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Rise of Liquid in a Capillary Tube01:18

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When very thin cylindrical tubes, called capillaries, are dipped in a liquid, the liquid rises or falls in the tube compared to the surrounding liquid. This phenomenon is called capillary action. Capillary action occurs due to the combination of two opposing forces: the cohesive forces of the liquid, which cause it to stick to itself and form a rounded shape, and the adhesive forces between the liquid and the walls of the container, which cause the liquid to be attracted to the container walls.
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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.
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Capillarity describes the movement of liquid in small spaces without external forces acting on it. The capillarity is driven by surface tension and adhesive interactions between the liquid and surrounding solid surfaces. This effect is often seen in narrow tubes, porous materials, and fine particles.
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Fluid mechanics model studies often utilize scaled-down systems to predict fluid behavior in full-scale environments, such as river flows, dam spillways, and structures interacting with open surfaces. Maintaining Froude number similarity in river models is crucial, as it replicates surface flow features like wave patterns and velocities.
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Surface Tension, Capillary Action, and Viscosity02:57

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Surface Tension
The various IMFs between identical molecules of a substance are examples of cohesive forces. The molecules within a liquid are surrounded by other molecules and are attracted equally in all directions by the cohesive forces within the liquid. However, the molecules on the surface of a liquid are attracted only by about one-half as many molecules. Because of the unbalanced molecular attractions on the surface molecules, liquids contract to form a shape that minimizes the number...
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The shape of a small drop of liquid can be considered spherical, neglecting the effect of gravity. This drop can further be considered as two equal hemispherical drops put together due to surface tension. The forces acting on the spherical drop are due to the pressure of the liquid inside the drop, the pressure due to air outside the drop, and the force due to the surface tension acting on the two hemispherical drops.
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Capillary Rise: Validity of the Dynamic Contact Angle Models.

Pingkeng Wu1, Alex D Nikolov1, Darsh T Wasan1

  • 1Department of Chemical Engineering, Illinois Institute of Technology , Chicago, Illinois 60616, United States.

Langmuir : the ACS Journal of Surfaces and Colloids
|July 20, 2017
PubMed
Summary
This summary is machine-generated.

The Lucas-Washburn-Rideal equation overestimates capillary rise due to dynamic contact angles. Modified models, especially the molecular self-layering approach, accurately predict capillary rise by accounting for wetting film energy dissipation.

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Area of Science:

  • Fluid Dynamics
  • Surface Science
  • Physical Chemistry

Background:

  • The classical Lucas-Washburn-Rideal (LWR) equation often overpredicts capillary rise compared to experimental results.
  • This discrepancy is largely attributed to the influence of velocity-dependent dynamic contact angles, not accounted for in the equilibrium model.

Purpose of the Study:

  • To investigate and compare various dynamic contact angle models for their effectiveness in correcting capillary rise predictions.
  • To analyze the role of molecular-level phenomena in dynamic contact angle effects during capillary rise.

Main Methods:

  • Conducted capillary rise experiments using diverse wetting liquids in borosilicate glass capillaries.
  • Compared experimental data with predictions from LWR equations modified by different dynamic contact angle models (molecular kinetic theory, hydrodynamic, Joos' empirical, molecular self-layering).

Main Results:

  • LWR equations modified by molecular kinetic theory and hydrodynamic models showed good predictions with fitting parameters for all tested liquids.
  • The molecular self-layering model provided accurate predictions for specific liquids (carbon tetrachloride, octamethylcyclotetrasiloxane, n-alkanes) and silicone oils across a range of viscosities.
  • The molecular self-layering model highlighted the significance of the pre-meniscus wetting film in energy dissipation.

Conclusions:

  • The molecular self-layering model offers superior accuracy in predicting capillary rise, emphasizing the importance of molecular film dynamics.
  • This model provides valuable insights into the capillary dynamics of polymer melts and other complex fluids.