Thermocapillary Convection in Superimposed Layers of Self-Rewetting Fluids: Analytical and Lattice Boltzmann Computational Study

TL;DR

This study develops analytical and computational models to analyze thermocapillary convection in superimposed self-rewetting fluid layers, revealing unique flow patterns and the influence of surface tension sensitivity on flow behavior.

Contribution

It introduces a new analytical solution and a lattice Boltzmann computational method for studying thermocapillary convection in SRFs, highlighting differences from normal fluids.

Findings

SRFs produce eight counterrotating convection rolls, unlike four in NFs.

Flow direction in SRFs is towards hotter zones, opposite to NFs.

Flow patterns and magnitude can be tuned by surface tension sensitivity coefficients.

Abstract

Self-rewetting fluids (SRFs), such as aqueous solutions of long-chain alcohols, exhibit anomalous quadratic dependence of surface tension on temperature having a minimum and with a positive gradient. When compared to the normal fluids (NFs), the SRFs can be associated with significantly modified interfacial dynamics, which have recently been exploited to enhance flow and thermal transport in various applications (e.g., microgravity and microscale transport systems). In this work, first, we develop a new analytical solution of thermocapillary convection in superimposed two SRF layers confined within a microchannel that is sinusoidally heated on one side and maintained at a uniform temperature on the other side under the creeping flow regime. Then, a robust central moment lattice Boltzmann method using the Allen-Cahn equation for interface tracking, two-fluid motion, and the energy transport for numerical simulations of SRFs is constructed. The analytical and computational techniques are generally shown to be in good quantitative agreement with one another. Moreover, the effect of the various characteristic parameters on the magnitude and the distribution thermocapillary-driven motion is studied. The thermocapillary flow patterns in SRFs are shown to be strikingly different when compared to the NFs: For otherwise the same conditions, the SRFs result in eight periodic counterrotating thermocapillary convection rolls, while the NFs exhibit only four such vortices. Moreover, the direction of the circulating fluid motion in such vortical structures for the SRFs is found to be towards the hotter zones on the interfaces, which is opposite to that in NFs. By tuning the sensitivity coefficients of the surface tension on temperature, it is shown that the magnitude as well the overall thermocapillary flow patterns can be significantly manipulated.