The Wulff shape of alumina: I. Modeling the kinetics of morphological evolution

Citation
M. Kitayama et al., The Wulff shape of alumina: I. Modeling the kinetics of morphological evolution, J AM CERAM, 83(10), 2000, pp. 2561-2571
Citations number
54
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Material Science & Engineering
Journal title
JOURNAL OF THE AMERICAN CERAMIC SOCIETY
ISSN journal
00027820 → ACNP
Volume
83
Issue
10
Year of publication
2000
Pages
2561 - 2571
Database
ISI
SICI code
0002-7820(200010)83:10<2561:TWSOAI>2.0.ZU;2-5
Abstract
The rate at which fully facetted nonequilibrium shaped particles and pores approach their equilibrium (Wulff) shape via surface diffusion was modeled, and calculations relevant to alumina were performed to guide experimental studies. The modeling focuses on 2-D features, and considers initial partic le/pore shape, size, surface energy anisotropy, and temperature (surface di ffusivity) as variables. The chemical potential differences driving the sha pe change are expressed in terms of facet-to-facet differences in weighted mean curvature, Two approaches to modeling the surface flux are taken. One linearizes the difference in the mean chemical potential of adjacent facets , and assumes the flux is proportional to this difference. The other approa ch treats the surface chemical potential as a continuous function of positi on, and relates the displacement rate of the surface to the divergence of t he surface flux. When consistent values for the relevant materials paramete rs are used, the predictions of these two modeling approaches agree to with in a factor of 1.5, As expected, the most important parameters affecting th e evolution times are the cross-sectional area (volume in 3-D) and the temp erature through its effect on the surface diffusivity, Pores of micrometer size are predicted to reach near-equilibrium shapes in reasonable times at temperatures as low as 1600 degrees C. The detailed geometry of the initial nonequilibrium shape and the Wulff shape appear to have relatively minor e ffects on the times required to reach a near-equilibrium shape.