Critical length limiting super-low friction
arXiv:1501.00360 · doi:10.1103/PhysRevLett.114.055501
Abstract
Since the demonstration of super-low friction (superlubricity) in graphite at nanoscale, one of the main challenges in the field of nano- and micro-mechanics was to scale this phenomenon up. A key question to be addressed is to what extent superlubricity could persist, and what mechanisms could lead to its failure. Here, using an edge-driven Frenkel-Kontorova model, we establish a connection between the critical length above which superlubricity disappears and both intrinsic material properties and experimental parameters. A striking boost in dissipated energy with chain length emerges abruptly due to a high-friction stick-slip mechanism caused by deformation of the slider leading to a local commensuration with the substrate lattice. We derived a parameter-free analytical model for the critical length that is in excellent agreement with our numerical simulations. Our results provide a new perspective on friction and nano-manipulation and can serve as a theoretical basis for designing nano-devices with super-low friction, such as carbon nanotubes.
arXiv commentAccepted on PRL
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Cited by in corpus (11)
- Superlubricity of Graphene Nanoribbons on Gold Surfaces
- Observation of normal-force-independent superlubricity in mesoscopic graphite contacts
- Solidification and superlubricity with molecular alkane films
- Kinetic Friction of Structurally Superlubric 2D Material Interfaces
- Current trends in the physics of nanoscale friction
- Static friction boost in edge-driven incommensurate contacts
- Moiré-pattern evolution couples rotational and translational friction at crystalline interfaces
- Atomistic mechanism of friction force independence on the normal load and other friction laws for dynamic structural superlubricity
- Effective stick-slip parameter for structurally lubric 2D interface friction
- The impact of static distortion waves on superlubricity
- Sliding states of a soft-colloid cluster crystal: Cluster versus single-particle hopping