Related Experiment Video
Updated: May 26, 2025

10:56
Confocal Imaging of Confined Quiescent and Flowing Colloid-polymer Mixtures
Published on: May 20, 2014
12.1K
Emergence of Capillary Waves in Miscible Coflowing Fluids
Alessandro Carbonaro1, Giovanni Savorana1, Luca Cipelletti1,2
1Laboratoire Charles Coulomb (L2C), UMR 5221 CNRS-Universitè de Montpellier, F-34095 Montpellier, France.
Physical Review Letters
|February 21, 2025
Summary
We discovered capillary waves at the interface of miscible fluids, enabling measurement of transient interfacial tension. This finding challenges existing fluid dynamics models and opens new research avenues.
Area of Science:
- Fluid Dynamics
- Interfacial Science
- Wave Phenomena
Background:
- Capillary waves are typically observed at interfaces between immiscible fluids.
- Understanding fluid interfaces is crucial for various industrial and scientific applications.
Purpose of the Study:
- To investigate the existence and behavior of capillary waves at the interface of miscible coflowing fluids.
- To develop a method for measuring transient interfacial tension in miscible systems.
- To explore the transition between different wave regimes in confined fluid flows.
Main Methods:
- Experimental observation of capillary waves in coflowing miscible fluids.
- Analysis of wave number-frequency scaling to identify different flow regimes.
- Development of a theoretical model to explain observed phenomena and measure interfacial tension.
Main Results:
- Demonstrated the existence of capillary waves at miscible fluid interfaces.
- Identified a transition from an inertial regime (k∼ω^{0}) to a capillary wave regime (k∼ω^{2/3}).
- Successfully measured effective interfacial tension and its rapid decay on millisecond timescales.
Conclusions:
- The interplay of transient interfacial stresses and confinement drives capillary wave formation in miscible fluids.
- This work provides a novel method for measuring transient interfacial tension at unprecedentedly short timescales.
- The findings extend the understanding of interfacial dynamics in miscible fluid systems.
More Related Videos
Related Concept Videos
Rise of Liquid in a Capillary Tube
1.3K
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.
1.3K
Capillarity in Fluid
97
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...
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...
97
Couette Flow
183
Couette flow represents the flow of fluid between two parallel plates, with one plate fixed and the other moving with a constant velocity. This configuration allows for a simplified analysis using the Navier-Stokes equations, which govern fluid motion under conditions of viscosity and incompressibility. For Couette flow, the assumptions include a steady, laminar, incompressible flow with a zero-pressure gradient in the flow direction. This flow type is beneficial for understanding shear-driven...
183
Steady Flow of a Fluid Stream
232
Consider a control volume, such as a pipe with solid boundaries, through which fluid flows and changes direction due to the impulse exerted by the resulting force from the pipe walls. In steady flow, the mass of fluid entering the control volume at a given time, t, with velocity v1, is equal to the mass leaving after infinitesimal time dt, with velocity v2.
During this process, the momentum of the fluid within the control volume remains constant over the time interval dt. By applying the...
During this process, the momentum of the fluid within the control volume remains constant over the time interval dt. By applying the...
232

