (F ext ) is applied to all atoms within a thin slab (4.5 nm thick) at the free surfaces away for the contacting ones. 16,17 As described in Sec. II C, this closing force increases in a stepwise manner to characterize the elastic loading and plasticity in the contacting regions.…”
Section: B Contact Simulations and Hardnessmentioning
confidence: 99%
“…As is commonly done in atomistic simulations of fcc metals, 16,17 we identify dislocation activity by tracking atoms with hexagonal close packed local environments. Two consecutive planes of hcp atoms form the stacking fault ribbons that separate partial dislocations in fcc metals.…”
Section: Identification Of Atoms Responsible For Plastic Deformationmentioning
confidence: 99%
“…19 This potential was parameterized to reproduce the equilibrium lattice constant, sublimation energy, elastic contacts, and vacancy formation energy of Pt from experimental data and was used to study the strength of contacting bridges between rough surfaces, leading to predictions in good agreement with experiments. 16,17 Each simulation involves two 20-nm-thick Pt slabs with either a flat surface or a sinusoidal surface given by…”
Section: A Molecular Dynamics and Initial Structuresmentioning
We characterize how size and shape affects the hardness of nanoscale metallic contacts using large-scale molecular dynamics (MD) simulations. High-aspect-ratio contacts continue the experimentally observed trend of hardening with decreasing contact size down to the sub-10-nm regime. However, we find that this effect is shape dependent and the rate of hardening with decreasing contact size diminishes as the aspect ratio of the asperities becomes smaller. Interestingly, low-aspect-ratio asperities that can support simple dislocation glide exhibit softening with decreasing size. A detailed analysis of the MD trajectories reveals the dislocation mechanisms that govern these complex size effects.
“…This leads to a decrease in hardness with decreasing contact length since dislocations are localized within the high-stress, thin contact regions. 16,17 The atomic mechanisms that govern size effects in asperity/asperity and flat/asperity are similar. However, the dislocation structures generated show some differences.…”
Section: Atomic Mechanisms Of Size Effects In Contact Hardnessmentioning
confidence: 94%
“…The transition from hardening to softening is reminiscent of the Hall-Petch maximum in nanocrystalline or nanolaminate materials [13][14][15] but is governed by very different mechanisms. The hardness of these nanoscale contacts is between 50% and 70% larger than their corresponding tensile strength, 16,17 and their size effects exhibit similarities and interesting differences.…”
Section: Introductionmentioning
confidence: 90%
“…This external force (F ext ) is applied to all atoms within a thin slab (4.5 nm thick) at the free surfaces away for the contacting ones. 16,17 As described in Sec. II C, this closing force increases in a stepwise manner to characterize the elastic loading and plasticity in the contacting regions.…”
Section: B Contact Simulations and Hardnessmentioning
confidence: 99%
“…As is commonly done in atomistic simulations of fcc metals, 16,17 we identify dislocation activity by tracking atoms with hexagonal close packed local environments. Two consecutive planes of hcp atoms form the stacking fault ribbons that separate partial dislocations in fcc metals.…”
Section: Identification Of Atoms Responsible For Plastic Deformationmentioning
confidence: 99%
“…19 This potential was parameterized to reproduce the equilibrium lattice constant, sublimation energy, elastic contacts, and vacancy formation energy of Pt from experimental data and was used to study the strength of contacting bridges between rough surfaces, leading to predictions in good agreement with experiments. 16,17 Each simulation involves two 20-nm-thick Pt slabs with either a flat surface or a sinusoidal surface given by…”
Section: A Molecular Dynamics and Initial Structuresmentioning
We characterize how size and shape affects the hardness of nanoscale metallic contacts using large-scale molecular dynamics (MD) simulations. High-aspect-ratio contacts continue the experimentally observed trend of hardening with decreasing contact size down to the sub-10-nm regime. However, we find that this effect is shape dependent and the rate of hardening with decreasing contact size diminishes as the aspect ratio of the asperities becomes smaller. Interestingly, low-aspect-ratio asperities that can support simple dislocation glide exhibit softening with decreasing size. A detailed analysis of the MD trajectories reveals the dislocation mechanisms that govern these complex size effects.
In boundary lubrication, the detachment of lubricant molecules from a solid surface is likely to occur due to the presence of high compressive normal stress combined with shear stress exerted on the solid–liquid interface. This phenomenon often results in a delamination behavior at the interface. We aim to investigate the nanoscale roughness effect on the oil film delamination from sliding iron surfaces with grain boundaries by coarse-grained molecular dynamics simulations. As a result, the oil film delamination was effectively suppressed in higher roughness. Two distinct mechanisms of delamination were found depending on surface roughness when the critical normal stress is exceeded. High roughness enhanced the ability to prevent complete slip but had negligible influence on partial slip.
Graphical Abstract
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