The structural features and the thermodynamics of melting of thermally reversible gels of
poly(diphenylsiloxane) (PDPhS) formed from 1.5 to 85 wt % solutions in diphenyl ether (DPhE) have
been studied by means of differential scanning calorimetry, X-ray diffraction, and electron scanning
microscopy. It was established that gelation occurs as a consequence of the crystallization of PDPhS that
leads to a specific spherulitic morphology; i.e., overlapped spherulite-like superstructures, which are
composed of lamellar crystallites, form a three-dimensional skeleton filled with the solvent. The phase
diagram of the PDPhS/DPhE system was constructed. Its particular feature, resulting from the crystal−mesophase transition in the undiluted PDPhS, is interference between the crystal−isotropic solution
and the thermotropic mesophase−isotropic solution equilibrium. The equilibrium temperature T
m° and
the heat Δ
H
m° of a virtual crystal−isotropic melt transition in PDPhS in the absence of solvent were
estimated (280 °C and 10.34 kJ mol-1) through use of the Flory equation when taking the melting
temperatures of the annealed gels as the equilibrium melting points of PDPhS crystals in the presence
of DPhE. The isotropization temperature (∼560 °C) of the mesophase, which cannot be measured
experimentally because of PDPhS thermal degradation, was assessed by extrapolation of the mesophase−isotropic solution boundary curve on the phase diagram of the PDPhS/DPhE system to the 100% polymer
concentration. Phase diagrams expected for the system solvent−crystalline flexible/semirigid-chain
polymer, exhibiting a crystal−mesophase transition, were schematically considered and compared to that
of the PDPhS/DPhE system. On the basis of this consideration, the conclusion was drawn that the
mesophase behavior of PDPhS is connected, at least in part, with a relatively high stiffness of its
macromolecules.