TY - JOUR
T1 - Acoustic streaming
T2 - An arbitrary Lagrangian-Eulerian perspective
AU - Nama, Nitesh
AU - Huang, Tony Jun
AU - Costanzo, Francesco
N1 - Funding Information:
This work was supported by National Institutes of Health (1R01 GM112048-01A1, 1R33EB019785-01), National Science Foundation (CBET-1438126 and IIP-1346440), and the Penn State Center for Nanoscale Science (MRSEC) under grant DMR-0820404.
Publisher Copyright:
© 2017 Cambridge University Press.
PY - 2017/8/25
Y1 - 2017/8/25
N2 - We analyse acoustic streaming flows using an arbitrary Lagrangian Eulerian (ALE) perspective. The formulation stems from an explicit separation of time scales resulting in two subproblems: a first-order problem, formulated in terms of the fluid displacement at the fast scale, and a second-order problem, formulated in terms of the Lagrangian flow velocity at the slow time scale. Following a rigorous time-averaging procedure, the second-order problem is shown to be intrinsically steady, and with exact boundary conditions at the oscillating walls. Also, as the second-order problem is solved directly for the Lagrangian velocity, the formulation does not need to employ the notion of Stokes drift, or any associated post-processing, thus facilitating a direct comparison with experiments. Because the first-order problem is formulated in terms of the displacement field, our formulation is directly applicable to more complex fluid-structure interaction problems in microacoustofluidic devices. After the formulation's exposition, we present numerical results that illustrate the advantages of the formulation with respect to current approaches.
AB - We analyse acoustic streaming flows using an arbitrary Lagrangian Eulerian (ALE) perspective. The formulation stems from an explicit separation of time scales resulting in two subproblems: a first-order problem, formulated in terms of the fluid displacement at the fast scale, and a second-order problem, formulated in terms of the Lagrangian flow velocity at the slow time scale. Following a rigorous time-averaging procedure, the second-order problem is shown to be intrinsically steady, and with exact boundary conditions at the oscillating walls. Also, as the second-order problem is solved directly for the Lagrangian velocity, the formulation does not need to employ the notion of Stokes drift, or any associated post-processing, thus facilitating a direct comparison with experiments. Because the first-order problem is formulated in terms of the displacement field, our formulation is directly applicable to more complex fluid-structure interaction problems in microacoustofluidic devices. After the formulation's exposition, we present numerical results that illustrate the advantages of the formulation with respect to current approaches.
UR - http://www.scopus.com/inward/record.url?scp=85025477595&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85025477595&partnerID=8YFLogxK
U2 - 10.1017/jfm.2017.338
DO - 10.1017/jfm.2017.338
M3 - Review article
C2 - 29051631
AN - SCOPUS:85025477595
SN - 0022-1120
VL - 825
SP - 600
EP - 630
JO - Journal of Fluid Mechanics
JF - Journal of Fluid Mechanics
ER -