2010
DOI: 10.1039/b921914e
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Simultaneous separation and detection of cations and anions on a microfluidic device with suppressed electroosmotic flow and a single injection point

Abstract: A rapid and simultaneous separation of cationic and anionic peptides and proteins in a glass microfluidic device that has been covalently modified with a neutral poly(ethylene glycol) (PEG) coating to minimize protein adsorption is presented. The features of the device allow samples that contain both anions and cations to be introduced from a central flow stream and separated in different channels with different outlets-all in the presence of low electroosmotic flow (EOF) imparted by the PEG coating. The analy… Show more

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Cited by 15 publications
(12 citation statements)
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“…In a subsequent article by Reschke et al [30], the glass microfluidic device for simultaneous cation and anion detection was modified. The device retained the single, hydrodynamically pumped sample stream, but separation and detection occurred in two separate channels, one for anions and one for cations.…”
Section: Separation Of Anions and Cationsmentioning
confidence: 99%
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“…In a subsequent article by Reschke et al [30], the glass microfluidic device for simultaneous cation and anion detection was modified. The device retained the single, hydrodynamically pumped sample stream, but separation and detection occurred in two separate channels, one for anions and one for cations.…”
Section: Separation Of Anions and Cationsmentioning
confidence: 99%
“…Reschke et al from West Virginia University described devices that were used for the separation of ions [29,30]. In the first article, a glass microfluidic device where flow is controlled by electrophoresis was used for anion and cation separation and detection [29].…”
Section: Separation Of Anions and Cationsmentioning
confidence: 99%
“…We review the sinusoidal model that has been studied previously [2,6,7], introduce traveling-electrode and stationary-electrode models, and show that only the stationary-electrode model produces plateaus. Experiments [3][4][5] have observed localization and trapping thresholds as predicted by the 2D model [2,3], but have not yet observed velocity plateaus. These plateaus might just be observable in careful experiments, but their physical origin is unclear.…”
mentioning
confidence: 99%
“…For low mobilities R < R l , particles are confined to the locality of electrodes and u = 0. For high mobilities R > R t , particles are trapped by the wave and u = c. As R increases from the localization threshold R l to the trapping threshold [2][3][4][5], with channel height h and four electrodes per wavelength, λ. These electrodes are held at the AC potentials Φ0(t), Φ1(t), Φ2(t), and Φ3(t), each potential differing in phase by 90…”
mentioning
confidence: 99%
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