Fractionation of cell mixtures using acoustic and laminar flow fields

Manoj Kumar; Donald L. Feke; Joanne M. Belovich

doi:10.1002/bit.20294

Fractionation of cell mixtures using acoustic and laminar flow fields

Biotechnology and Bioengineering ◽

10.1002/bit.20294 ◽

2004 ◽

Vol 89 (2) ◽

pp. 129-137 ◽

Cited By ~ 39

Author(s):

Manoj Kumar ◽

Donald L. Feke ◽

Joanne M. Belovich

Keyword(s):

Laminar Flow ◽

Flow Fields

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Fractionation of fine particle suspensions by coordinated planar ultrasonic and laminar flow fields in a rectangular acoustic chamber.

The Journal of the Acoustical Society of America ◽

10.1121/1.403442 ◽

1992 ◽

Vol 91 (4) ◽

pp. 2353-2353

Author(s):

Z. I. Mandralis ◽

D. L. Feke

Keyword(s):

Laminar Flow ◽

Fine Particle ◽

Flow Fields ◽

Particle Suspensions ◽

Acoustic Chamber

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Electrocoalescence of water droplet trains in sunflower oil under the coupling of Non-uniform electric and Laminar flow fields

Chemical Engineering Science ◽

10.1016/j.ces.2021.117158 ◽

2022 ◽

Vol 248 ◽

pp. 117158

Author(s):

Bin Li ◽

Xiaohui Dou ◽

Kai Yu ◽

Wei Zhang ◽

Haojie Xu ◽

...

Keyword(s):

Laminar Flow ◽

Sunflower Oil ◽

Water Droplet ◽

Flow Fields

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Laminar Flow Fields

Transport Phenomena in Multiphase Flows - Fluid Mechanics and Its Applications ◽

10.1007/978-3-319-15793-1_5 ◽

2015 ◽

pp. 75-95

Author(s):

Roberto Mauri

Keyword(s):

Laminar Flow ◽

Flow Fields

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Steady Laminar Fluid Flow Through Variable Constrictions in Vascular Tube

Journal of Fluids Engineering ◽

10.1115/1.2910244 ◽

1994 ◽

Vol 116 (1) ◽

pp. 66-71 ◽

Cited By ~ 27

Author(s):

T. S. Lee

Keyword(s):

Reynolds Number ◽

Fluid Flow ◽

Laminar Flow ◽

Recirculation Zone ◽

Flow Fields ◽

Laminar Fluid Flow ◽

Spacing Ratio ◽

Flow Through ◽

Steady Laminar

Steady laminar flow fields in the neighborhoods of two consecutive constrictions in a vascular tube were studied for approaching Reynolds number Re in the range of 5 to 200. The upstream stenosis was set at a dimensionless diameter constriction c1 of 0.5 while the downstream stenoses were allowed to vary from c2 = 0.2 to 0.6. The proximity of the constrictions was determined by the spacing ratio of S/D = 1, 2, 3, and ∞. When c2 > c1, a recirculation zone filled the valley between the two constrictions with little changes to the separation and reattachment points as Re was further increased. For c2 < c1 and when Re was increased, the recirculating eddy formed downstream of the first constriction tended to spread beyond the region of the second constriction. This resulted in negative wall vorticity peak occurring in the region of the second constriction for smaller S/D at high Re.

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