The gels formed under high pressures were collected as wet gels after cooling and depressurization and characterized by DSC using a high pressure DSC capsule. For the wet gel, DSC scans show a gel melting peak at around 110 °C observed in a heating run and a gel formation peak at around 45 °C observed in a cooling run that follows. These temperatures are comparable with the phase transition temperatures which were determined in the view cell. Once the gel is dried, the DSC scans still show a gel melting peak in a higher temperature range in a heating run while no gel formation peak is observed in a cooling run. The wet and dry gels were characterized by FTIR also. The helical ä phase structure was observed in both the wet and the dry gels assigned by the presence of absorbance of helix bands in the region 500-600 cm-1 and a doublet at 934/943 cm-1 in these spectra that are characteristic of the ä phase [3]. These results indicate that there is still some toluene entrapped in the polymer matrix to form a clathrate phase even in a dry gel. To remove the entrapped solvent from polymer matrix, supercritical CO2-extraction at 40 °C and 22 MPa was employed. High-porosity aerogels with low density were obtained after extraction from both the wet and dry gels.
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