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Volumn 132, Issue 8, 2010, Pages

Simulation study of the disjoining pressure profile through a three-phase contact line

Author keywords

[No Author keywords available]

Indexed keywords

INTERFACES (MATERIALS); MAGNETIC BUBBLES;

EID: 77749292976     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3327840     Document Type: Article
Times cited : (31)

References (60)
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    • When applied to the geometry of Fig., one must slightly modify the definition of the interface potential V (h) if one desires to maintain the boundary condition V (∞) =0, due to the fact that y→∞ corresponds to partial wetting (not complete wetting) and due to the increased amount of planar LV interface induced by a limiting slope of θ (Ref.)
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    • W/δh. It is important to realize that the disjoining pressure sum rule obtained in this manner is invariant with respect to the different choices of interface potential, local and nonlocal. This is reflected in the fact that Eqs. define the same equation for the disjoining pressure. Thus, for a specified Π (y) the film height profile [Eqs.] is independent of the choice of interface potential, local or nonlocal, i.e., it defines the coarse-grained profile of any interface Hamiltonian whose disjoining pressure is identical to an experimental Π (y). In this sense it is an "exact" result for the coarse-grained profile. In contrast, the line tension result is derived via a renormalized Hamiltonian with a local potential, allowing for the use of Indekeu's simplest theory. The renormalization has enforced conservation of momentum normal to the substrate and so in this sense Eq. is perhaps the best one can do within a local potential approximation. One should be aware that this approximation might breakdown qualitatively in some circumstances, such as in the approach to an interfacial phase transition. It would therefore be of interest to consider how far (or if at all) explicit representations of nonlocality might justify our use of the renormalized order parameter. 10.1088/0953-8984/18/28/001 (Pubitemid 43982952)
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