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首页> 外文期刊>Physical review, E. Statistical physics, plasmas, fluids, and related interdisciplinary topics >Microscopic basis of free-volume concept as studied by quasielastic neutron scattering and positron annihilation lifetime spectroscopy
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Microscopic basis of free-volume concept as studied by quasielastic neutron scattering and positron annihilation lifetime spectroscopy

机译:准弹性中子散射和正电子an没寿命光谱研究的自由体积概念的微观基础

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摘要

We have reexamined the free-volume concept presented by Cohen and Turnbull on the basis of two microscopic quantities: the excess mean-square displacement (u(2))(f) and the total free volume V-PA,V-t , of poly- butadiene evaluated from the quasielastic neutron scattering and the positron annihilation lifetime spectroscopy (PALS) data, respectively. Comparing with the viscosity eta we found two relations, eta= eta(0) exp u(0)(2)/[u(2)](f) eta=eta(0)exp V-PA,V-0*/V-PA,V-t= eta(0) exp V-PA,V-0*/v(PA,f) where U-0(2),V-PA,V-0* and v(PA,0)* are the critical values for the mean-square displacement, the total PALS free volume, and the PALS free volume per molecule, respectively, and further v(PA,0)*=V-PA,V-0*/N, N being the total number of molecules or segments. On the basis of these relations, we discuss the microscopic basis of the free-volume theory. The experimentally evaluated critical u(0)(2) and v(PA,0)* are much larger than the average values of [u(2)](f) and v(PA,f) calculated from the distributions . This has been explained from the low probability of escaping motions from a molecular cage. The free volume per monomer and the free-volume fraction were calculated from the excess mean-square displacement ([u(2)](f)) The former was compared with the free-volume hole obtained by PALS, suggesting that 22 monomers are required for one PALS free-volume hole. The free-volume fraction obtained from the excess mean-square displacement was found to be 6.4% at 250 K, which is in reasonable agreement with that evaluated from the rheological data (9.0%). [S1063-651X(99)00308-6]. [References: 27]
机译:我们根据两个微观量重新审查了Cohen和Turnbull提出的自由体积概念:多均方根的均方差(u(2))(f)和总自由体积V-PA,Vt丁二烯分别由准弹性中子散射和正电子an没寿命光谱(PALS)数据评估。与粘度eta相比,我们发现两个关系,eta = eta(0)exp u(0)(2)/ [u(2)](f)eta = eta(0)exp V-PA,V-0 * / V-PA,Vt = eta(0)exp V-PA,V-0 * / v(PA,f)其中U-0(2),V-PA,V-0 *和v(PA,0)*分别是均方位移,每个分子的总PALS自由体积和PALS自由体积的临界值,并且v(PA,0)* = V-PA,V-0 * / N,N为分子或片段的总数。在这些关系的基础上,我们讨论了自由体积理论的微观基础。实验评估的临界u(0)(2)和v(PA,0)*远大于根据分布计算的[u(2)](f)和v(PA,f)的平均值。这是由于从分子笼中逃逸运动的可能性很小。根据过量的均方位移([u(2)](f)计算每个单体的自由体积和自由体积分数。将前者与PALS获得的自由体积孔进行比较,表明存在22种单体一个PALS自由体积孔需要。由过量均方位移获得的自由体积分数在250 K下为6.4%,这与从流变数据评估得出的自由体积分数(9.0%)在合理的范围内。 [S1063-651X(99)00308-6]。 [参考:27]

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