Clarkson University
The CAMP building
Of Interest
CRCD Home
ME 537 Home
Syllabus
Assignments
Downloads
Site Map
Course Notes
Engineering Mathematics
Review of Viscous Flows
Review of Computational Fluid Mechanics

Particle Adhesion
Simulation Methods
Experimental Techniques
Applications
Search Powered by Google

The National Science Foundation
ME 537 The National Science Foundation
 Particle Adhesion
Van der Waals Force | JKR and Other Adhesion Models | Particle Adhesion & Removal | Effects of Charge | Effect of Humidity | Ultrasonic and Megasonic Cleaning

Effects of Charge

Neighbor Forces Acting on Particle

Charged-Patch Model

Assume that the particle charge is localized to a discreet section of the particle

Electrostatic contribution to attractive force FE is given by

AC is the contact area

s is the charge density

Estimate of FVW

Note:These particles are irregularly-shaped

No silica:

Particle radius = 4mm

WA = 0.05 J/m2

q/m = 37 + 3 mC/g

r = 1.2 g/cm3

From JKR theory:

Measured value:FS = 970 nN

2% Silica:

Assume JKR contact radius = 196 nm

rsilica = 30 nm

rsilica = 1.75 g/cm3.

Þhave about 10 silica particles within the contact zone.

Approximate JKR removal force by

= 39 nN.

Measured:FS = 70 nN

Estimate of FIm:

Þ FIm = 20 – 40 nN

Estimate of FE:

Patch charge density limited by dielectric strength of air.

Þ FE » 30 nN

Key feature to note:If the particle has sufficient irregularity, van der Waals forces, electrostatic image forces, and charged-patch forces all predict about the same size force, which is comparable to experimentally determined detachment force.



Dr. Goodarz Ahmadi | Turbulence & Multiphase Fluid Flow Laboratory | Department of Mechanical & Aeronautical Engineering
Copyright © 2002-2005 Dr. Goodarz Ahmadi. All rights reserved.
Potsdam, New York, 13699
ahmadi@clarkson.edu