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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

  • Czech description

Classification

  • Type

    J<sub>imp</sub> - Article in a specialist periodical, which is included in the Web of Science database

  • CEP classification

  • OECD FORD branch

    10305 - Fluids and plasma physics (including surface physics)

Result continuities

  • Project

  • 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