Skip to content
DraconiticResearch
Search Sources API
203,234 studies31 sourcesUpdated 5 min ago
PreprintCC BYChemRxiv

Nanothermodynamic Generalization of the Young–Laplace and Young Equations for Sessile Droplets with Line Effects

  1. 1Department of Chemistry
  2. 2Norwegian University of Science and Technology

Abstract

Thermodynamic investigations of wetting phenomena require that we handle the nanoscale. By combining Hill’s small-system thermodynamics with a Gibbsian composite-system description, we formulate the equilibrium thermodynamics of a sessile nanodroplet. We consider a one-component liquid droplet resting on an ideal, flat, inert solid substrate and in contact with reservoirs that fix the temperature and chemical potential. Finite-size effects are retained in the liquid bulk phase, the liquid–vapor interface, and the three-phase contact line, while the solid–vapor and solid–liquid interfaces are assumed to follow regular thermodynamics and treated macroscopically. The distinction between integral and differential pressure, surface tension, and line tension is used to derive nanothermodynamic generalizations of the Young–Laplace and Young equations. The resulting equations account for the size-and shape dependence of the finite thermodynamic contributions and recover the classical equilibrium equations in the macroscopic limit.

Related

  1. Do good neighbours compensate for bad climate? The case of sessile oak Quercus petraea in phylogenetically distant neighbourhoods
    Keliang Zhang, Vincent Jung, Maud Deniau +5
    OikosPeer-reviewedCC BY 4.0Full textEcologyEnvironmental science & pollutionHAL
  2. Preferential concentration of cloud droplets: Coupled effects of phase change and gravitational settling
    Zi-Mo Liao
    arXivPreprintarXiv licenceFull textAtmospheric science & meteorologyFluid dynamicsarXiv
  3. Nitrite to Nitrate Spontaneous Oxidation in Suspended Aqueous Droplets
    C. Meroni, Adrien Gandolfo, C. George
    Geophysical Research LettersPeer-reviewedCC BY 4.0Full textTheoretical & computational chemistryAtmospheric science & meteorologyHAL
  4. Stochastic homogeneous freezing of supercooled droplets in mixed-phase clouds in particle-based idealised microphysics framework (exemplified with PySDM v3.0)
    Tim Lüttmer, Sylwester Arabas, Peter Spichtinger
    Geoscientific Model DevelopmentPeer-reviewedCC BY 4.0Full textClimate scienceCrossref
  5. Immunodetection of a Cell-Surface Biomarker via the Freezing of Supercooled Water Droplets
    Paul Bieber, Ghinwa H. Darwish, Paris Salamon +3
    ChemRxivPreprintCC BY-NC-NDFull textAtmospheric science & meteorologyChemRxiv
BibTeX
@misc{cunha2026nanothermodynamic,
  title = {{Nanothermodynamic Generalization of the Young–Laplace and Young Equations for Sessile Droplets with Line Effects}},
  author = {Vitor H. C. Cunha and Signe Kjelstrup and Dick Bedeaux},
  howpublished = {ChemRxiv},
  year = {2026},
  month = sep,
  doi = {10.26434/chemrxiv.15008838/v1},
  url = {https://chemrxiv.org/doi/full/10.26434/chemrxiv.15008838/v1},
  note = {CC BY},
}
RIS
TY  - UNPB
TI  - Nanothermodynamic Generalization of the Young–Laplace and Young Equations for Sessile Droplets with Line Effects
AU  - Vitor H. C. Cunha
AU  - Signe Kjelstrup
AU  - Dick Bedeaux
PY  - 2026
DA  - 2026/09/15
PB  - ChemRxiv
DO  - 10.26434/chemrxiv.15008838/v1
UR  - https://chemrxiv.org/doi/full/10.26434/chemrxiv.15008838/v1
AB  - Thermodynamic investigations of wetting phenomena require that we handle the nanoscale. By combining Hill’s small-system thermodynamics with a Gibbsian composite-system description, we formulate the equilibrium thermodynamics of a sessile nanodroplet. We consider a one-component liquid droplet resting on an ideal, flat, inert solid substrate and in contact with reservoirs that fix the temperature and chemical potential. Finite-size effects are retained in the liquid bulk phase, the liquid–vapor interface, and the three-phase contact line, while the solid–vapor and solid–liquid interfaces are assumed to follow regular thermodynamics and treated macroscopically. The distinction between integral and differential pressure, surface tension, and line tension is used to derive nanothermodynamic generalizations of the Young–Laplace and Young equations. The resulting equations account for the size-and shape dependence of the finite thermodynamic contributions and recover the classical equilibrium equations in the macroscopic limit.
ER  -