2019
DOI: 10.1063/1.5121728
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Numerical and experimental investigation of the stability of a drop in a single-axis acoustic levitator

Abstract: Paper published as part of the special topic on Drops and Flows in Acoustic Levitation Note: This paper is part of the Special Topic on Drops and Flows in Acoustic Levitation. This paper was selected as Featured ARTICLES YOU MAY BE INTERESTED IN Review of transport processes and particle self-assembly in acoustically levitated nanofluid droplets

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Cited by 30 publications
(14 citation statements)
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References 72 publications
(108 reference statements)
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“…2 denote the time average over one cycle of acoustic oscillation. The first term represents the high acoustic pressure region exerting a positive pressure over the droplet surface, while the second term implies the Bernoulli effect representing the oscillation of the air particles exerting a negative pressure on the droplet ( 35 ). However, it is extremely difficult to determine F A exerted on the droplet because of the sensitivity of the twin trap ultrasonic field.…”
Section: Resultsmentioning
confidence: 99%
“…2 denote the time average over one cycle of acoustic oscillation. The first term represents the high acoustic pressure region exerting a positive pressure over the droplet surface, while the second term implies the Bernoulli effect representing the oscillation of the air particles exerting a negative pressure on the droplet ( 35 ). However, it is extremely difficult to determine F A exerted on the droplet because of the sensitivity of the twin trap ultrasonic field.…”
Section: Resultsmentioning
confidence: 99%
“…1A, the droplet located in the standing wave will be levitated by the acoustic radiation force F rad , which can be defined by integrating the radiation pressure p rad over the droplet surface S . 60 where n is the normal unit vector pointing outward from the surface S , and the time-averaged radiation pressure p rad distribution over the droplet surface can be calculated bywhere ρ 0 is the unperturbed air density, c 0 is the speed of sound in air, p is the acoustic pressure, u is the medium particle velocity, and 〈 〉 denotes the time-averaged value over one cycle. The time-averaged radiation pressure, as given by eqn (2), is dependent on two distinct terms.…”
Section: Resultsmentioning
confidence: 99%
“…The technique of acoustic levitation can levitate almost any type of liquid without requiring the samples' electric/ magnetic properties. [13][14][15] This means it could provide contact-free manipulation and active stimulus to a wide range of materials, including complex fluids and soft matter. Owing to the inhibition of solid surfaces, acoustic levitation showed great potential for the investigation of the dynamics and physics of the liquid-air interfaces from interfacial rheology, and assembly to phase behaviors.…”
Section: Introductionmentioning
confidence: 99%