Počet záznamů: 1  

Critical behaviour of the contact angle within nonwetting gaps.

  1. 1.
    SYSNO ASEP0582854
    Druh ASEPJ - Článek v odborném periodiku
    Zařazení RIVJ - Článek v odborném periodiku
    Poddruh JČlánek ve WOS
    NázevCritical behaviour of the contact angle within nonwetting gaps.
    Tvůrce(i) Parry, A.O. (GB)
    Malijevský, Alexandr (UCHP-M) RID, ORCID, SAI
    Rascón, C. (ES)
    Číslo článku17LT01
    Zdroj.dok.Journal of Physics-Condensed Matter. - : Institute of Physics Publishing - ISSN 0953-8984
    Roč. 36, č. 17 (2024)
    Poč.str.6 s.
    Jazyk dok.eng - angličtina
    Země vyd.US - Spojené státy americké
    Klíč. slovawetting transitions ; criticality ; classical density functional theory
    Obor OECDCondensed matter physics (including formerly solid state physics, supercond.)
    CEPGA21-27338S GA ČR - Grantová agentura ČR
    Způsob publikováníOpen access
    Institucionální podporaUCHP-M - RVO:67985858
    UT WOS001152972200001
    EID SCOPUS85183959694
    DOI10.1088/1361-648X/ad20a3
    AnotaceRecent density functional theory and simulation studies of fluid adsorption near planar walls in systems where the wall–fluid and fluid–fluid interactions have different ranges, have shown that critical point wetting may not occur and instead nonwetting gaps appear in the surface phase diagram, separating lines of wetting and drying transitions, that extend up to the critical temperature Tc. Here we clarify the features of the surface phase diagrams that are common, regardless of the range and balance of the forces, showing, in particular, that the lines of temperature driven wetting and drying transitions, as well as lines of constant contact angle $\pi\gt\theta\gt 0$, always converge to an ordinary surface phase transition at Tc. When nonwetting gaps appear the contact angle either vanishes or tends to π as $t\equiv(T_c-T)/T_c\to 0$. More specifically, when the wall–fluid interaction is long-ranged (dispersion-like) and the fluid–fluid short-ranged we estimate $\pi-\theta\propto t^{0.16}$, compared with $\theta\propto t^{0.77}$ when the wall–fluid interaction is short-ranged and the fluid–fluid dispersion-like, allowing for the effects of bulk critical fluctuations. The universal convergence of the lines of constant contact angle implies that critical point filling always occurs for fluids adsorbed in wedges.
    PracovištěÚstav chemických procesů
    KontaktEva Jirsová, jirsova@icpf.cas.cz, Tel.: 220 390 227
    Rok sběru2025
    Elektronická adresahttps://iopscience.iop.org/article/10.1088/1361-648X/ad20a3/pdf
Počet záznamů: 1  

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