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Volumn 58, Issue 3, 1998, Pages 3072-3082

Ergodic-nonergodic phase diagram for a concentrated suspension of charge-stabilized colloids: Rescaled mean spherical approximation

Author keywords

[No Author keywords available]

Indexed keywords

APPROXIMATION THEORY; COLLOIDS; DISPERSIONS; GLASS TRANSITION; MATHEMATICAL MODELS; PHASE SPACE METHODS; SUSPENSIONS (FLUIDS); VOLUME FRACTION;

EID: 0032158468     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.58.3072     Document Type: Article
Times cited : (15)

References (70)
  • 10
  • 12
    • 0003625787 scopus 로고
    • J. P. Hansen, D. Levesque, J. Zinn-Justin, North-Holland, Amsterdam
    • W. Götze, in Liquids, Freezing and the Glass Transition, edited by J. P. Hansen, D. Levesque, and J. Zinn-Justin (North-Holland, Amsterdam, 1991), p. 287
    • (1991) Liquids, Freezing and the Glass Transition , pp. 287
    • Götze, W.1
  • 30
    • 0031190177 scopus 로고    scopus 로고
    • A preliminary study of the liquid-glass transition phase diagram within the DLVO potential (see text) was given in this work. Equations (234) given there should respectively be replaced more correctly by Eqs. (212223) here. The latter equations are appropriate for a colloidal suspension. These changes, however, do not affect the numerical values for the idealized liquid-glass transition loci since the solidification equation remains unchanged (rigorous justification is given in Refs. c25 c27 c28 PLEEE8
    • S. K. Lai, W. J. Ma, W. van Megen, and I. K. Snook, Phys. Rev. E 56, 766 (1997). A preliminary study of the liquid-glass transition phase diagram within the DLVO potential (see text) was given in this work. Equations (234) given there should respectively be replaced more correctly by Eqs. (212223) here. The latter equations are appropriate for a colloidal suspension. These changes, however, do not affect the numerical values for the idealized liquid-glass transition loci since the solidification equation remains unchanged (rigorous justification is given in Refs. 25, 27, and 28).PLEEE8
    • (1997) Phys. Rev. E , vol.56 , pp. 766
    • Lai, S.K.1    Ma, W.J.2    van Megen, W.3    Snook, I.K.4
  • 36
    • 85121089392 scopus 로고
    • (in Japanese). ZZZZZZ
    • Butsuri, Bull., Phys. Soc. Jpn.)48, 869 (1993) (in Japanese).ZZZZZZ
    • (1993) Bull., Phys. Soc. Jpn.) , vol.48 , pp. 869
  • 64
    • 85121089333 scopus 로고    scopus 로고
    • Here we follow the work of c27 for the definition of the memory function, which differs from those of c26 c25 by a factor [Formula Presented] [cf. Eq. (1.2) in c26 and Eq. (13) in c27]
    • Here we follow the work of 27 for the definition of the memory function, which differs from those of 2625 by a factor D0q2 [cf. Eq. (1.2) in 26 and Eq. (13) in 27].
  • 69
    • 85121089099 scopus 로고    scopus 로고
    • G. Senatore, in Structure and dynamics of Strongly Interacting Colloids and Supramolecular Aggregates in Solution, edited by S. H. Chen, J. S. Huang, and P. Tartaglia (Kluwer Academic, Dordrecht, 1992), p. 181
    • G. Senatore, in Structure and dynamics of Strongly Interacting Colloids and Supramolecular Aggregates in Solution, edited by S. H. Chen, J. S. Huang, and P. Tartaglia (Kluwer Academic, Dordrecht, 1992), p. 181.
  • 70
    • 85121089482 scopus 로고    scopus 로고
    • K. S. Schmitz, Macroions in Solution and Colloidal Suspension (VCH, New York, 1993), pp. 17–67
    • K. S. Schmitz, Macroions in Solution and Colloidal Suspension (VCH, New York, 1993), pp. 17–67.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.