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Vibrational and configurational heat capacity of poly(vinyl acetate) from dynamic measurements

机译:聚乙酸乙烯酯的振动和构型热容动态测量

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The complex heat capacity C-p(*) of poly(vinyl acetate) has been measured at 20.95 mrad/s modulation frequency during the cooling as well as on heating at 24, 8, and 2 K/h and during cooling at 0.5 K/h. The study is complemented with (the rate-dependent) C-p,C-app measured during cooling and heating at 60, 24, and 8 K/h. At low temperatures, the real component of C-p(*) yields the unrelaxed C-p or C-p,C-vib, the vibrational part of C-p. It is found to be indistinguishable from C-p,C-glass and lies on a line extrapolated to its equilibrium melt's temperature. At T near T-g,Delta C-p(=C-p,C-melt-C-p,C-glass) shows no detectable contribution from C-p,C-vib. The finding conflicts with a modified entropy theory calculation [E. A. DiMarzio and F. Dowell, J. Appl. Phys. 50, 6061 (1979)], which had predicted that similar to 27% of Delta C-p of poly(vinyl acetate) at T near T-g is vibrational in origin and the remainder configurational. At T < T-g, the real component of C-p(*) varies more slowly with T than C-p,C-app.
机译:在冷却期间以及在以24、8和2 K / h加热以及以0.5 K / h冷却期间,在20.95 mrad / s调制频率下测量了聚乙酸乙烯酯的复热容Cp(*) 。该研究补充了在60、24和8 K / h的冷却和加热过程中测得的(取决于速率)C-p,C-app。在低温下,C-p(*)的实部会产生未松弛的C-p或C-p,C-vib,即C-p的振动部分。它与C-p,C-玻璃是无法区分的,并且位于外推至其平衡熔体温度的直线上。在T接近T-g时,ΔC-p(= C-p,C-熔体-C-p,C-玻璃)没有显示出C-p,C-vib的可检测贡献。这一发现与改进的熵理论计算相冲突[E. A. DiMarzio和F. Dowell,J。Appl。物理50,6061(1979)],其预测在T-g附近的T处,类似于聚乙酸乙烯酯的Delta C-p的27%是起源振动的,其余是构型的。在T

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