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Alternating Current Electro-Osmotic Flow of the Maxwell Fluids Through a Circular Micro-Pipe

Published online by Cambridge University Press:  20 December 2012

L.-X. Sun
Affiliation:
School of Mathematical Science, Inner Mongolia University, Hohhot, Inner Mongolia 010021, China
Y.-J. Jian*
Affiliation:
School of Mathematical Science, Inner Mongolia University, Hohhot, Inner Mongolia 010021, China
L. Chang
Affiliation:
School of Mathematical Science, Inner Mongolia University, Hohhot, Inner Mongolia 010021, China School of Mathematics and Statistics, Inner Mongolia Finance and Economics College, Hohhot, Inner Mongolia 010051, China
H.-Y. Zhang
Affiliation:
College of Mathematical Science, Baotou teacher's college, Inner Mongolia 014030, China
Q.-S. Liu
Affiliation:
School of Mathematical Science, Inner Mongolia University, Hohhot, Inner Mongolia 010021, China
*
*Corresponding author (jianyongjun@yahoo.com.cn)
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Abstract

Analytical solutions are presented for time periodic EOF flow of linear viscoelastic fluids through a cylindrical micro-pipe. The linear viscoelastic fluids used here are described by the general Maxwell model. The solution involves analytically solving the linearized Poisson-Boltzmann equation, together with the Cauchy momentum equation and the general Maxwell constitutive equation considering the depletion effect produced by the interaction between macro-molecules of the Maxwell fluid and the channel surface. The overall flow is divided into depletion layer and bulk flow outside of depletion layer. The velocity expressions of these two layers were obtained, respectively. By numerical computations, the influences of the periodic EOF electric oscillating Reynolds number Re, Deborah number De, depletion layer thickness δ and the viscosity ratio γ of Maxwell to Newtonian fluids on velocity profile are presented. For a prescribed De, the increasing Re will cause large changes of the EOF velocity with decreasing velocity magnitude. For a given Re, large De gives large EOF velocity magnitude. Increasing γ will lead to larger velocity amplitude for a given lower Re. However, at higher Re, the velocity amplitude decreases with the viscosity ratio γ, especially within the depletion layer. In addition, large depletion layer thickness gives small EOF velocity magnitude for fixed Re and De. Finally, the influence of De on energy dissipation is studied. These results provide a detail insight of the flow characteristic of this flow configuration.

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Articles
Copyright
Copyright © The Society of Theoretical and Applied Mechanics, R.O.C. 2013

