Does the longer-range wall potential in generalized Sullivan models favour a first-order wetting transition?

1991 ◽  
Vol 3 (9) ◽  
pp. 1197-1205 ◽  
Author(s):  
E J Ding
Materials ◽  
2021 ◽  
Vol 14 (23) ◽  
pp. 7138
Author(s):  
Paweł Bryk ◽  
Artur P. Terzyk

Wettablity is one of the important characteristics defining a given surface. Here we show that the effective interface potential method of determining the wetting temperature, originally proposed by MacDowell and Müller for the surfaces exhibiting the first order wetting transition, can also be used to estimate the wetting temperature of the second order (continuous) wetting transition. Some selected other methods of determination of the wetting temperature are also discussed.


1993 ◽  
Vol 48 (2) ◽  
pp. 1131-1135 ◽  
Author(s):  
R. Bausch ◽  
R. Blossey

1988 ◽  
Vol 37 (7) ◽  
pp. 3818-3820 ◽  
Author(s):  
G. Forgacs ◽  
N. M. S̆vrakić ◽  
V. Privman

Langmuir ◽  
2001 ◽  
Vol 17 (10) ◽  
pp. 2995-2998 ◽  
Author(s):  
J. Y. Wang ◽  
M. Crawley ◽  
B. M. Law

1992 ◽  
Vol 03 (05) ◽  
pp. 1025-1058 ◽  
Author(s):  
KURT BINDER ◽  
KATHARINA VOLLMAYR ◽  
HANS-PETER DEUTSCH ◽  
JOSEPH D. REGER ◽  
MANFRED SCHEUCHER ◽  
...  

This brief review discusses methods to locate and characterize first order phase transitions, paying particular attention to finite size effects. In the first part, the order parameter probability distribution and its fourth-order cumulant is discussed for thermally driven first-order transitions (the 3-state Potts model in d=3 dimensions is treated as an example). First-order transitions are characterized by a minimum of the cumulant, which gets very deep for large enough systems. In the second part, we discuss how to locate first order phase boundaries ending in a critical point in a large parameter space. As an example, the study of the unmixing transition of asymmetric polymer mixtures by a combination of histogram techniques and finite size scaling is described. As a final problem, we discuss the shift of the gas-liquid condensation in thin-film geometry confined between two parallel plates due to boundary fields (“capillary condensation”). Being interested in temperatures far below bulk criticality (e. g. near the wetting transition), special thermodynamic integration techniques are the method of choice, rather than the use of finite sizes scaling to map out the (asymmetric) phase diagram.


2002 ◽  
Vol 66 (5) ◽  
Author(s):  
F. A. M. Leermakers ◽  
J. H. Maas ◽  
M. A. Cohen Stuart

2010 ◽  
Vol 83 (10) ◽  
pp. 1198-1202 ◽  
Author(s):  
Hiroki Matsubara ◽  
Yosuke Ikebe ◽  
Yasutaka Ushijima ◽  
Youichi Takata ◽  
Takanori Takiue ◽  
...  

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