Abstract

Standard DEP theory, based on the Clausius–Mossotti (CM) factor derived from solving the boundary-value problem of macroscopic electrostatics, fails to describe the dielectrophoresis (DEP) data obtained for 22 different globular proteins over the past three decades. The calculated DEP force appears far too small to overcome the dispersive forces associated with Brownian motion. An empirical theory, employing the equivalent of a molecular version of the macroscopic CM-factor, predicts a protein’s DEP response from the magnitude of the dielectric β-dispersion produced by its relaxing permanent dipole moment. A new theory, supported by molecular dynamics simulations, replaces the macroscopic boundary-value problem with calculation of the cross-correlation between the protein and water dipoles of its hydration shell. The empirical and formal theory predicts a positive DEP response for protein molecules up to MHz frequencies, a result consistently reported by electrode-based (eDEP) experiments. However, insulator-based (iDEP) experiments have reported negative DEP responses. This could result from crystallization or aggregation of the proteins (for which standard DEP theory predicts negative DEP) or the dominating influences of electrothermal and other electrokinetic (some non-linear) forces now being considered in iDEP theory.

Highlights

  • The subject of protein dielectrophoresis (DEP) is at an important stage where a maturing theory, supported by molecular dynamics (MD) simulations of solvated proteins [1] has clarified aspects that have largely remained unresolved since the pioneering studies reported in 1994 by Washizu et al [2]

  • The applied electric fields and field gradients are in many cases far too weak to generate DEP forces capable of overcoming the thermal (Brownian) force acting on a protein molecule [3,4,5]

  • RNA, for example? Or perhaps each class of biomolecule will present its own particular challenge? Based on an empirical theory, it was proposed that the DEP response of a globular protein can be predicted from the magnitude and frequency profile of its dielectric β-dispersion, which reflects the protein’s squared dipole moment and its relaxation time [4]

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Summary

Introduction

The subject of protein dielectrophoresis (DEP) is at an important stage where a maturing theory, supported by molecular dynamics (MD) simulations of solvated proteins [1] has clarified aspects that have largely remained unresolved since the pioneering studies reported in 1994 by Washizu et al [2]. The new theory takes into account the polarization of the protein’s hydration shell induced by the protein’s permanent dipole moment These should be considered as generic aspects for molecular DEP, and highlight the importance of dielectric spectroscopy and MD simulations going forward. Researchers engaged in eDEP, where conductive electrodes generate the required field gradient, have tended to follow these guidelines In such cases, there are consistent reports of a positive DEP response observed for the 22 different proteins so far studied [4], in line with the new theory plus MD simulations [1] and as predicted by the empirical theory [4]. The possibility that field-driven protein aggregation can occur at a threshold of protein concentration, which may provide new opportunities of exploitation, merits further consideration under the category of ‘Something Else’

Limitations of Macroscopic Electrostatics with Respect to Protein DEP
The β- and δ-Dispersions Associated with Protein Hydration
Summary of Dielectric Theory of Relevance to Protein DEP
Maximum Size of a Lorentz Cavity
Fröhlich’s Theory Relating Permittivity and Spontaneous Polarization
South and Grant’s Theory of Protein Dipole Relaxation
The Theory
Molecular Dynamics Studies
Something Else?
Findings
Concluding Comments

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