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Journal ArticleDOI

Granulation, Phase Change, and Microstructure Kinetics of Phase Change. III

Melvin Avrami
- 01 Feb 1941 - 
- Vol. 9, Iss: 2, pp 177-184
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TLDR
In this paper, a comprehensive description of the phenomena of phase change may be summarized in Phase Change, Grain Number and Microstructure Formulas or Diagrams, giving, respectively, the transformed volume, grain, and microstructure densities as a function of time, temperature, and other variables.
Abstract
The theory of the preceding papers is generalized and the notation simplified. A cluster of molecules in a stable phase surrounded by an unstable phase is itself unstable until a critical size is reached, though for statistical reasons a distribution of such clusters may exist. Beyond the critical size, the cluster tends to grow steadily. The designation ``nuclei'' or ``grains'' is used according as the clusters are below or above the critical size. It is shown that a comprehensive description of the phenomena of phase change may be summarized in Phase Change, Grain Number and Microstructure Formulas or Diagrams, giving, respectively, the transformed volume, grain, and microstructure densities as a function of time, temperature, and other variables. To facilitate the deduction of formulas for these densities the related densities of the ``extended'' grain population are introduced. The extended population is that system of interpenetrating volumes that would obtain if the grains granulated and grew through each other without mutual interference. The extended densities are much more readily derivable from an analysis of the fundamental processes of granulation and growth. It is shown that, under very general circumstances, the densities of the actual grain population may be expressed simply in terms of the extended population.

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Journal ArticleDOI

Crystal growth of nanoporous metal organic frameworks

TL;DR: In this Perspective article, a short overview of the current work and understanding concerning the nucleation and growth processes of nanoporous MOFs is provided and how this work may be expanded upon to further the authors' comprehension of this subject.
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Silver-induced layer exchange for the low-temperature preparation of intrinsic polycrystalline silicon films

TL;DR: In this article, the preparation of large grained continuous polycrystalline silicon layers by metal-induced crystallization was reported, and the macroscopic layer exchange of an amorphous silicon precursor layer in contact with a silver layer was observed for temperatures below the softening point of glass.
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Effect of filler on cure behavior of an epoxy system: Cure modeling

TL;DR: In this paper, the effects of filler on the reaction of an epoxy system cured with aromatic diamine have been studied within the temperature range 70 ˜ 130°C using a differential scanning calorimeter.
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Pure ices IV and XII from high-density amorphous ice

TL;DR: In this paper, high-density amorphous ice (HDA) made by compression of hexagonal ice at 77 K, was heated at a constant pressure of 0.81 GPa up to 183 K and its phase transition followed by displacement-temperatu...
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Crystallization kinetics and morphology of partially melted poly(lactic acid)

TL;DR: In this article, the authors investigated the nonisothermal and isothermal crystallization behavior of pre-crystallized poly(lactic acid) (PLA) after partial or complete melting.
References
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Journal ArticleDOI

Kinetics of Phase Change. I General Theory

TL;DR: In this paper, the theory of phase change is developed with the experimentally supported assumptions that the new phase is nucleated by germ nuclei which already exist in the old phase, and whose number can be altered by previous treatment.
Journal ArticleDOI

Kinetics of Phase Change. II Transformation‐Time Relations for Random Distribution of Nuclei

TL;DR: In this article, a relation between the actual transformed volume V and a related extended volume V1 ex is derived upon statistical considerations, and a rough approximation to this relation is shown to lead, under the proper conditions, to the empirical formula of Austin and Rickett.
Journal ArticleDOI

Grand Partition Functions and So‐Called ``Thermodynamic Probability''

TL;DR: The relation due to Boltzmann between entropy and thermodynamic probability is enunciated in a precise form in this paper and generalized in such a way that each of the other thermodynamic potentials is related in a similar manner to a ''thermodynamic probability'' for which a more suitable name is a ''partition function''.