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Onset of Visible Capillary Waves from High-Frequency Acoustic Excitation
[Image: see text] Remarkably, the interface of a fluid droplet will produce visible capillary waves when exposed to acoustic waves. For example, a small (∼1 μL) sessile droplet will oscillate at a low ∼10(2) Hz frequency when weakly driven by acoustic waves at ∼10(6) Hz frequency and beyond. We meas...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2023
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10018762/ https://www.ncbi.nlm.nih.gov/pubmed/36857201 http://dx.doi.org/10.1021/acs.langmuir.2c03403 |
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author | Zhang, Shuai Orosco, Jeremy Friend, James |
author_facet | Zhang, Shuai Orosco, Jeremy Friend, James |
author_sort | Zhang, Shuai |
collection | PubMed |
description | [Image: see text] Remarkably, the interface of a fluid droplet will produce visible capillary waves when exposed to acoustic waves. For example, a small (∼1 μL) sessile droplet will oscillate at a low ∼10(2) Hz frequency when weakly driven by acoustic waves at ∼10(6) Hz frequency and beyond. We measured such a droplet’s interfacial response to 6.6 MHz ultrasound to gain insight into the energy transfer mechanism that spans these vastly different time scales, using high-speed microscopic digital transmission holography, a unique method to capture three-dimensional surface dynamics at nanometer space and microsecond time resolutions. We show that low-frequency capillary waves are driven into existence via a feedback mechanism between the acoustic radiation pressure and the evolving shape of the fluid interface. The acoustic pressure is distributed in the standing wave cavity of the droplet, and as the shape of the fluid interface changes in response to the distributed pressure present on the interface, the standing wave field also changes shape, feeding back to produce changes in the acoustic radiation pressure distribution in the cavity. A physical model explicitly based upon this proposed mechanism is provided, and simulations using it were verified against direct observations of both the microscale droplet interface dynamics from holography and internal pressure distributions using microparticle image velocimetry. The pressure-interface feedback model accurately predicts the vibration amplitude threshold at which capillary waves appear, the subsequent amplitude and frequency of the capillary waves, and the distribution of the standing wave pressure field within the sessile droplet responsible for the capillary waves. |
format | Online Article Text |
id | pubmed-10018762 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-100187622023-03-17 Onset of Visible Capillary Waves from High-Frequency Acoustic Excitation Zhang, Shuai Orosco, Jeremy Friend, James Langmuir [Image: see text] Remarkably, the interface of a fluid droplet will produce visible capillary waves when exposed to acoustic waves. For example, a small (∼1 μL) sessile droplet will oscillate at a low ∼10(2) Hz frequency when weakly driven by acoustic waves at ∼10(6) Hz frequency and beyond. We measured such a droplet’s interfacial response to 6.6 MHz ultrasound to gain insight into the energy transfer mechanism that spans these vastly different time scales, using high-speed microscopic digital transmission holography, a unique method to capture three-dimensional surface dynamics at nanometer space and microsecond time resolutions. We show that low-frequency capillary waves are driven into existence via a feedback mechanism between the acoustic radiation pressure and the evolving shape of the fluid interface. The acoustic pressure is distributed in the standing wave cavity of the droplet, and as the shape of the fluid interface changes in response to the distributed pressure present on the interface, the standing wave field also changes shape, feeding back to produce changes in the acoustic radiation pressure distribution in the cavity. A physical model explicitly based upon this proposed mechanism is provided, and simulations using it were verified against direct observations of both the microscale droplet interface dynamics from holography and internal pressure distributions using microparticle image velocimetry. The pressure-interface feedback model accurately predicts the vibration amplitude threshold at which capillary waves appear, the subsequent amplitude and frequency of the capillary waves, and the distribution of the standing wave pressure field within the sessile droplet responsible for the capillary waves. American Chemical Society 2023-03-01 /pmc/articles/PMC10018762/ /pubmed/36857201 http://dx.doi.org/10.1021/acs.langmuir.2c03403 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Zhang, Shuai Orosco, Jeremy Friend, James Onset of Visible Capillary Waves from High-Frequency Acoustic Excitation |
title | Onset of Visible Capillary Waves from High-Frequency
Acoustic Excitation |
title_full | Onset of Visible Capillary Waves from High-Frequency
Acoustic Excitation |
title_fullStr | Onset of Visible Capillary Waves from High-Frequency
Acoustic Excitation |
title_full_unstemmed | Onset of Visible Capillary Waves from High-Frequency
Acoustic Excitation |
title_short | Onset of Visible Capillary Waves from High-Frequency
Acoustic Excitation |
title_sort | onset of visible capillary waves from high-frequency
acoustic excitation |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10018762/ https://www.ncbi.nlm.nih.gov/pubmed/36857201 http://dx.doi.org/10.1021/acs.langmuir.2c03403 |
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