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Continuous Condensation in Nanogrooves.

The result's identifiers

  • Result code in IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F67985858%3A_____%2F18%3A00497922" target="_blank" >RIV/67985858:_____/18:00497922 - isvavai.cz</a>

  • Result on the web

    <a href="http://dx.doi.org/10.1103/PhysRevE.97.052804" target="_blank" >http://dx.doi.org/10.1103/PhysRevE.97.052804</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1103/PhysRevE.97.052804" target="_blank" >10.1103/PhysRevE.97.052804</a>

Alternative languages

  • Result language

    angličtina

  • Original language name

    Continuous Condensation in Nanogrooves.

  • Original language description

    We consider condensation in a capillary groove of width L and depth D, formed by walls that are completely wet (contact angle theta=0), which is in a contact with a gas reservoir of the chemical potential mu. On a mesoscopic level, the condensation process can be described in terms of the midpoint height l of a meniscus formed at the liquid-gas interface. For macroscopically deep grooves (D -> 8), and in the presence of long-range (dispersion) forces, the condensation corresponds to a second-order phase transition, such that l similar to (mu(cc)-mu)(-1/4) as mu ->mu(-)(cc) where mu(cc) is the chemical potential pertinent to capillary condensation in a slit pore of width L. For finite values of D, the transition becomes rounded and the groove becomes filled with liquid at a chemical potential higher than mu(cc) with a difference of the order of D-3. For sufficiently deep grooves, the meniscus growth initially follows the power law l similar to (mu(cc-mu)cc)(-1/4) , but this behavior eventually crosses over to l similar to D-(mu-mu(cc))-1/3 above mu cc, with a gap between the two regimes shown to be (delta) over bar mu similar to D-3. Right at mu=mu(cc), when the groove is only partially filled with liquid, the height of the meniscus scales as l* similar to ((DL)-L-3)(1/4). Moreover, the chemical potential (or pressure) at which the groove is half-filled with liquid exhibits a nonmonotonic dependence on D with a maximum at D approximate to 3L/2 and coincides with mu(cc) when L approximate to D. Finally, we show that condensation in finite grooves can be mapped on the condensation in capillary slits formed by two asymmetric (competing) walls a distance D apart with potential strengths depending on L. All these predictions, based on mesoscopic arguments, are confirmed by fully microscopic Rosenfeld's density functional theory with a reasonable agreement down to surprisingly small values of both L and D.

  • 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

    10403 - Physical chemistry

Result continuities

  • Project

    <a href="/en/project/GA17-25100S" target="_blank" >GA17-25100S: Geometrically and Chemically Modified Surfaces: From Statics to Dynamics</a><br>

  • Continuities

    P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)

Others

  • Publication year

    2018

  • 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

  • Volume of the periodical

    97

  • Issue of the periodical within the volume

    5

  • Country of publishing house

    US - UNITED STATES

  • Number of pages

    11

  • Pages from-to

  • UT code for WoS article

    000433068100006

  • EID of the result in the Scopus database

    2-s2.0-85047778626