The quasi-steady diffusiophoresis
of a charged porous sphere situated
at the center of a charged spherical cavity filled with a liquid solution
of a symmetric electrolyte is analyzed. The porous particle can represent
a solvent-permeable and ion-penetrable polyelectrolyte molecule or
floc of nanoparticles in which fixed charges and frictional segments
are uniformly distributed, whereas the spherical cavity can denote
a charged pore involved in microfluidic or drug-delivery systems.
The linearized electrokinetic differential equations governing the
ionic concentration, electric potential, and fluid velocity distributions
in the system are solved by using a perturbation method with the fixed
charge density of the particle and the ζ-potential of the cavity
wall as the small perturbation parameters. An expression for the diffusiophoretic
(electrophoretic and chemiphoretic) mobility of the confined particle
with arbitrary values of a/b, κa, and λa is obtained in closed form,
where a and b are the radii of the
particle and cavity, respectively; κ and λ are the reciprocals
of the Debye screening length and the length characterizing the extent
of flow penetration into the porous particle, respectively. The presence
of the charged cavity wall significantly affects the diffusiophoretic
motion of the particle in typical cases. The diffusio-osmotic (electro-osmotic
and chemiosmotic) flow occurring at the cavity wall can substantially
alter the particle velocity and even reverse the direction of diffusiophoresis.
In general, the particle velocity decreases with an increase in a/b, increases with an increase in κa, and decreases with an increase in λa, but exceptions exist.