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Critical effects and scaling at meniscus osculation transition

Identifikátory výsledku

  • Kód výsledku v IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F67985858%3A_____%2F22%3A00564225" target="_blank" >RIV/67985858:_____/22:00564225 - isvavai.cz</a>

  • Výsledek na webu

    <a href="https://hdl.handle.net/11104/0335935" target="_blank" >https://hdl.handle.net/11104/0335935</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1103/PhysRevE.106.054802" target="_blank" >10.1103/PhysRevE.106.054802</a>

Alternativní jazyky

  • Jazyk výsledku

    angličtina

  • Název v původním jazyce

    Critical effects and scaling at meniscus osculation transition

  • Popis výsledku v původním jazyce

    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 0 ∝ Rβosc w 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, thenexponent 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 βcos 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 thatnβosc ≈ βcos ≈ 0.326 close to the predicted value of 1/3 appropriate to the mean-field regime for dispersion forces

  • Název v anglickém jazyce

    Critical effects and scaling at meniscus osculation transition

  • Popis výsledku anglicky

    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 0 ∝ Rβosc w 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, thenexponent 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 βcos 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 thatnβosc ≈ βcos ≈ 0.326 close to the predicted value of 1/3 appropriate to the mean-field regime for dispersion forces

Klasifikace

  • Druh

    J<sub>imp</sub> - Článek v periodiku v databázi Web of Science

  • CEP obor

  • OECD FORD obor

    10301 - Atomic, molecular and chemical physics (physics of atoms and molecules including collision, interaction with radiation, magnetic resonances, Mössbauer effect)

Návaznosti výsledku

  • Projekt

    <a href="/cs/project/GA20-14547S" target="_blank" >GA20-14547S: Povrchové a kritické jevy v nano-strukturovaném prostředí</a><br>

  • Návaznosti

    I - Institucionalni podpora na dlouhodoby koncepcni rozvoj vyzkumne organizace

Ostatní

  • Rok uplatnění

    2022

  • Kód důvěrnosti údajů

    S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Údaje specifické pro druh výsledku

  • Název periodika

    Physical Review E

  • ISSN

    2470-0045

  • e-ISSN

    2470-0053

  • Svazek periodika

    106

  • Číslo periodika v rámci svazku

    5

  • Stát vydavatele periodika

    US - Spojené státy americké

  • Počet stran výsledku

    8

  • Strana od-do

    054802

  • Kód UT WoS článku

    000891636900013

  • EID výsledku v databázi Scopus

    2-s2.0-85143896254