Abstract

How to describe the ``electric double layer'' that is at the root of all electrokinetic phenomena such as electrophoresis and electro-osmosis? A new theoretical approach, introducing the concept of a surface potential trap and applying the constraint of global charge neutrality rigorously, answers this century-old question in the context of contemporary electrokinetics involving nanoscale systems and time-dependent electric fields.

Highlights

  • Electrokinetics (EK) is a classic subject that dates back nearly two centuries [1]

  • The consistency requirement leads to the charge-conserving Poisson-Boltzmann (CCPB) equation, which guarantees charge neutrality

  • (2) A crucial element of our model is the introduction of a surface potential trap that attributes an energy cost to the interfacial charge dissociation process

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Summary

INTRODUCTION

Electrokinetics (EK) is a classic subject that dates back nearly two centuries [1]. It involves the interaction of ions in the fluid with the solid surface, and their dynamics under an applied electric field tangential to the fluid-solid interface. The resulting treatment is not mathematically self-contained This can be a problem in treating nanoscale or time-varying electrokinetics, for example, since the interfacial charge layer would necessarily respond to the local fluid conditions, either as a function of time or as a function of separation between two charged surfaces, thereby requiring constant hands-on corrections for achieving charge neutrality. Experimental evidences, mainly obtained from atomic-force-microscope measurements, have indicated a variation of the surface charge density when the channel width decreases below the Debye length, which does not agree with the predictions resulting from either the CP or the CC boundary condition This discrepancy is generally attributed to the “charge regulation” phenomenon, denoting the fact that the interfacial charge layer must vary as a function of local environment. IX with a summary of the main points, and note the challenges ahead

Poisson-Nernst-Planck equations
Static limit of the PNP equations—the Poisson-Boltzmann model
Physical picture of Gouy-Chapman
Inconsistencies between the PB equation and the PNP equations
Charge-conserving Poisson-Boltzmann equation
Surface potential trap model
Generalization to the case of surface nonspecific salt ion addition
Reduction to the PB equation form
Generalized definition of the ζ potential
Comparison and contrast with the traditional picture
COMPARISON WITH ALTERNATIVE MODELS AND EXPERIMENTS
FORCE BETWEEN TWO CHARGED SURFACES
Coupling to the Navier-Stokes equation
Definition of the time-dependent model
Electro-osmotic effect and its time dependence
VIII. ONSAGER RELATION
Findings
SUMMARY AND CONCLUDING REMARKS
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