Acoustic Streaming and Its Applications

Broadly speaking, acoustic streaming is generated by a nonlinear acoustic wave with a finite amplitude propagating in a viscid fluid. The fluid volume elements of molecules, <inline-formula> <math display="inline"> <semantics> <mrow> <mi>d</mi> <mi>...

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Main Author: Junru Wu
Format: Article
Language:English
Published: MDPI AG 2018-12-01
Series:Fluids
Subjects:
Online Access:https://www.mdpi.com/2311-5521/3/4/108
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spelling doaj-52a07150a2c04c60b5d3f210295bc9332020-11-24T23:58:06ZengMDPI AGFluids2311-55212018-12-013410810.3390/fluids3040108fluids3040108Acoustic Streaming and Its ApplicationsJunru Wu0Department of Physics, 82 University Place, University of Vermont, Burlington, VT 05405, USABroadly speaking, acoustic streaming is generated by a nonlinear acoustic wave with a finite amplitude propagating in a viscid fluid. The fluid volume elements of molecules, <inline-formula> <math display="inline"> <semantics> <mrow> <mi>d</mi> <mi>V</mi> </mrow> </semantics> </math> </inline-formula>, are forced to oscillate at the same frequency as the incident acoustic wave. Due to the nature of the nonlinearity of the acoustic wave, the second-order effect of the wave propagation produces a time-independent flow velocity (DC flow) in addition to a regular oscillatory motion (AC motion). Consequently, the fluid moves in a certain direction, which depends on the geometry of the system and its boundary conditions, as well as the parameters of the incident acoustic wave. The small scale acoustic streaming in a fluid is called &#8220;microstreaming&#8222;. When it is associated with acoustic cavitation, which refers to activities of microbubbles in a general sense, it is often called &#8220;cavitation microstreaming&#8222;. For biomedical applications, microstreaming usually takes place in a boundary layer at proximity of a solid boundary, which could be the membrane of a cell or walls of a container. To satisfy the non-slip boundary condition, the flow motion at a solid boundary should be zero. The magnitude of the DC acoustic streaming velocity, as well as the oscillatory flow velocity near the boundary, drop drastically; consequently, the acoustic streaming velocity generates a DC velocity gradient and the oscillatory flow velocity gradient produces an AC velocity gradient; they both will produce shear stress. The former is a DC shear stress and the latter is AC shear stress. It was observed the DC shear stress plays the dominant role, which may enhance the permeability of molecules passing through the cell membrane. This phenomenon is called &#8220;sonoporation&#8222;. Sonoporation has shown a great potential for the targeted delivery of DNA, drugs, and macromolecules into a cell. Acoustic streaming has also been used in fluid mixing, boundary cooling, and many other applications. The goal of this work is to give a brief review of the basic mathematical theory for acoustic microstreaming related to the aforementioned applications. The emphasis will be on its applications in biotechnology.https://www.mdpi.com/2311-5521/3/4/108acoustic streamingsonoporationmicrofluidic devicesurface acoustic waves (SAW)fluid mixingtargeted drug delivery
collection DOAJ
language English
format Article
sources DOAJ
author Junru Wu
spellingShingle Junru Wu
Acoustic Streaming and Its Applications
Fluids
acoustic streaming
sonoporation
microfluidic device
surface acoustic waves (SAW)
fluid mixing
targeted drug delivery
author_facet Junru Wu
author_sort Junru Wu
title Acoustic Streaming and Its Applications
title_short Acoustic Streaming and Its Applications
title_full Acoustic Streaming and Its Applications
title_fullStr Acoustic Streaming and Its Applications
title_full_unstemmed Acoustic Streaming and Its Applications
title_sort acoustic streaming and its applications
publisher MDPI AG
series Fluids
issn 2311-5521
publishDate 2018-12-01
description Broadly speaking, acoustic streaming is generated by a nonlinear acoustic wave with a finite amplitude propagating in a viscid fluid. The fluid volume elements of molecules, <inline-formula> <math display="inline"> <semantics> <mrow> <mi>d</mi> <mi>V</mi> </mrow> </semantics> </math> </inline-formula>, are forced to oscillate at the same frequency as the incident acoustic wave. Due to the nature of the nonlinearity of the acoustic wave, the second-order effect of the wave propagation produces a time-independent flow velocity (DC flow) in addition to a regular oscillatory motion (AC motion). Consequently, the fluid moves in a certain direction, which depends on the geometry of the system and its boundary conditions, as well as the parameters of the incident acoustic wave. The small scale acoustic streaming in a fluid is called &#8220;microstreaming&#8222;. When it is associated with acoustic cavitation, which refers to activities of microbubbles in a general sense, it is often called &#8220;cavitation microstreaming&#8222;. For biomedical applications, microstreaming usually takes place in a boundary layer at proximity of a solid boundary, which could be the membrane of a cell or walls of a container. To satisfy the non-slip boundary condition, the flow motion at a solid boundary should be zero. The magnitude of the DC acoustic streaming velocity, as well as the oscillatory flow velocity near the boundary, drop drastically; consequently, the acoustic streaming velocity generates a DC velocity gradient and the oscillatory flow velocity gradient produces an AC velocity gradient; they both will produce shear stress. The former is a DC shear stress and the latter is AC shear stress. It was observed the DC shear stress plays the dominant role, which may enhance the permeability of molecules passing through the cell membrane. This phenomenon is called &#8220;sonoporation&#8222;. Sonoporation has shown a great potential for the targeted delivery of DNA, drugs, and macromolecules into a cell. Acoustic streaming has also been used in fluid mixing, boundary cooling, and many other applications. The goal of this work is to give a brief review of the basic mathematical theory for acoustic microstreaming related to the aforementioned applications. The emphasis will be on its applications in biotechnology.
topic acoustic streaming
sonoporation
microfluidic device
surface acoustic waves (SAW)
fluid mixing
targeted drug delivery
url https://www.mdpi.com/2311-5521/3/4/108
work_keys_str_mv AT junruwu acousticstreaminganditsapplications
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