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Temperature and pressure dependence of the free volume in the perfluorinated polymer glass CYTOP: A positron lifetime and pressure‐volume‐temperature study
Authors:G Dlubek  J Pionteck  M Sniegocka  E M Hassan  R Krause‐Rehberg
Institution:1. ITA Institut für Innovative Technologien, K?then/Halle, Wiesenring 4, D‐06120 Lieskau (Halle/S.), GermanyITA Institut für Innovative Technologien, K?then/Halle, Wiesenring 4, D‐06120 Lieskau (Halle/S.), Germany;2. Leibniz‐Institut für Polymerforschung Dresden e.V., Hohe Strasse 6, D‐01069 Dresden, Germany;3. Institute of Physics, Maria Curie‐Sklodowska University, Pl. M. Curie‐Sklodowskiej 1, PL‐20‐031 Lublin, Poland;4. Institut für Physik, Martin‐Luther‐Universit?t Halle‐Wittenberg, D‐06099 Halle/S., Germany
Abstract:The microstructure of the free volume was studied for an amorphous perfluorinated polymer (Tg = 378 K). To this aim we employed pressure–volume–temperature experiments (PVT) and positron annihilation lifetime spectroscopy (PALS). Using the Simha‐Somcynsky equation of state the hole free volume fraction h and the specific free and occupied volumes, Vf = hV and Vocc = (1 ? h)V, were determined. Their expansivities and compressibilities were calculated from fits of the Tait equation to the volume data. It was found that in the glass Vocc has a particular high compressibility, while the compressibility of Vf is rather low, although h (300 K) = 0.108 is large. In the rubbery state the free volume dominates the total compressibility. From the PALS spectra the hole size distribution, its mean, 〈vh〉, and mean dispersion, σh, were calculated. From a comparison of 〈vh〉 with Vf a constant hole density of Nh′ = 0.25 × 1021 g?1 was estimated. The volume of the smallest representative freely fluctuating subsystem, 〈VSV〉 ∝ 1/σh2, is unusually small. This was explained by an inherent topologic disorder of this polymer. 〈vh〉 and σh show an exponential‐like decrease with increasing pressure P at 298 K. The hole density, calculated from Nh′ = Vf/〈vh〉, seems to show an increase with P which is unexpected. This was explained by the compression of holes in the glass in two, rather than three, dimensions. © 2007 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 45: 2519–2534, 2007
Keywords:fluoropolymers  glass transition  thermal properties
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