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Critical effects and scaling at meniscus osculation transitions
Andrew O Parry1, Martin Pospíšil2, Alexandr Malijevský2
1Department of Mathematics, Imperial College London, London SW7 2BZ, United Kingdom.
We developed a scaling theory for liquid drop transitions in confined geometries. The interfacial height exponent depends on intermolecular forces, revealing two distinct regimes: fluctuation-dominated and mean-field.
Area of Science:
- Physics
- Soft Matter Physics
- Surface Science
Background:
- Meniscus osculation occurs when a liquid drop's Laplace radius matches the confining geometry's curvature.
- Understanding critical phenomena in confined liquids is crucial for various physical and chemical processes.
Purpose of the Study:
- To propose a scaling theory for critical effects at meniscus osculation transitions in parabolic geometries.
- To identify and characterize distinct regimes of interfacial height scaling based on intermolecular forces.
Main Methods:
- Development of a simple scaling theory.
- Analysis of interfacial height scaling exponent (β_osc) in relation to the confining radius (R_w).
- Confirmation using an interfacial Hamiltonian model and numerical simulations based on density-functional theory.
Main Results:
- Two regimes of interfacial height scaling (β_osc) were identified: fluctuation-dominated and mean-field.
- The upper critical dimension separating these regimes depends on intermolecular force range.
- For short-range forces in 2D, β_osc = 3/7, confirmed by theory and simulation.
- For long-range forces, the mean-field regime yields β_osc = β_s^co, consistent with complete wetting.
Conclusions:
- The study provides a unified scaling theory for meniscus osculation transitions.
- The identified regimes and critical dimension offer new insights into liquid behavior in confined systems.
- The findings are relevant for understanding interfacial phenomena in diverse scientific and technological applications.
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