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首页> 外文期刊>Journal of Polymer Science, Part B. Polymer Physics >Temperature and pressure dependence of the free volume in the perfluorinated polymer glass CYTOP: A positron lifetime and pressure-volume-temperature study
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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

机译:全氟聚合物玻璃CYTOP中自由体积的温度和压力依赖性:正电子寿命和压力-体积-温度研究

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The microstructure of the free volume was studied for an amorphous perfluorinated polymer (T-g= 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, V-f = hV and V-occ = (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 V-occ 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, upsilon(h), and mean dispersion, sigma(h), were calculated. From a comparison Of upsilon(h) with Vf a constant hole density of N-h' = 0.25 X 10(21) g(-1) was estimated. The volume of the smallest representative freely fluctuating 2 subsystem, V-sv proportional to 1/sigma(2)(h), is unusually small. This was explained by an inherent topologic disorder of this polymer. upsilon(h) and sigma(h) show an exponential-like decrease with increasing pressure P at 298 K. The hole density, calculated from N-h' = V-f/upsilon(h), 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. (c) 2007 Wiley Periodicals, Inc.
机译:研究了无定形全氟化聚合物(T-g = 378 K)的自由体积的微观结构。为此,我们采用了压力-体积-温度实验(PVT)和正电子an没寿命谱(PALS)。使用Simha-Somcynsky状态方程,确定无孔体积分数h和比自由体积和占有体积V-f = hV和V-occ =(1- h)V。根据Tait方程对体积数据的拟合计算出它们的膨胀性和可压缩性。已经发现在玻璃中,V-occ具有特别高的可压缩性,而Vf的可压缩性却很低,尽管h(300K)= 0.108很大。在橡胶态下,自由体积决定了总的可压缩性。从PALS光谱中计算出孔的尺寸分布,其平均值upsilon(h)和平均色散σ(h)。通过upsilon(h)与Vf的比较,可以得出恒定的孔密度N-h'= 0.25 X 10(21)g(-1)。最小的具有代表性的自由波动2子系统的体积V-sv与1 / sigma(2)(h)成比例,非常小。这是由该聚合物的固有拓扑异常解释的。 upsilon(h)和sigma(h)在298 K下随压力P的增加呈指数状下降。根据N-h'= V-f / upsilon(h)计算的孔密度似乎随着P的增加而增加,这是出乎意料的。这是由于玻璃中孔的压缩是二维的,而不是三维的。 (c)2007年Wiley Periodicals,Inc.

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