Microfluidics and Miniaturization
Analyte transport past a nanofluidic intermediate electrode junction in a microfluidic device
Article first published online: 23 JUL 2010
DOI: 10.1002/elps.201000068
Copyright © 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
Issue

ELECTROPHORESIS
Special Issue: INSTRUMENTATION FOR CE AND MICROCHIP-CE
Volume 31, Issue 15, pages 2686–2694, August 2010
Additional Information
How to Cite
Mao, X., Reschke, B. R. and Timperman, A. T. (2010), Analyte transport past a nanofluidic intermediate electrode junction in a microfluidic device. ELECTROPHORESIS, 31: 2686–2694. doi: 10.1002/elps.201000068
Publication History
- Issue published online: 23 JUL 2010
- Article first published online: 23 JUL 2010
- Manuscript Accepted: 9 MAY 2010
- Manuscript Revised: 6 MAY 2010
- Manuscript Received: 8 FEB 2010
Funded by
- NSF RII award EPS. Grant Number: 0554328
- WV EPSCoR Office
- WVU Research Corporation
- Abstract
- Article
- References
- Cited By
Keywords:
- Current sink;
- Electrode junction;
- Microfluidics;
- Nanofluidic
Abstract
A glass microfluidic device is presented in which a microchannel is split into two regions with different electric fields by a nanochannel intermediate electrode junction formed by dielectric breakdown. The objective is to sink current through the nanochannel junction without sample loss or broadening of the band as it passes the junction. This type of performance is desired in many microfluidic applications, including the coupling of microchannel/CE with ESI-MS, electrochemical detection, and electric field gradient focusing. The voltage offsets in this study are suitable for microchannel/CE-ESI-MS. Imaging of the transport of model anions and cations through the junction indicates that the junction exhibits nanofluidic behavior and the mean depth of the nanochannel is estimated to be ∼105 nm. The ion permselectivity of the nanochannel induces concentration polarization and enriched and depleted concentration polarization zones form on opposite sides of the nanochannel, altering the current and electric field distributions along the main microchannel. Anion transport efficiency past the junction was high, 96.0%, and varied little over the pH range of 4.0–8.0. In contrast, cation transport is much lower, and decreases from 72 to 11% from pH 4.0 to 8.0. Band broadening increases with increasing pH less than 70% over the pH range of 4.0–8.0. It is anticipated that this characterization will aid in the understanding and optimization of such junctions made from permselective membranes and porous glass.

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