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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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Citations
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Journal ArticleDOI

A new theory of bubble formation in magma

TL;DR: In this article, the authors developed an accurate theoretical model of bubble formation in supersaturated magma with a relatively low viscosity under the formulation by Toramaru (1995), and obtained analytical solutions for the time evolution of the nucleation rate and the number density of nucleated bubbles in cases with constant decompression rates and constant supersaturation pressures.
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Crystallisation behaviour of high density polyethylene blends with bimodal molar mass distribution: 2. Non-isothermal crystallisation

TL;DR: In this article, the Avrami index under non-isothermal conditions was analyzed with a method developed by Harnisch and Muschik, and the results indicated that thermal nucleation and spherical growth regimes are present in all studied materials.
Journal ArticleDOI

How Xenopus laevis embryos replicate reliably: investigating the random-completion problem.

TL;DR: In this article, the authors investigated the random-completion problem using a type of model first developed to describe the kinetics of first-order phase transitions, and derived the distribution of replication completion times for a finite genome.
Journal ArticleDOI

Isothermal and Nonisothermal Cold Crystallization Behaviors of Biodegradable Poly(l-lactide)/Octavinyl-Polyhedral Oligomeric Silsesquioxanes Nanocomposites

TL;DR: In this paper, isothermal and nonisothermal cold crystallization behaviors of biodegradable poly(l-lactide) (PLLA)/octavinyl-polyhedral oligomeric silsesquioxanes (ovi-POSS) nanocomposites at low ovi-pOSS loadings were investigated.
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''.