Abstract

Using a unique, near-field microscopy technique, fringe patterns and nanoparticle motions are visualized immediately following a nanofluid droplet deposition on a glass substrate in which an air bubble is entrapped. The nanofluid consists of DI-water, 0.10% Aluminum Oxide nanoparticles with an average diameter of 50 nm, and 0.0005% yellow-green polystyrene fluorescent particles of 1 μm diameter. High-speed, fluorescent-mode confocal imaging enables investigation of depth-wise sectioned particle movements in the nanofluid droplet inside which a bubble is entrapped. The static contact angle is increased when a bubble is applied. In the presence of the bubble in the droplet, the observed flow toward the center of the droplet is opposite to the flow observed in a droplet without the bubble. When the bubble is present, the evaporation process is retarded. Also, random motion is observed in the contact line region instead of the typical evaporation-driven flow toward the droplet edge. Once the bubble bursts, however, the total evaporation time decreases due to the change in the contact line characteristics. Moreover, the area of fringe patterns beneath the bubble increases with time. Discussed herein is a unique internal flow that has not been observed in nanofluid droplet evaporation.

Highlights

  • Difference due to entrapment of an air bubble

  • The equilibrium static contact angle was measured θ = 67 ± 0.75° for a droplet without an air bubble, while it was observed θ = 89 ± 0.10° for a droplet with an air bubble using a contact angle measurement apparatus developed at Michigan Technological University[22]

  • Confocal imaging allows for visualizing velocities in a thin optical plane while simultaneously capturing fringe patterns that describe the shape of the interface

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Summary

Introduction

Difference due to entrapment of an air bubble. Once the air bubble is entrapped, the contact angle becomes larger and the droplet contact diameter and center-height increases. When an entrapped air bubble is present the internal flow direction is altered. The change in internal flow direction affects the evaporation process as well as the nanoparticle deposition pattern once the droplets have dried. This study shows the unique internal flow beneath the air bubble and no directional flow (random motion) at the edge of the droplet via the use of an anomalous bubble inside the nanofluid droplet

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