Lyotropic
solutions containing two types of semiflexible macromolecules
in spherical confinement are studied by molecular dynamics simulations
and density functional theory, using a coarse-grained model. The case
of strong stiffness disparity between both types of polymers is treated,
and for simplicity, we take the contour lengths of both types of polymers
to be equal. Only sphere radii larger than this contour length are
considered, so that many chains can be packed inside the sphere, even
when the chains are stretched out in a nematic state. For the chosen
polymer solution, in the bulk one finds with increasing monomer concentration
a transition from an isotropic phase through an isotropic–nematic
two-phase region to a homogeneous nematic phase to which both constituents
contribute. In the corresponding confined systems, there is an interplay
between these phase transitions and surface enrichment of one component
(typically, but not always, the stiffer one). In rather dilute confined
solutions, the main effect of the surfaces is that the random orientation
of the end-to-end vectors of the stiff chains is perturbed in a surface
shell whose thickness is roughly the contour length. In more concentrated
systems, a thin layer of wall-attached stiff chains is observed in
addition, while (for equal mole fractions of both constituents) the
stiffer component can also form an almost cylindrical domain with
a bipolar orientational order, surrounded in the remainder of the
sphere by the less stiff component. Topological defects in the nematic
order can be identified, similar to the case where a single type of
semiflexible polymer is confined in a sphere. The radial profiles
of monomer concentrations and of various order parameters are compared
to analogous data near planar and cylindrical repulsive walls, to
provide a comprehensive picture of confinement effects on such polymer
solutions.