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Configurational and residual entropies of nonergodic crystalsand the entropy's behavior on glass formation

机译:非遍历晶体的构型和残差熵及其在玻璃形成过程中的行为

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We use thermodynamics of lattice vacancies to test the merits of the view that (i) statistical entropy,kB In St vanishes on vitrification of a liquid and hence there is no residual entropy and (ii) k_BIn 1Zof a nonergodic state would increase with time t as its structure relaxes. We argue that this viewconflicts with the precepts of the configurational entropy of a crystal,-R[x In x+ (1-x)ln(1-x)],where x is the fractional population of vacancies, and with the observed decrease in x with t onstructural relaxation. The issue of whether the entropy of a kinetically arrested crystal state is equal to k_BIn Ωor equal to -R[x ln x+ (1-x)ln(1-x)] can be resolved by measuring the vapor pressure,the emf of an electrolytic cell, and by scanning calorimetry. We also consider how the energylandscapes of a crystal and liquid differ, and point out that since crystals are in a nonequilibriumstate, their thermodynamic data are inappropriate for testing the validity of the third law.
机译:我们使用晶格空位的热力学来检验以下观点的优劣:(i)统计熵kB In St在液体玻璃化时消失,因此没有残留熵;并且(ii)非遍历状态的k_BIn 1Z将随时间t增加随着其结构的放松。我们认为,这种观点与晶体的结构熵-R [x In x +(1-x)ln(1-x)]的规范相冲突,其中x是空位的分数人口,并且与观察到的x具有结构上的松弛。可以通过测量蒸气压来解决动力学停止的晶体状态的熵等于k_BInΩ或等于-R [x ln x +(1-x)ln(1-x)]的问题。电解池,并通过扫描量热法。我们还考虑了晶体和液体的能量景观如何不同,并指出由于晶体处于非平衡状态,因此它们的热力学数据不适用于检验第三定律的有效性。

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