Superlubricity

Foam in an egg carton which simulates the atomic surface structure of graphite, commensurable due to alignment in this photo
Incommensurable due to twisting, so the valleys and hills don't line up

Superlubricity is a regime of motion in which friction vanishes or very nearly vanishes. What is a "vanishing" friction level is not clear, which makes the term of the superlubricity to be quite vague. As an ad hoc definition, a kinetic coefficient of friction less than 0.001 can be adopted.[1] This definition also requires further discussion and clarification.

Superlubricity may occur when two crystalline surfaces slide over each other in dry incommensurate contact. This effect, also called structural lubricity, was suggested in 1991 and verified with great accuracy between two graphite surfaces in 2004.[2] The atoms in graphite are oriented in a hexagonal manner and form an atomic hill-and-valley landscape, which looks like an egg-crate. When the two graphite surfaces are in registry (every 60 degrees), the friction force is high. When the two surfaces are rotated out of registry, the friction is largely reduced. This is like two egg-crates which can slide over each other more easily when they are "twisted" with respect to each other.

Observation of superlubricity in microscale graphite structures was reported in 2012,[3] by shearing a square graphite mesa a few micrometers across, and observing the self-retraction of the sheared layer. Such effects were also theoretically described[4] for a model of graphene and nickel layers. This observation, which is reproducible even under ambient conditions, shifts interest in superlubricity from a primarily academic topic, accessible only under highly idealized conditions, to one with practical implications for micro and nanomechanical devices.[5]

A state of ultralow friction can also be achieved when a sharp tip slides over a flat surface and the applied load is below a certain threshold. Such "superlubric" threshold depends on the tip-surface interaction and the stiffness of the materials in contact, as described by the Tomlinson model.[6] The threshold can be significantly increased by exciting the sliding system at its resonance frequency, which suggests a practical way to limit wear in nanoelectromechanical systems.[7]

Superlubricity was also observed between a gold AFM tip and Teflon substrate due to repulsive Van der Waals forces and hydrogen-bonded layer formed by glycerol on the steel surfaces. Formation of the hydrogen-bonded layer was also shown to lead to superlubricity between quartz glass surfaces lubricated by biological liquid obtained from mucilage of Brasenia schreberi.

The similarity of the term superlubricity with terms such as superconductivity and superfluidity is misleading; other energy dissipation mechanisms can lead to a finite (normally small) friction force.

Superlubricity at the macroscale

In 2015, "Argonne scientists used Mira [supercomputer] to identify and improve a new mechanism for eliminating friction, which fed into the development of a hybrid material that exhibited superlubricity at the macroscale for the first time [..] simulating up to 1.2 million atoms for dry environments and up to 10 million atoms for humid environments [..] The researchers used the LAMMPS (Large-scale Atomic/Molecular Massively Parallel Simulator) code to carry out the computationally demanding reactive molecular dynamics simulations. [.. A] team of computational scientists [..] were able to overcome a performance bottleneck with the code's ReaxFF module, an add-on package that was needed to model the chemical reactions occurring in the system. [.. The team] optimized LAMMPS and its implementation of ReaxFF by adding OpenMP threading, replacing MPI point-to-point communication with MPI collectives in key algorithms, and leveraging MPI I/O. Altogether, these enhancements allowed the code to perform twice as fast as before."[8]

"The research team is in the process of seeking a patent for the hybrid material, which could potentially be used for applications in dry environments, such as computer hard drives, wind turbine gears, and mechanical rotating seals for microelectromechanical and nanoelectromechanical systems."[8]

See also

References

  1. ↑ Müser, Martin H. (2015-01-01). Gnecco, Enrico; Meyer, Ernst, eds. Fundamentals of Friction and Wear on the Nanoscale. NanoScience and Technology. Springer International Publishing. pp. 209–232. doi:10.1007/978-3-319-10560-4_11. ISBN 9783319105598.
  2. ↑ Superlubricity of Graphite Martin Dienwiebel, Gertjan S. Verhoeven, Namboodiri Pradeep, Joost W. M. Frenken, Jennifer A. Heimberg, and Henny W. Zandbergen Phys. Rev. Lett. 92, 126101 (2004) doi:10.1103/PhysRevLett.92.126101
  3. ↑ Observation of Superlubricity in Microscale Graphite Ze Liu, Jiarui Yang, Francois Grey, Jefferson Zhe Liu, Yilun Liu, Yibing Wang, Yanlian Yang, Yao Cheng, and Quanshui Zheng Phys. Rev. Lett. 108, 205503 (2012) doi:10.1103/PhysRevLett.108.205503
  4. ↑ Superlubricity through graphene multilayers between Ni(111) surfaces
  5. ↑ Graphite super lube works at micron scale Philip Robinson, Chemistry World, 28 May 2012
  6. ↑ Transition from Stick-Slip to Continuous Sliding in Atomic Friction: Entering a New Regime of Ultralow Friction Anisoara Socoliuc, Enrico Gnecco, Roland Bennewitz, and Ernst Meyer Phys. Rev. Lett. 92, 134301 (2004) doi:10.1103/PhysRevLett.92.134301
  7. ↑ Atomic-Scale Control of Friction by Actuation of Nanometer-Sized Contacts Anisoara Socoliuc, Enrico Gnecco, Sabine Maier, Oliver Pfeiffer, Alexis Baratoff, Roland Bennewitz, and Ernst Meyer Science 313, 207 (2006) doi:10.1126/science.1125874
  8. 1 2 http://www.sciencedaily.com/releases/2015/07/150721194001.htm
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