SCOPUS 정보 검색 플랫폼

Volumn 45, Issue 14, 1992, Pages 8173-8176

Ostwald ripening in two and three dimensions

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0000447296 PISSN: 01631829 EISSN: None Source Type: Journal
DOI: 10.1103/PhysRevB.45.8173 Document Type: Article

Times cited : (86)

References (23)

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- Further results will be given in a future paper: J. H. Yao, K. R. Elder, H. Guo, and M. Grant (unpublished).

22
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- The free parameter in Ardell's theory arises from a physically motivated, but ad hoc cutoff for steady state diffusion. He mimics finite volume fraction effects via the cutoff length r'=R+β overline l, where overline l is the mean distance between a droplet and its nearest neighbor and so is determined by the volume fraction, R is the radius of an average droplet, and β is a number set by Ardell to case 1/2. He notes that this choice is arbitrary (Ref. onlineciteArdell), so we have simply fixed β by fitting K as mentioned above. Alternatively, if we fit Ardell's distribution as best as possible to the numerically observed one, the coarsening rate from that theory is too large by a factor of 3.

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