Abstract

Electrophoresis of a tightly fitting sphere of radius $a$ along the centreline of a liquid-filled circular cylinder of radius $R$ is studied for a gap width $h_0=R-a\ll a$ . We assume a Debye length $\kappa ^{-1}\ll h_0$ , so that surface conductivity is negligible for zeta potentials typically seen in experiments, and the Smoluchowski slip velocity is imposed as a boundary condition at the solid surfaces. The pressure difference between the front and rear of the sphere is determined. If the cylinder has finite length $L$ , this pressure difference causes an additional volumetric flow of liquid along the cylinder, increasing the electrophoretic velocity of the sphere, and an analytic prediction for this increase is found when $L\gg R$ . If $N$ identical, well-spaced spheres are present, the electrophoretic velocity of the spheres increases with $N$ , in agreement with the experiments of Misiunas & Keyser (Phys. Rev. Lett., vol. 122, 2019, 214501).

Highlights

  • Analyses and computations of colloidal particle electrophoresis in a liquid-filled circular cylinder usually assume that the cylinder is infinitely long (Keh & Anderson 1985; Keh & Chiou 1996; Yariv & Brenner 2002, 2003; Hsu & Yeh 2007; Sherwood & Ghosal 2018)

  • The volumetric flow rate far from the particle is determined by the electroosmotic slip velocity created by the uniform electric field if the wall of the cylinder is charged

  • If several particles are present within a cylinder or channel of finite length, electrophoresis is faster than for a single particle (Misiunas & Keyser 2019)

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Summary

Introduction

Analyses and computations of colloidal particle electrophoresis in a liquid-filled circular cylinder usually assume that the cylinder is infinitely long (Keh & Anderson 1985; Keh & Chiou 1996; Yariv & Brenner 2002, 2003; Hsu & Yeh 2007; Sherwood & Ghosal 2018). Sherwood & Ghosal (2018) used a lubrication analysis to determine the electrophoretic velocity of a tightly fitting sphere inside an infinite cylinder They found a pressure difference Δp which was nominally O((R/h0)5/2), whereas the total force due to wall shear stresses was O((R/h0)3/2). A force balance on a cylindrical control volume containing the spherical particle was impossible in the limit h0/R → 0, unless the leading-order pressure difference Δp vanished, which required the electrophoretic velocity of the sphere to be USmol/2 This is the electrophoretic velocity in the limit h0/R → 0 determined analytically by Yariv & Brenner (2003) and numerically by Keh & Chiou (1996). The hydrodynamic problem is strongly dominated by the region of the narrow gap (more so than the electrostatic problem), and a solution in the narrow gap is all that we shall need

The Smoluchowski slip boundary conditions
Governing equations
The leading-order axial velocity u0
Second-order axial velocity u1
The electric field
The pressure field
Comparison with experiments
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