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

Citation
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
Citations number
27
Categorie Soggetti
Polymer Sciences
Journal title
ISSN journal
00249297
Volume
27
Issue
1
Year of publication
1994
Pages
164 - 170
Database
ISI
SICI code
0024-9297(1994)27:1<164:SPTFWH>2.0.ZU;2-C
Abstract
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.