Gelation, crystallization and morphological transformations of syndiotactic polystyrene in acetophenone and acetophenone + carbon dioxide mixtures at high pressures

The gelation and crystallization processes in 5 wt% solutions of syndiotactic polystyrene in acetophenone and acetophenone + carbon dioxide fluid mixtures were studied in a variable-volume view-cell system over a pressure range from 7 to 50 MPa for CO2 concentrations up to 40 wt%. The solution in pure acetophenone displayed only a sol–gel (gelation) phase boundary. Solutions containing 25 wt% CO2 displayed both a sol–gel and a liquid–liquid phase boundary. Solutions containing 40% CO2 displayed instead a fluid–solid (crystallization) and a liquid–liquid phase boundary. The consequences of crossing the gelation, crystallization or the liquid–liquid demixing boundaries first on the eventual morphology and the crystal structures that develop were investigated. It is shown that when the gelation boundary is crossed first, the resulting crystal structure is the δ form. When the L–L phase boundary is crossed first, polymer-rich phase leads to a mixture of δ + β crystal forms while only the δ form is found in the polymer-lean phase from solutions with 25 wt% CO2. Crossing the crystallization boundary first in solutions with 40 wt% CO2, leads to the β form with no presence of the δ crystal form. However, when the liquid–liquid phase boundary is crossed first, the polymer-rich phase forms only the β crystal form and the polymer-lean phase leads to a mixed crystal structure containing the β and δ forms. Formation of the different crystal structures are verified by XRD, FTIR and SEM characterizations and are rationalized with a phase diagram describing the paths the system follows as a result of a change in pressure and/or the temperature.

The gelation and crystallization processes in 5 wt% solutions of syndiotactic polystyrene in acetophenone and acetophenone + carbon dioxide fluid mixtures were studied in a variable-volume view-cell system over a pressure range from 7 to 50 MPa for CO2 concentrations up to 40 wt%. The solution in pure acetophenone displayed only a sol–gel (gelation) phase boundary. Solutions containing 25 wt% CO2 displayed both a sol–gel and a liquid–liquid phase boundary. Solutions containing 40% CO2 displayed instead a fluid–solid (crystallization) and a liquid–liquid phase boundary. The consequences of crossing the gelation, crystallization or the liquid–liquid demixing boundaries first on the eventual morphology and the crystal structures that develop were investigated. It is shown that when the gelation boundary is crossed first, the resulting crystal structure is the δ form. When the L–L phase boundary is crossed first, polymer-rich phase leads to a mixture of δ + β crystal forms while only the δ form is found in the polymer-lean phase from solutions with 25 wt% CO2. In solutions with 40 wt% CO2, crossing the crystallization boundary first leads to the β form with no presence of the δ crystal form. However, when the liquid–liquid phase boundary is crossed first, the polymer-rich phase forms only the β crystal form and the polymer-lean phase leads to a mixed crystal structure containing the β and δ forms. Formation of the different crystal structures are verified by XRD, FTIR and SEM characterizations and are rationalized with a phase diagram describing the paths the system follows as a result of a change in pressure and/or the temperature.Figure optionsDownload as PowerPoint slide