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Contact Angle01:13

Contact Angle

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When a solid is dipped inside a liquid, the liquid surface becomes curved near the contact. For some solid–liquid interfaces, the liquid is pulled up along the solid, while for others, the liquid surface is convex or depressed near the solid surface. This phenomenon can be explained using the concept of cohesive and adhesive forces.
The adhesive force is the molecular force between molecules of different materials, that is, between the molecules of the solid and the liquid. The cohesive...
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Microtensiometer for Confocal Microscopy Visualization of Dynamic Interfaces
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Modeling Contact Angles with Chemically Specific Dissipative Particle Dynamics.

Guadalupe Jiménez-Serratos1, Patrick B Warren1, Scott Singleton2

  • 1The Hartree Centre, STFC Daresbury Laboratory, Warrington WA4 4AD, U.K.

Langmuir : the ACS Journal of Surfaces and Colloids
|February 5, 2025
PubMed
Summary
This summary is machine-generated.

We developed a method to introduce walls into dissipative particle dynamics simulations, enabling precise control over surface energies and contact angles for interfaces like oil/water. This approach ensures the Young equation is satisfied, validated by simulations and experiments.

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Area of Science:

  • Computational chemistry and materials science
  • Soft matter physics and interfacial phenomena

Background:

  • Accurately modeling interfacial behavior, such as contact angles, is crucial in diverse fields.
  • Existing simulation methods often struggle to precisely control surface properties and their impact on wetting phenomena.

Purpose of the Study:

  • To introduce and validate a method for incorporating walls into chemically specific dissipative particle dynamics (DPD) models.
  • To enable precise tuning of surface energies to achieve desired contact angles for liquid interfaces.
  • To ensure the developed methodology satisfies the Young equation for accurate wetting predictions.

Main Methods:

  • Developed a technique to introduce chemically specific walls into DPD simulations.
  • Established a procedure for determining wall surface energies (positive or negative) to control contact angles.
  • Validated the DPD methodology against direct numerical simulations of oil-in-water droplets.
  • Tested the approach using an experimental model of water droplets on a silica surface with a monolayer.

Main Results:

  • Successfully implemented a DPD framework capable of defining surface energies for introduced walls.
  • Demonstrated that the chosen surface energies automatically satisfy the Young equation, predicting accurate contact angles.
  • Validated the simulation results against independent numerical simulations and experimental data for oil/water and water/oil systems.

Conclusions:

  • The proposed DPD methodology provides a robust and accurate way to model interfacial phenomena with controlled wetting.
  • This approach offers a valuable tool for designing and simulating complex fluid-surface interactions in materials science and nanotechnology.
  • The ability to tune surface energies and satisfy the Young equation enhances the predictive power of DPD for interfacial engineering.