When a charged particle translates
through an electrolyte solution,
the electric double layer around it deforms in response to the fluid
motion and creates an electric force opposite the direction of motion,
decreasing the settling velocity. This is a multidisciplinary phenomenon
that combines fluid mechanics and electrodynamics, differentiating
it from the classical problem of an uncharged sedimenting particle.
It has many applications varying from mechanical to biomedical, such
as in drug delivery in blood through charged microparticles. Related
studies so far have focused on Newtonian fluids, but recent studies
have proven that many biofluids, such as human blood plasma, have
elastic properties. To this end, we perform a computational study
of the steady sedimentation of a spherical, charged particle in human
blood plasma due to the centrifugal force. We used the Giesekus model
to describe the rheological behavior of human blood plasma. Assuming
axial symmetry, the governing equations include the momentum and mass
balances, Poisson’s equation for the electric field, and the
species conservation. The finite size of the ions is considered through
the local-density approximation approach of Carnahan–Starling.
We perform a detailed parametric analysis, varying parameters such
as the ζ potential, the size of the ions, and the centrifugal
force exerted upon the particle. We observe that as the ζ potential
increases, the settling velocity decreases due to a stronger electric
force that slows the particle. We also conduct a parametric analysis
of the relaxation time of the material to investigate what happens
generally in viscoelastic electrolyte solutions and not only in human
blood plasma. We conclude that elasticity plays a crucial role and
should not be excluded from the study. Finally, we examine under which
conditions the assumption of point-like ions gives different predictions
from the Carnahan–Starling approach.