Bounds on the electrical resistance between contacting elastic rough bodies

By J. Barber. Proceedings of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences, 2003

232 citations recorded by the source corpus.

Subfields: Atomic and Molecular Physics, and Optics, Mechanics of Materials

View Paper: https://www.semanticscholar.org/paper/5e3617b7ab639d0a1893d2f00d44cb7a7ff7b1e4

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In Atomic and Molecular Physics, and Optics

In Mechanics of Materials

Citations in the corpus

On local indentation and impact compliance of isotropic auxetic materials from the continuum mechanics viewpoint (2012, methodology): “Observe that formula (8) is in complete agreement with Barber’s theorem on incremental indentation compliance (Barber, 2003).”
Inclusion of “interaction” in the Greenwood and Williamson contact theory (2008, methodology): “[3,5,6] also calculated the conductance (per nit area) between the surfaces, by using the theorem due to arber [7], that the conductance may be found from the stiffess by replacing the contact modulus, E*, by the electrical or hermal conductance, ρ−1 or K.”
Meeting the Contact-Mechanics Challenge (2017, background): “, dp/dū, also called the interfacial stiffness, is often assumed to be proportional to the electrical contact conductance, so that knowledge of ū(p∗) allows one to estimate that property [60,61].”
Modeling and simulation in tribology across scales: An overview (2018, methodology): “on the lower frequency contents of the PSD, as demonstrated by Barber [366].”
Statistical model of nearly complete elastic rough surface contact (2014, background): “A rigorous proof of the above equivalence can be found in the work of Barber (2003). Let us define the entire z 1⁄4 0 plane of the equivalent rough surface as domain X.”
A Review of Elastic–Plastic Contact Mechanics (2017, background): “Many subsequent works [86,201–215] have employed fractals to characterize rough surfaces, typically using one the aforementioned models to handle the contact mechanics.”