2010
DOI: 10.1016/j.jcis.2010.03.039
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Wall-induced lateral migration in particle electrophoresis through a rectangular microchannel

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Cited by 73 publications
(74 citation statements)
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References 58 publications
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“…In contrast, 3 mm particles entered into the serpentine section in an already focused stream along the channel centerline. This happened mainly due to the wall-induced lateral migration as demonstrated recently by Liang et al [37]. Moreover, since they experienced a much larger dielectrophoretic force than 1 mm particles, 3 mm particles were deflected past the channel centerline to the outer sidewall.…”
Section: Resultsmentioning
confidence: 83%
“…In contrast, 3 mm particles entered into the serpentine section in an already focused stream along the channel centerline. This happened mainly due to the wall-induced lateral migration as demonstrated recently by Liang et al [37]. Moreover, since they experienced a much larger dielectrophoretic force than 1 mm particles, 3 mm particles were deflected past the channel centerline to the outer sidewall.…”
Section: Resultsmentioning
confidence: 83%
“…It has become one of the most promising techniques for the delivery and manipulation of colloidal particles in lab-on-a-chip devices in the absence of complicated moving components [1]. So far, extensive theoretical analysis [2][3][4][5][6][7][8][9][10][11][12] and experimental studies [8,10,[13][14][15][16][17] have been performed on the electrokinetic particle translocation in microchannels.…”
Section: Introductionmentioning
confidence: 99%
“…We approximate diffusion as negligible (Pe, the P eclet number, ) 1), particle inertial effects as small compared to the fluid and DEP forces (St, the Stokes number, ( 1), and neglect the wall-induced particle migration effects observed in long microchannels. [34][35][36] (As the length of the constriction between adjacent obstacles is on the order of the obstacle diameter, 2a ¼ 100 lm.) In the absence of DEP forces, each cell acts as a Lagrangian tracer, passively following the fluid streamlines unless the cell contacts an obstacle, at which time a no-penetration condition is enforced using an ad hoc quadratic penalty function designed to mimic the compression of a deformable sphere.…”
Section: Cell Transport Simulationsmentioning
confidence: 99%