SCOPUS 정보 검색 플랫폼

Volumn 47, Issue 21, 1993, Pages 14110-14125

Theory and simulation of Ostwald ripening

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Indexed keywords

EID: 35949007820 PISSN: 01631829 EISSN: None Source Type: Journal
DOI: 10.1103/PhysRevB.47.14110 Document Type: Article

Times cited : (323)

References (33)

3
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- edited by, C. Domb, J. L. Lebowitz, Academic, London, Vol. 8.
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- Gunton, J.D.¹ San Miguel, M.² Sahni, P.S.³

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- (1984) Physica , vol.123 A , pp. 386
- Tokuyama, M.¹ Kawasaki, K.²

9
- 84926926577
- Here, we only present the mean field results of TKE, called the drift term approximation by them. In our earlier paper (Ref. onlineciteyao), we used an incorrect definition of the volume fraction given by TKE in Ref. onlineciteKawasaki. This resulted in an inaccurate calculation of their coarsening rate and the distribution function which is corrected here.

10
- 0021521028
- (1984) Acta Metall. , vol.32 , pp. 2001
- Voorhees, P.W.¹ Glicksman, M.E.²

11
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- (1984) Acta Metall. , vol.32 , pp. 2013
- Voorhees, P.W.¹ Glicksman, M.E.²

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- Tsumuraya, K.¹ Miyata, Y.²

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- A.
- (1979) Acta Metall. , vol.27 , pp. 489
- Brailsford, D.¹ Wynblatt, P.²

20
- 84926945709
- Mardar's theory includes spatial correlations which are absent from our approach. In principle, these effects are expected to become important for large volume fractions. However, his approach involves uncontrolled approximations such that, in our opinion, spatial correlations are not included systematically. Indeed, for nonzero volume fraction, there is no regime of agreement between his work and any other theory, or the numerical simulation presented herein.

21
- 0000447296
- Some of these results have been previously published in a short paper:
- (1992) Phys. Rev. B , vol.45 , pp. 8173
- Yao, J.H.¹ Elder, K.R.² Guo, H.³ Grant, M.⁴

24
- 0001656835
- (1989) Phys. Rev. A , vol.39 , pp. 4848
- Zheng, Q.¹ Gunton, J.D.²

25
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- (1989) Phys. Rev. B , vol.39 , pp. 11-956
- Rogers, T.M.¹ Desai, R.C.²

29
- 84926945707
- Note that on using Eq. ( refeq:grw), we obtain the continuous version of Eq. ( refeq:cons), int0∞ d(vRD)/dt f(R,t)dR = 0. Therefore, partial θav / partial t = 0; i.e., from the conservation law, Eq. ( refeq:cons), the total amount of solute in the majority phase remains constant.

30
- 0001055782
- (1971) Acta Metall. , vol.19 , pp. 321
- Rastogi, K.¹ Ardell, A.J.²

31
- 84926888688
- Because Zheng and Gunton did not present the distribution function for φ = 0.01 or φ = 0.05, we are not able to compare with their results.

32
- 4243747907
- (1993) Phys. Rev. B , vol.47 , pp. 1270
- Yao, J.H.¹ Guo, H.² Grant, M.³

* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.