Vibrational Transportation of Deformable Axisymmetric Particles

TL;DR

This paper models the vibrational transportation of deformable axisymmetric particles on a surface acoustic wave, incorporating realistic contact mechanics and hysteresis to analyze particle drift and motion regimes.

Contribution

It introduces a contact model based on Cattaneo-Mindlin mechanics and the Method of Memory Diagrams for deformable particles, extending traditional point-mass theories.

Findings

Particles can drift in or against wave direction depending on contact regime.

Multiple rebounds can lead to directed horizontal motion via synchronization.

Deformable particles exhibit different behavior than point masses, with potential for controlled transport.

Abstract

A particle on a substrate supporting a surface acoustic wave can experience horizontal drift excited by the dry friction force. The effect is referred to as vibrational transportation, or as a surface acoustic wave motor. A traditional theory of vibrational transportation considers a particle as a material point moving on a rigid substrate. A more realistic representation is a contact model based on Cattaneo-Mindlin (also called Hertz-Mindlin) mechanics applicable to an axisymmetric deformable particle. A recent semi-analytical extension of the Cattaneo-Mindlin solution called the Method of Memory Diagrams allows one to compute the hysteretic friction force for an arbitrary loading history in terms of contact displacements, and, subsequently, to numerically solve the equations of motion. Depending on the materials' and excitation parameters, the particle can stay in permanent contact with the substrate or experience multiple jumps. In the former case, the particle can slide along the surface, during each wave period, advancing and receding with different efficiencies, which finally results in a drift. The drift can occur both in the wave propagation direction and against it. In the regime of multiple jumps, directed horizontal motion is also possible. It is based on synchronization between the wave period and rebounding events. A rebound occurs once per period and consistently at the same phase. At the beginning of the process, the particle moves with an acceleration that decreases and finally disappears. Exactly the same type of motion against the wave has been observed in our preliminary experiments. We demonstrate that a point mass behaves differently: in a regime of permanent contact, negative and positive sliding are equilibrated, which produces no drift, whereas multiple rebounds of a point mass are always chaotic, at least for fully conservative collisions.