Evidence map›Paper›PMID 39259594›Full record

ArticleProceedings of the National Academy of Sciences of the United States of America2024

The role of the water contact layer on hydration and transport at solid/liquid interfaces.

J Gäding, V Della Balda, J Lan, J Konrad, M Iannuzzi, R H Meißner, G Tocci

Abstract read
In one paragraph

Article in Proceedings of the National Academy of Sciences of the United States of America, 2024. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 5 papers.

0numbers the graph read from it
0cells of the map it votes in
5citing papers in PubMed
–field-weighted citation impact
1 · What the graph read from it

What it found

Each row is one number read from the abstract, on the scale the paper reported it, with its interval. Left of the dashed line favours the treatment, right favours the comparator. Under each row is the sentence it came from. New to these charts? A ten-minute tutorial.

The abstract states no effect estimate the extractor could read, or names no intervention and outcome on the map, so this paper lights no cell and moves no belief. It is still indexed, cited and linked below.

2 · The registry

The trial behind it

Trials whose registry record cites this paper, or whose number appears in the abstract. A trial that started after this paper was published is citing it as background, not reporting it.

Neither the registry nor the abstract names a trial number. If this is a trial report, that itself is worth knowing.

3 · Its place in the literature

Who cites it

5 citing papers in PubMed.

  1. Article
  2. Article
  3. Article
  4. Review
  5. The role of the water contact layer on hydration and transport at solid/liquid interfaces.Proceedings of the National Academy of Sciences of the United States of America · 2024
    Article
4 · The record

Corrections and comments

PubMed lists nothing against this paper. Absence here is not a guarantee, only a check that was made.

5 · Who and what money

Authors and funding

7 authors.

J GädingInstitute of Soft Matter Modeling, Hamburg University of Technology, Hamburg 21073, Germany.ORCID 0000-0002-4690-2849
V Della BaldaDepartment of Chemistry, University of Zurich, Zurich 8057, Switzerland.ORCID 0009-0008-0632-3720
J LanDepartment of Chemistry, New York University, New York, NY 10003.
J KonradInstitute of Soft Matter Modeling, Hamburg University of Technology, Hamburg 21073, Germany.ORCID 0000-0002-8466-9291
M IannuzziDepartment of Chemistry, University of Zurich, Zurich 8057, Switzerland.ORCID 0000-0001-9717-2527
R H MeißnerInstitute of Soft Matter Modeling, Hamburg University of Technology, Hamburg 21073, Germany.ORCID 0000-0003-1926-114X
G TocciDepartment of Chemistry, University of Zurich, Zurich 8057, Switzerland.ORCID 0000-0001-9118-9758

Funding

Deutsche Forschungsgemeinschaft (DFG) 192346071Deutsche Forschungsgemeinschaft (DFG) 39079442Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung (SNF) PZ00P2_179964Simons Foundation (SF) n/a
6 · The paper itself

Abstract

Understanding the structure in the nanoscopic region of water that is in direct contact with solid surfaces, so-called contact layer, is key to quantifying macroscopic properties that are of interest to e.g. catalysis, ice nucleation, nanofluidics, gas adsorption, and sensing. We explore the structure of the water contact layer on various technologically relevant solid surfaces, namely graphene, MoS[Formula: see text], Au(111), Au(100), Pt(111), and Pt(100), which have been previously hampered by time and length scale limitations of ab initio approaches or force field inaccuracies, by means of molecular dynamics simulations based on ab initio machine learning potentials built using an active learning scheme. Our results reveal that the in-plane intermolecular correlations of the water contact layer vary greatly among different systems: Whereas the contact layer on graphene and on Au(111) is predominantly homogeneous and isotropic, it is inhomogeneous and anisotropic on MoS[Formula: see text], on Au(100), and on the Pt surfaces, where it additionally forms two distinct sublayers. We apply hydrodynamics and the theory of the hydrophobic effect, to relate the energy corrugation and the characteristic length-scales of the contact layer with wetting, slippage, the hydration of small hydrophobic solutes and diffusio-osmotic transport. Thus, this work provides a microscopic picture of the water contact layer and links it to macroscopic properties of liquid/solid interfaces that are measured experimentally and that are relevant to wetting, hydrophobic solvation, nanofluidics, and osmotic transport.

Indexed as

aqueous interfacesmachine learningmolecular dynamicsnanofluidics

Identifiers

PMID39259594
PMCPMC11420213

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Read under generation 80e0d062 · epoch 390. Bibliography from PubMed, PubMed Central and OpenAlex; grants from NIH RePORTER; trial links from ClinicalTrials.gov; estimates, votes and beliefs from the OpenQuestion graph.