Critical effects and scaling at meniscus osculation transitions
The result's identifiers
Result code in IS VaVaI
<a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F60461373%3A22340%2F22%3A43924827" target="_blank" >RIV/60461373:22340/22:43924827 - isvavai.cz</a>
Result on the web
<a href="https://journals.aps.org/pre/abstract/10.1103/PhysRevE.106.054802" target="_blank" >https://journals.aps.org/pre/abstract/10.1103/PhysRevE.106.054802</a>
DOI - Digital Object Identifier
<a href="http://dx.doi.org/10.1103/PhysRevE.106.054802" target="_blank" >10.1103/PhysRevE.106.054802</a>
Alternative languages
Result language
angličtina
Original language name
Critical effects and scaling at meniscus osculation transitions
Original language description
We propose a simple scaling theory describing critical effects at rounded meniscus osculation transitions which occur when the Laplace radius of a condensed macroscopic drop of liquid coincides with the local radius of curvature Rw in a confining parabolic geometry. We argue that the exponent βosc characterizing the scale of the interfacial height ℓ0 ∝ Rw^βosc at osculation, for large Rw, falls into two regimes representing fluctuation-dominated and mean-field-like behavior, respectively. These two regimes are separated by an upper critical dimension, which is determined here explicitly and depends on the range of the intermolecular forces. In the fluctuation-dominated regime, representing the universality class of systems with short-range forces, the exponent is related to the value of the interfacial wandering exponent ζ by βosc = 3ζ/(4-ζ). In contrast, in the mean-field regime, which was not previously identified and which occurs for systems with longer-range forces (and higher dimensions), the exponent βosc takes the same value as the exponent βs^co for complete wetting, which is determined directly by the intermolecular forces. The prediction βosc = 3/7 in d = 2 for systems with short-range forces (corresponding to ζ = 1/2) is confirmed using an interfacial Hamiltonian model which determines the exact scaling form for the decay of the interfacial height probability distribution function. A numerical study in d = 3, based on a microscopic model density-functional theory, determines that βosc ≈ βs^co ≈0.326 close to the predicted value of 1/3 appropriate to the mean-field regime for dispersion forces.
Czech name
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Czech description
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Classification
Type
J<sub>imp</sub> - Article in a specialist periodical, which is included in the Web of Science database
CEP classification
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OECD FORD branch
10305 - Fluids and plasma physics (including surface physics)
Result continuities
Project
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Continuities
I - Institucionalni podpora na dlouhodoby koncepcni rozvoj vyzkumne organizace
Others
Publication year
2022
Confidentiality
S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů
Data specific for result type
Name of the periodical
PHYSICAL REVIEW E
ISSN
2470-0045
e-ISSN
2470-0053
Volume of the periodical
106
Issue of the periodical within the volume
5
Country of publishing house
US - UNITED STATES
Number of pages
8
Pages from-to
054802
UT code for WoS article
000891636900013
EID of the result in the Scopus database
2-s2.0-85143896254