Critical behavior of polystyrene-cyclohexane: Heat capacity and mass density
Annotatsiya
At temperatures between $7.5\text{ }\ifmmode^\circ\else\textdegree\fi{}\text{C}$ and $20\text{ }\ifmmode^\circ\else\textdegree\fi{}\text{C}$ as well as $26\text{ }\ifmmode^\circ\else\textdegree\fi{}\text{C}$ and $40\text{ }\ifmmode^\circ\else\textdegree\fi{}\text{C}$ we have recorded the densities and specific heat at constant pressure for critical mixtures of polystyrene in cyclohexane. The degrees of polymerization were $N=288$ (critical temperature ${T}_{c}=9.77\text{ }\ifmmode^\circ\else\textdegree\fi{}\text{C}$) and $N=6242$ $({T}_{c}=27.56\text{ }\ifmmode^\circ\else\textdegree\fi{}\text{C})$, respectively. In the two-phase regime a series of reproducible events exists in the specific-heat traces, indicating the existence of nonequilibrium intermediate states as likely resulting from an oscillatory instability of droplet formation. In the one-phase region the critical contribution to the heat capacity follows power law with critical exponent $\ensuremath{\alpha}=0.11$ compatible with Ising-like criticality. At larger $N$, however, the critical amplitude of the heat capacity is noticeably smaller than at lower degree of polymerization. This finding may be taken as an indication of different effects from competing mesoscale lengths: the radius of gyration of the polymer and the fluctuation correlation length of the mixture. The density traces reveal marginal deviations from simple linear temperature dependencies. If these deviations are analyzed in terms of critical contributions, different signs in the amplitude result, in conformity with the signs in the pressure dependence of the critical temperature. The absolute values of the amplitudes, however, are substantially larger than predicted from the critical amplitudes of the heat capacities.