Cornell University - Visit www.cornell.edu Kirby Research Group at Cornell: Microfluidics and Nanofluidics : - Home College of Engineering - visit www.engr.cornell.edu Cornell University - Visit www.cornell.edu
Cornell University, College of Engineering Search Cornell
News Contact Info Login
Copyright Brian J. Kirby. With questions, contact Prof. Kirby here. This material may not be distributed without the author's consent. When linking to these pages, please use the URL http://www.kirbyresearch.com/textbook.

This web posting is a draft, abridged version of the Cambridge University Press text. Follow the links to buy at Cambridge or Amazon or Powell's or Barnes and Noble. Contact Prof. Kirby here. Click here for the most recent version of the errata for the print version.

[Return to Table of Contents]


Jump To: [Kinematics] [Couette/Poiseuille Flow] [Fluid Circuits] [Mixing] [Electrodynamics] [Electroosmosis] [Potential Flow] [Stokes Flow] [Debye Layer] [Zeta Potential] [Species Transport] [Separations] [Particle Electrophoresis] [DNA] [Nanofluidics] [Induced-Charge Effects] [DEP] [Solution Chemistry]

13.5 Exercises [particle electrophoresis top]

  1. The Smoluchowski limit (thin double layer limit) for electrophoresis of a cylinder aligned perpendicular to the electric field with thin double layers is
    microfluidics textbook nanofluidics textbook Brian Kirby Cornell
    (13.33)

    while the Hückel limit (thick double layer limit) for electrophoresis of a cylinder aligned perpendicular to the electric field with thick double layers is
    microfluidics textbook nanofluidics textbook Brian Kirby Cornell
    (13.34)

    Consider the solution for the electric field around an insulating cylinder (which is the superposition of a uniform field and a dipole), and evaluate the maximum electric field on the surface in this case as compared to the bulk electric field. In the case of thin double layers, this maximum electric field is applied to the ions in the double layer, and gives rise to the particle motion relative to the fluid. In the case of thick double layers, the field applied to the ions in the double layer is for the most part the bulk electric field. Draw a schematic of these two cases and explain why the electrophoretic velocities in these two cases differ by 12.

  2. Plot the exact and approximate relations for Henry’s functions for spheres and cylinders. Plot a* on a log scale from 1×10-2 to 1×103. Estimate the maximum error of the approximate functions.
  3. Most exercises are excluded from this web posting. Follow the links to buy the text at Cambridge or Amazon or Powell's or Barnes and Noble.

[Return to Table of Contents]



Jump To: [Kinematics] [Couette/Poiseuille Flow] [Fluid Circuits] [Mixing] [Electrodynamics] [Electroosmosis] [Potential Flow] [Stokes Flow] [Debye Layer] [Zeta Potential] [Species Transport] [Separations] [Particle Electrophoresis] [DNA] [Nanofluidics] [Induced-Charge Effects] [DEP] [Solution Chemistry]

Copyright Brian J. Kirby. Please contact Prof. Kirby here with questions or corrections. This material may not be distributed without the author's consent. When linking to these pages, please use the URL http://www.kirbyresearch.com/textbook.

This web posting is a draft, abridged version of the Cambridge University Press text. Follow the links to buy at Cambridge or Amazon or Powell's or Barnes and Noble. Contact Prof. Kirby here. Click here for the most recent version of the errata for the print version.