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References

REFERENCES

1.Stone, H. A., Stroock, A. D. and Ajdari, A., “Engineering Flows in Small Devices: Microfluidics Toward a Lab-On-A-Chip,” Annual Review of Fluid Mechanics, 36, pp. 381411 (2004).CrossRefGoogle Scholar
2.Bayraktar, T. and Pidugu, S. B., “Characterization of Liquid Flows in Microfluidic Systems,” International Journal of Heat and Mass Transfer, 49, pp. 815824 (2006).Google Scholar
3.Das, S. and Chakraborty, S., “Analytical Solutions for Velocity, Temperature and Concentration Distribution in Electroosmotic Micro-Channel Flows in a Non-Newtonian Bio-Fluid,” Analytical Chimica Acta, 559, pp. 1524 (2006).Google Scholar
4.Chakraborty, S., “Electroosmotically Driven Capillary Transport of Typical Non-Newtonian Biofluids in Rectangular Microchannels,” Analytical Chimica Acta, 605, pp. 175184 (2007).Google Scholar
5.Zhao, C., Zholkovskij, E., Masliyah, J. H. and Yang, C., “Analysis of Electroosmotic Flow of Power-Law Fluids in a Slit Microchannel,” Journal of Colloid and Interface Science, 326, pp. 503510 (2008).CrossRefGoogle Scholar
6.Vasu, N. and De, S., “Electroosmotic Flow of Power-Law Fluids at High Zeta Potentials,” Colloids and Surfaces A: Physicochemical and Engineering Aspects, 368, pp. 4452 (2010)CrossRefGoogle Scholar
7.Zhao, C. and Yang, C., “Nonlinear Smoluchowski velocity for Electroosmosis of Power-Law Fluids Over a Surface with Arbitrary Zeta Potentials,” Electrophoresis, 31, pp. 973979 (2010).CrossRefGoogle Scholar
8.Tang, G. H., Li, X. F., He, Y. L. and Tao, W. Q., “Electroosmotic Flow of Non-Newtonian Fluid in Microchannels,” Journal Non-Newtonian Fluid Mechanics, 157, pp. 133137 (2009).CrossRefGoogle Scholar
9.Park, H. M. and Lee, W. M., “Helmholtz-Smoluchowski Velocity for Viscoelastic Electroosmotic Flows,” Journal of Colloid and Interface Science, 317, pp. 631636 (2008).Google Scholar
10.Park, H. M. and Lee, W. M., “Effect of Viscoelasticity on the Flow Pattern and the Volumetric Flow Rate in Electroosmotic Flows Through a Microchannel,” Lab on a Chip, 8, pp. 11631170 (2008).Google Scholar
11.Liu, Q. S., Jian, Y. J. and Yang, L. G., “Time Periodic Electroosmotic Flow of the Generalized Maxwell Fluids Between Two Micro-Parallel Plates.” Journal Non-Newtonian Fluid Mechanics, 166, pp. 478486 (2011).Google Scholar
12.Jian, Y. J., Liu, Q. S. and Yang, L. G., “AC Electroosmotic Flow of Generalized Maxwell Fluids in a Rectangular Microchannel,” Journal Non-Newtonian Fluid Mechanics, 166, pp. 13041314 (2011).Google Scholar
13.Afonso, A. M., Alves, M. A. and Pinho, F. T., “Analytical Solution of Mixed Electroosmotic Pressure Driven Flows of Viscoelastic Fluids in Microchannels,” Journal of Colloid and Interface Science, 159, pp. 5063 (2009).Google Scholar
14.Bird, R. B., Dotson, P. J. and Jonson, N. L., “Polymer Solution Rheology Based on a Finitely Extensible Bead-Spring Chain Model,” Journal Non-Newtonian Fluid Mechanics, 7, pp. 213235 (1980).CrossRefGoogle Scholar
15.Dhinakaran, S., Afonso, A. M., Alves, M. A. and Pinho, F. T., “Steady Viscoelastic Fluid Flow Between Parallel Plates Under Electroosmotic Forces: Phan-Thien-Tanner Model,” Journal of Colloid and Interface Science, 344, pp. 513520 (2010).Google Scholar
16.Olivares, M. L., Vera-Candioti, L. and Berli, C. L. A., “The EOF of Polymer Solutions,” Electrophoresis, 30, pp. 921929 (2009).Google Scholar
17.Sousa, J. J., Afonso, A. M. and Pinho, F. T., “Effect of the Skimming Layer on Electro-Osmotic-Poiseuille Flows of Viscoelastic Fluids,” Microfluidics and Nanofluidics, 10, pp. 107122 (2011).Google Scholar
18.Liu, Q. S., Jian, Y. J. and Yang, L. G., “Alternating Current Electroosmotic Flow of the Jeffreys Fluids Time Through a Slit Microchannel,” Physics of Fluids, 23, 102001 (2011).Google Scholar
19.Akbar, N. S. and Nadeem, S., “Jeffrey Fluid Model for Blood Flow Through a Tapered Artery with a Stenosis,” Journal of Mechanics in Medicine and Biology, 11, pp. 529545 (2011).Google Scholar
20.Berli, C. L. A. and Olivares, M. L., “Electrokinetic Flow of Non-Newtonian Fluids on Microchannels,” Journal of Colloid and Interface Science, 320, pp. 582589 (2008).Google Scholar
21.Jian, Y. J., Yang, L. G. and Liu, Q. S., “Time Periodic Electroosmotic Flow Through a Microannulus,” Phyics of Fluids, 22, 042001 (2010).Google Scholar
22.Bird, R. B., Armstrong, R. C. and Hassager, O., Dynamics of Polymeric Liquids. Volume 1: Fluid Mechanics, 2nd Edition, John Wiley & Sons, Inc., New York (1987).Google Scholar
23.Bird, R. B., Stewart, W. E. and Lightfoot, E. N., Transport Phenomena, 2nd Edition, John Wiley & Sons, Inc., New York (2011).Google Scholar