Electroosmotic flow in small-scale channels induced by surface-acoustic waves

TL;DR

This paper uses numerical simulations to demonstrate that surface-acoustic waves induce a significant electroosmotic flow in nanochannels, offering a potential alternative method for fluid pumping in microfluidic systems without electrodes.

Contribution

It reveals the mechanism of SAW-induced electroosmotic flow in nanochannels and analyzes how frequency and phase-shifted waves optimize the flow, expanding understanding of acoustofluidic actuation.

Findings

SAWs induce a time-averaged electroosmotic flow in nanochannels.

Flow magnitude depends on SAW frequency and phase-shift configuration.

SAW-EOF can dominate other pumping mechanisms in narrow channels.

Abstract

Numerical simulations of the Navier-Stokes, Nernst-Planck, and the Poisson equations are employed to describe the transport processes in an aqueous electrolyte in a parallel-plate nanochannel, where surface-acoustic waves (SAWs) are standing or traveling along (piezo-active) channel walls. It is found that -- in addition to the conventional acoustic streaming flow -- a time-averaged electroosmotic flow is induced. Employing the stream function-vorticity formulation, it is shown that the Maxwell stress term causes an electroosmotic propulsion that is qualitatively identical to the one discussed in the context of alternating current (AC) electroosmosis (EOF). Differences arise mainly due to the high actuation frequencies of SAWs, which are in the MHz range rather than in the kHz regime typical for ACEOF. Moreover, the instantaneous spatial periodicity of the EOF in the travel direction of the SAW is intrinsically linked to the dispersion relation of the latter rather than a free geometric parameter. This leads to a specific frequency band where an EOF of sizable magnitude can be found. On the low frequency end, the ratio between the electric double layer (EDL) thickness and the SAW wavelength becomes extremely small so that the net force leading to a non-vanishing time-averaged flow becomes equally small. On the high frequency end, the RC time of the EDL is much larger than the inverse of the SAW frequency leading to a vanishing effective charge density of the EDL. For a parallel-plate channel, the EOF can be maximized by using two SAWs on both channel walls that have the same frequency but are phase-shifted by $180^\circ$. It appears that the SAW-EOF is the dominant pumping mechanism for such a scenario. The proposed actuation might be a viable alternative for driving liquid electrolytes through narrow ducts and channels, without the need for electric interconnects and electrodes.