SCALED PARTICLE THEORY FOR WORMLIKE HARD SPHEROCYLINDERS - CALCULATION OF PHASE-DIAGRAMS FOR TERNARY-SYSTEMS CONSISTING OF 2 SEMIFLEXIBLE POLYMERS WITH DIFFERENT LENGTHS AND A SOLVENT
T. Sato et al., SCALED PARTICLE THEORY FOR WORMLIKE HARD SPHEROCYLINDERS - CALCULATION OF PHASE-DIAGRAMS FOR TERNARY-SYSTEMS CONSISTING OF 2 SEMIFLEXIBLE POLYMERS WITH DIFFERENT LENGTHS AND A SOLVENT, Macromolecules, 27(1), 1994, pp. 164-170
We extended the scaled particle theory of Cotter and Wacker for multic
omponent systems of straight hard spherocylinders to multicomponent so
lutions of wormlike hard spherocylinders and calculated phase diagrams
of ternary systems consisting of two homologous semiflexible polymer
components with different lengths and a low molar mass good solvent. T
he basic parameters in this theory are the chain contour lengths (L(1)
, L(2)), the hard core diameter (d), and the persistence length (q) of
the polymer components. The theoretical ternary phase diagrams calcul
ated by this scaled particle theory for wormlike hard spherocylinders
were compared with experimental ternary phase diagrams obtained previo
usly for systems of schizophyllan + water and poly(n-hexyl isocyanate)
+ toluene. When the hard core diameter d was chosen to have a value c
lose to that estimated from the osmotic pressure or solvent chemical p
otential data for the corresponding binary solutions, good agreements
between experimental and theoretical ternary phase diagrams were obtai
ned for the isotropic-anisotropic binodal curves and the tie lines of
all the systems compared. On the other hand, the present theory failed
to predict anisotropic-anisotropic-isotropic three-phase coexistence
as well as anisotropic-anisotropic two-phase coexistence in ternary so
lutions containing two samples with the Kuhn segment numbers N-1 (drop
L(1)/2q) = 0.930 and N-2 (drop L(2)/2q) = 0.0765, whereas these multi
phase separations were found for aqueous solutions of schizophyllan wi
th the same N-i's. When N-2 was decreased to smaller than 0.07 with N-
1 kept at 0.93, these phase-coexisting regions appeared in the theoret
ical phase diagram.