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Abstracts and Talk Materials
Mathematics of Microfluidic Transport Phenomena
December 05-06, 2009


Shelley Anna - Carnegie Mellon University
http://www.me.cmu.edu/default.aspx?id=anna

An Introduction to interfaces and multiphase flows in microfluidics
December 06, 2009 2:00 pm - 3:30 pm


Martin Bazant - Massachusetts Institute of Technology
http://web.mit.edu/bazant/www/

Induced-charge electrokinetics
December 06, 2009 4:00 pm - 5:30 pm


Sandip Ghosal - Northwestern University
http://ghosal.mech.northwestern.edu/

Electroosmotic flow and dispersion in microfluidics
December 05, 2009 2:00 pm - 3:30 pm


Susan Muller - University of California, Berkeley
http://www.cchem.berkeley.edu/sjmgrp/

Confinement effects with macromolecules
December 06, 2009 10:45 am - 12:15 pm


Ali Nadim - Claremont Graduate University
http://wfs.cgu.edu/nadima/home

Electrowetting and digital microfluidics
December 06, 2009 9:00 am - 10:30 am

In this tutorial, a number of approaches to mathematical modeling of electrowetting-on-dielectric (EWOD), also known as digital microfluidics (DMF) will be reviewed. EWOD refers to methods for causing droplets to move along solid surfaces or changing the shapes of attached drops (e.g., to actuate a liquid lens) by applying a potential difference between the drop and an underlying electrode, separated from the conducting drop via a thin dielectric layer. The main equation describing electrowetting is known as the Young-Lippmann (YL) equation, which provides a relationship between the local contact angle of the drop and the square of the potential difference. In this tutorial, a simple derivation of the YL equation is provided based on an energy minimization principle. We will then introduce both lumped and field models to characterize the electrostatic forces acting on a drop as a function of its position relative to the underlying electrodes. The lumped model is based simply on treating the dielectric layer as a parallel-plate capacitor and considering the changes in the energy of the system as a function of the location of the drop. The field model requires the use of concepts from electromechanics, including Maxwell's electric stress tensor. We will consider both DC and AC electric potentials and describe how to analyze the system in both cases.

David Saintillan - University of Illinois at Urbana-Champaign
http://mechse.illinois.edu/research/dstn/

Electrokinetic phenomena in particulate suspensions: an introduction
December 05, 2009 10:45 am - 12:15 pm


Todd Squires - University of California, Santa Barbara
http://www.chemengr.ucsb.edu/people/faculty_d.php?id=5

Electrokinetics of highly charged surfaces
December 05, 2009 9:00 am - 10:30 am


Boris Zaltzman - Jacob Blaustein Institute for Desert Research

Electric double layer and concentration polarization
December 05, 2009 4:00 pm - 5:30 pm


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