2007
DOI: 10.1007/s10404-007-0207-y
|View full text |Cite
|
Sign up to set email alerts
|

Simulation-based analysis of flow due to traveling-plane-wave deformations on elastic thin-film actuators in micropumps

Abstract: One of the propulsion mechanisms of microorganisms is based on propagation of bending deformations on an elastic tail. In principle, an elastic thin-film can be placed in a channel and actuated for pumping of the fluid by means of introducing a series of traveling-wave deformations on the film. Here, we present a simulation-based analysis of transient, two-dimensional Stokes flow induced by propagation of sinusoidal deformations on an elastic thin-film submerged in a fluid between parallel plates. Simulations … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

1
6
0

Year Published

2008
2008
2018
2018

Publication Types

Select...
5
1

Relationship

0
6

Authors

Journals

citations
Cited by 11 publications
(7 citation statements)
references
References 29 publications
1
6
0
Order By: Relevance
“…In Figures 4 and 5, average flow rate is shown as a function of time for wavelengths of 80µm and 640 µm respectively. Similar behavior is observed in the numerical simulations of the micropump that is actuated by travelling-plane-wave deformations [13].…”
Section: Resultssupporting
confidence: 81%
See 1 more Smart Citation
“…In Figures 4 and 5, average flow rate is shown as a function of time for wavelengths of 80µm and 640 µm respectively. Similar behavior is observed in the numerical simulations of the micropump that is actuated by travelling-plane-wave deformations [13].…”
Section: Resultssupporting
confidence: 81%
“…Normalizing swimming speed for the base case is obtained as 4.99 µm/s. The speed of a microswimmer is calculated by Behkam and Sitti based on the resistive force theory [10,13]…”
Section: Resultsmentioning
confidence: 99%
“…The fluidic domain in the channel Γ( t ) as depicted in Figure a, is governed by Newtonian, incompressible, 3D, and time‐dependent Navier–Stokes equations subject to conservation of mass in arbitrary Lagrangian–Eulerian (ALE) scheme as follows: leftρ()Ut+false(bold-italicUbold-italicufalse)·U=p+μ2bold-italicUleft·bold-italicU=0where u denotes the velocity vector of the moving mesh. Furthermore, the governing equation and equation of motion are written in nondimensional fashion, as practiced in previous studies . It is also noted that the fluidic domain Γ( t ) is considered to be under isothermal conditions at all times.…”
Section: Modelingmentioning
confidence: 99%
“…Known theoretical models predict the effect of the flow fields, invoked by simultaneous propulsion and pumping action of the complex geometries such as a cargo towed by a rotating helix, only up to a certain degree. The reason is the analytical methods of choice being subject to limiting geometrical and temporal assumptions in order to be able to obtain a solution without dealing with the problem at hand in full scale . Moreover, the highly non‐linear nature of the Navier–Stokes equations did not allow a comprehensive closed‐form analytical solution of the problem to this date.…”
Section: Introductionmentioning
confidence: 99%
“…[23,24,[41][42][43][44] The Re number is defined as Re = 0.01 for the results presented in this work. As a result, the scaling Reynolds number becomes Re = 2π fρD body 2 /μ, the reciprocal of which will be used to define the dimensionless dynamic viscosity of the domain (t), which is a common practice for micro-hydrodynamic analysis of such micro-swimmers.…”
Section: Modelingmentioning
confidence: 99%