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Surface Tension, Capillary Action, and Viscosity02:57

Surface Tension, Capillary Action, and Viscosity

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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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Viscosity of Fluid01:19

Viscosity of Fluid

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Viscosity measures the resistance a fluid offers to flow and deformation. It results from internal friction between layers of fluid moving relative to one another. Dynamic viscosity, denoted by the Greek letter mu (μ), quantifies the force needed to move one fluid layer over another. For Newtonian fluids like water and air, the relationship between the shearing stress and the rate of shearing strain is linear, meaning their viscosity remains constant regardless of the applied stress.
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Surface Tension of Fluid01:22

Surface Tension of Fluid

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Surface tension is a fundamental property of fluids, occurring at the boundary between a liquid and a gas or between two immiscible liquids. This phenomenon arises from the cohesive forces between molecules at the fluid's surface, creating an effect similar to a stretched elastic membrane. Inside each fluid, molecules are equally attracted in all directions by neighboring molecules, but surface molecules experience a net inward force, resulting in surface tension.
Surface tension varies...
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Viscosity01:17

Viscosity

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When water is poured into a glass, it falls freely and quickly, whereas if honey or maple syrup is poured over a pancake, it flows slowly and sticks to the surface of the container. This difference in the flow of different kinds of liquids arises due to the fluid friction between the liquid layers and the liquid and the surrounding material. This property of fluids is called fluid viscosity. In this example, water has a lower viscosity than honey and maple syrup.
The SI unit of viscosity is...
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Theories of Dissolution: The Danckwerts' Model and Interfacial Barrier Model01:09

Theories of Dissolution: The Danckwerts' Model and Interfacial Barrier Model

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Various dissolution theories provide insight into the factors that influence the dissolution rate. Danckwerts' Model suggests that turbulence, rather than a stagnant layer, characterizes the dissolution medium at the solid-liquid interface. In this model, the agitated solvent contains macroscopic packets that move to the interface via eddy currents, facilitating the absorption and delivery of the drug to the bulk solution. The regular replenishment of solvent packets maintains the...
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Capillarity in Fluid01:19

Capillarity in Fluid

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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.
Surface tension is crucial to capillarity. It results from cohesive forces between liquid molecules at the liquid-air boundary, forming a skin that resists external forces. When the capillary tube...
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Updated: Sep 7, 2025

Sample Preparation in Quartz Crystal Microbalance Measurements of Protein Adsorption and Polymer Mechanics
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Wetting dynamics of viscoelastic solid films.

Tetsuo Yamaguchi1, Masatoshi Morishita2, Tomohiko G Sano3

  • 1Department of Biomaterial Sciences, The University of Tokyo, Tokyo 113-8657, Japan. yamaguchi-tetsuo@g.ecc.u-tokyo.ac.jp.

Soft Matter
|June 20, 2022
PubMed
Summary
This summary is machine-generated.

We investigated the wetting of soft viscoelastic films on substrates. At low speeds, wetting is smooth, but higher speeds cause wavy contact lines and air bubbles due to buckling, revealing a maximum wetting velocity.

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Area of Science:

  • Materials Science
  • Soft Matter Physics
  • Surface Science

Background:

  • Understanding the wetting behavior of soft viscoelastic materials is crucial for applications in coatings, adhesives, and microfluidics.
  • The dynamics of contact line motion are complex and influenced by material properties and external conditions.

Purpose of the Study:

  • To investigate the wetting phenomena of a soft viscoelastic solid film on a smooth substrate.
  • To explore the influence of stage velocity on the dynamics of rubber-glass-air contact lines.
  • To identify the underlying mechanisms governing wetting behavior in viscoelastic films.

Main Methods:

  • Experiments involving a poly-dimethylsiloxane (PDMS) rubber film suspended and lowered onto a glass substrate at constant velocities.
  • Observation of wetting behavior and contact line dynamics.
  • Numerical modeling to reproduce experimental observations with an upper limit on contact line velocity.

Main Results:

  • Wetting dynamics vary with stage velocity; smooth wetting at low velocities, wavy contact lines and air bubble trapping at higher velocities.
  • A critical stage velocity was identified, beyond which contact line velocity decreases.
  • Experimental results were reproduced by a numerical model incorporating a maximum contact line velocity.

Conclusions:

  • The observed wetting behavior is attributed to a transition from tensile to compressive in-plane stress, leading to film buckling above the critical velocity.
  • A maximum wetting velocity exists for viscoelastic solids, significantly impacting their wetting dynamics.
  • This study highlights the importance of considering viscoelasticity and stress states in wetting phenomena.