Induced-Charge Electrokinetic Phenomena Martin Z. Bazant Department of Mathematics, MIT ESPCI-PCT & CNRS Gulliver Paris-Sciences Chair Lecture Series 2008, ESPCI 1. Introduction (7/1) 2. Induced-charge electrophoresis in colloids (10/1) 3. AC electro-osmosis in microfluidics (17/1) 4. Theory at large applied voltages (14/2)
Paris-Sciences Chair Lecture Series 2008, ESPCI. Induced-Charge Electrokinetic Phenomena. Introduction ( 7/1) Induced-charge electrophoresis in colloids (10/1) AC electro-osmosis in microfluidics (17/1) Theory at large applied voltages (14/2). Martin Z. Bazant - PowerPoint PPT Presentation
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Induced-Charge Electrokinetic Phenomena
Martin Z. BazantDepartment of Mathematics, MIT
ESPCI-PCT & CNRS Gulliver
Paris-Sciences Chair Lecture Series 2008, ESPCI
1. Introduction (7/1)
2. Induced-charge electrophoresis in colloids (10/1)
FORMERPhD: Jeremy Levitan, Kevin Chu (2005),Postodocs: Yuxing Ben (2004-06)Interns: Kapil Subramanian, Andrew Jones, Brian Wheeler, Matt Fishburn, Jacub KominiarczukCollaborators: Todd Squires (UCSB), Vincent Studer (ESPCI), Martin Schmidt (MIT),Shankar Devasenathipathy (Stanford)
Funding: • Army Research Office• National Science Foundation• MIT-France Program• MIT-Spain Program
Acknowledgments
Outline
1. Electrokinetic microfluidics2. ICEO mixers3. AC electro-osmotic pumps
Electro-osmosis
Slip:
Potential / plug flow for uniformly charged walls:
Electro-osmotic Labs-on-a-Chip
• Apply E across chip
• Advantages– EO plug flow has low
hydrodynamic dispersion– Standard uses of in
separation/detection
• Limitations: – High voltage (kV)– No local flow control – “Table-top technology”
Pressure generation by slip
Use small channels!
DC Electro-osmotic Pumps• Nanochannels or porous media
can produce large pressures (0.1-50 atm)
• Disadvantages: – High voltage (kV)– Faradaic reactions – Gas management– Hard to miniaturize
Yau et al, JCIS (2003)Juan Santiago’s group at Stanford
Porous Glass
Electro-osmotic mixing
• Non-uniform zeta produces vorticity• Patterned charge + grooves can also
drive transverse flows (Ajdari 2001) which allow lower voltage across a channel
• BUT – Must sustain direct current– Flow is set by geometry, not “tunable”
Outline
1. Electrokinetic microfluidics2. ICEO mixers3. AC electro-osmotic pumps
Induced-Charge Electro-osmosisGamayunov, Murtsovkin, Dukhin, Colloid J. USSR (1986) - flow around a metal sphereBazant & Squires, Phys, Rev. Lett. (2004) - general theory, broken symmetries, microfluidics
Example: An uncharged metal cylinder in a DC (or AC) field
Can generate vorticity and pressure with AC fields
• Disadvantages• small pressure (<< Pa)• low salt concentration
ICEO-based microfluidic mixing(C. K. Harnett, University of Louisville/M.P. Kanouff, Sandia National Laboratories)
•(a) Simulation of dye loading in the mixing channel by pressure-driven flow. Some slow diffusional mixing is seen.
•(b) Simulation of fast mixing after loading, when sidewall electrodes are energized.
•(c) Simulated velocity field surrounding the triangular posts when sidewall electrodes are energized.
•(d) Microfabricated device consisting of vertical gold-coated silicon posts and sidewall electrodes in an insulating channel. (Channel width 200 um, depth 300 um)
Features in flow images (top row) are replicated in the model (bottom row)•without electric field (a) (b)•and with electric field applied between channel sidewalls (c), (d).
ICEO-based microfluidic mixing(C. K. Harnett, University of Louisville/M.P. Kanouff, Sandia National Laboratories)
Comparison of experimental (a,c) and calculated (b,d) results during steady flow of dyed and un-dyed solutions (2 l/min combined flow rate) without power (a,b) and with power (c,d). Flow is from left to right. 10 Vpp, 37 Hz square wave applied across 200 um wide channel. Left-right transit time ~2 s.
ICEO-based microfluidic mixing(C. K. Harnett, University of Louisville/M.P. Kanouff, Sandia National Laboratories)
Power Off:Incompletediffusionalmixing
Power On:CompleteICEO-basedmixing
experimental
experimental
calculated
calculated
“Fixed-Potential ICEO”
Example: metal cylinder grounded to an electrode supplying an AC field.
Fixed-potential ICEO mixer
Idea: Vary the induced total charge in phase with the local field.
Squires & Bazant, J. Fluid Mech. (2004)
Generalizes “Flow FET” ofGhowsi & Gale, J. Chromatogr. (1991)
QuickTime™ and aDV/DVCPRO - NTSC decompressor
are needed to see this picture.
Flow past a 20 micron electroplated gold post (J. Levitan, PhD Thesis 2005)
Outline
1. Electrokinetic microfluidics2. Induced-charge mixers3. AC electro-osmotic pumps
AC electro-osmosisA. Ramos, A. Gonzalez, A. Castellanos (Sevilla), N. Green, H. Morgan (Southampton), 1999.
Circuit modelRamos et al. (1999)
Debye time:
“RC time”
ICEO flow over electrodes
• Example: response to a sudden DC voltage• ACEO flow peaks if period = charging time• Maximizes flow/voltage due to large field
AC electro-osmotic pumpsAjdari (2000)
“Ratchet” concept inspired by molecular motors:
Broken local symmetry in a periodic structure with “shaking” causes pumpingwithout a global gradient.