3. EDL over an infinite cylinder: Consider a infinitely long cylinder of radius Ro. The cylinder is negativelycharged at its surface. The cylinder is in contact with an symmetric electrolyte solution. Assumingaxisymmetry and low potential (i.e. dimensionless y « 1), obtain a linear differential equation for thedimensionless potential. Solve the resulting dimensionless problem for the potential distribution. Hint:The governing equation can be modified to Bessel's equation.

Surface forces are the integral form of interaction forces between surfaces of macroscopic things…

3. EDL over an infinite cylinder: Consider a infinitely long cylinder of radius Ro. The cylinder is negatively charged at its surface. The cylinder is in contact with an symmetric electrolyte solution. Assuming axisymmetry and low potential (i.e. dimensionless p « 1), obtain a linear differential equation for the dimensionless potential. Solve the resulting dimensionless problem for the potential distribution. Hint: The governing equation can be modified to Bessel's equation.

3. EDL over an infinite cylinder: Consider a infinitely long cylinder of radius Ro. The cylinder is negatively charged at its surface. The cylinder is in contact with an symmetric electrolyte solution. Assuming axisymmetry and low potential (i.e. dimensionless p « 1), obtain a linear differential equation for the dimensionless potential. Solve the resulting dimensionless problem for the potential distribution. Hint: The governing equation can be modified to Bessel's equation.

Principles of Heat Transfer (Activate Learning with these NEW titles from Engineering!)

8th Edition

ISBN:9781305387102

Author:Kreith, Frank; Manglik, Raj M.

Publisher:Kreith, Frank; Manglik, Raj M.

Chapter3: Transient Heat Conduction

Section: Chapter Questions

Problem 3.1P: Consider a flat plate or a plane wall with a thickness L and a long cylinder of radius r0. Both of...

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