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Volumn 79, Issue 5, 2009, Pages

Derivation of the phase-field-crystal model for colloidal solidification

Author keywords

[No Author keywords available]

Indexed keywords

BULK FREEZING; COLLOIDAL SUSPENSIONS; CRYSTAL DYNAMIC; CRYSTAL MODELS; CRYSTAL NUCLEATION; INDIVIDUAL PARTICLE MOTIONS; PARALLEL DIPOLES; PHASE FIELDS; SMOLUCHOWSKI EQUATION; UNDERCOOLED MELT;

EID: 67650915708     PISSN: 15393755     EISSN: 15502376     Source Type: Journal    
DOI: 10.1103/PhysRevE.79.051404     Document Type: Article
Times cited : (223)

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    • In particular, we chose s=60 for 31≤Γ≤35, s=7 for 37≤Γ<40, and s=5 for Γ40, in the DDFT, s=41 for Γ=33, s=21 for Γ=37, s=11 for 38≤Γ≤60, in the PFC1 model, and s=83 for Γ=37, s=41 for Γ=38, s=21 for Γ=39, and s=11 for 38≤Γ≤60 in the PFC2 model.
    • In particular, we chose s=60 for 31≤Γ≤35, s=7 for 37≤Γ<40, and s=5 for Γ40, in the DDFT, s=41 for Γ=33, s=21 for Γ=37, s=11 for 38≤Γ≤60, in the PFC1 model, and s=83 for Γ=37, s=41 for Γ=38, s=21 for Γ=39, and s=11 for 38≤Γ≤60 in the PFC2 model.
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    • The discussion of the behavior of vf (t τB) in the DDFT and the PFC models is deferred to a future publication. For the same behavior in a similar model of hard spheres, see.
    • The discussion of the behavior of vf (t τB) in the DDFT and the PFC models is deferred to a future publication. For the same behavior in a similar model of hard spheres, see.


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