Jove
Visualize
Contact Us

Related Concept Videos

Viscosity of Fluid01:19

Viscosity of Fluid

2.2K
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.
2.2K
Design Example: Deciding Thickness of Lubricating Fluid in a Shaft01:23

Design Example: Deciding Thickness of Lubricating Fluid in a Shaft

392
Effective lubrication between a rotating shaft and its bearing housing is essential in rotating machinery to minimize friction, wear, and energy loss. With carefully controlled thickness and viscosity, the lubricant layer prevents metal-to-metal contact, ensuring smooth operation.
To calculate the required thickness of the lubricant layer, the tangential velocity at the shaft's surface must first be determined. This velocity is calculated by converting the rotational speed to angular velocity...
392
Viscosity01:17

Viscosity

7.9K
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...
7.9K
Viscosity01:27

Viscosity

114
Viscosity is a property of fluids that measures their resistance to flow. It is influenced by factors such as the surface area of contact, the gradient of flow speed, and the fluid's viscosity constant, called the coefficient of viscosity. The coefficient of viscosity, also known as dynamic viscosity, is denoted by the symbol η. It determines the proportionality between the viscous force and the gradient of flow speed.Newton's law of viscosity states that the viscous force on a...
114
Membrane Fluidity01:23

Membrane Fluidity

179.3K
Cell membranes are composed of phospholipids, proteins, and carbohydrates loosely attached to one another through chemical interactions. Molecules are generally able to move about in the plane of the membrane, giving the membrane its flexible nature called fluidity. Two other features of the membrane contribute to membrane fluidity: the chemical structure of the phospholipids and the presence of cholesterol in the membrane.
179.3K
Membrane Fluidity01:26

Membrane Fluidity

17.9K
Membrane fluidity is explained by the fluid mosaic model of the cell membrane, which describes the plasma membrane structure as a mosaic of components—including phospholipids, cholesterol, proteins, and carbohydrates—that gives the membrane a fluid character.
Mosaic nature of the membrane
The mosaic characteristic of the membrane helps the plasma membrane remain fluid. The integral proteins and lipids exist as separate but loosely-attached molecules in the membrane. The membrane is...
17.9K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Spatial Organization of Biomass Controls Intrinsic Permeability of Porous Systems.

Environmental science & technology·2026
Same author

Root and microbial contributions to anoxic microsite formation in the rhizosphere: a microfluidic approach.

The New phytologist·2026
Same author

Stick-slip from heterogeneous Coulomb friction.

Physical review. E·2025
Same author

Enhanced Reaction Kinetics in Stationary Two-Phase Flow through Porous Media.

Environmental science & technology·2025
Same author

Soft matter physics of the ground beneath our feet.

Soft matter·2024
Same author

Dynamic imaging of force chains in 3D granular media.

Proceedings of the National Academy of Sciences of the United States of America·2024
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Experiment Video

Updated: Mar 30, 2026

Combining Microfluidics and Microrheology to Determine Rheological Properties of Soft Matter during Repeated Phase Transitions
11:38

Combining Microfluidics and Microrheology to Determine Rheological Properties of Soft Matter during Repeated Phase Transitions

Published on: April 19, 2018

8.6K

Interface evolution during radial miscible viscous fingering.

Jane Y Y Chui1, Pietro de Anna1, Ruben Juanes1

  • 1Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, Massachusetts 02139, USA.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|November 14, 2015
PubMed
Summary

We observed two fluid displacement regimes in a Hele-Shaw cell, transitioning from Saffman-Taylor instability to stable flow. The crossover time unexpectedly decreases with higher injection rates.

More Related Videos

Magnetically Induced Rotating Rayleigh-Taylor Instability
06:42

Magnetically Induced Rotating Rayleigh-Taylor Instability

Published on: March 3, 2017

10.2K
Challenges in Rheological Characterization of Highly Concentrated Suspensions — A Case Study for Screen-printing Silver Pastes
08:42

Challenges in Rheological Characterization of Highly Concentrated Suspensions — A Case Study for Screen-printing Silver Pastes

Published on: April 10, 2017

20.7K

Related Experiment Videos

Last Updated: Mar 30, 2026

Combining Microfluidics and Microrheology to Determine Rheological Properties of Soft Matter during Repeated Phase Transitions
11:38

Combining Microfluidics and Microrheology to Determine Rheological Properties of Soft Matter during Repeated Phase Transitions

Published on: April 19, 2018

8.6K
Magnetically Induced Rotating Rayleigh-Taylor Instability
06:42

Magnetically Induced Rotating Rayleigh-Taylor Instability

Published on: March 3, 2017

10.2K
Challenges in Rheological Characterization of Highly Concentrated Suspensions — A Case Study for Screen-printing Silver Pastes
08:42

Challenges in Rheological Characterization of Highly Concentrated Suspensions — A Case Study for Screen-printing Silver Pastes

Published on: April 10, 2017

20.7K

Area of Science:

  • Fluid Dynamics
  • Instability Phenomena

Background:

  • Miscible fluid displacement is crucial in various scientific and industrial applications.
  • The Saffman-Taylor instability governs early-stage fluid-fluid interface evolution in confined geometries.
  • Understanding displacement regimes is key to optimizing processes like enhanced oil recovery.

Purpose of the Study:

  • To experimentally investigate the radial displacement of a more viscous fluid by a less viscous one in a Hele-Shaw cell.
  • To identify and characterize different regimes of fluid-fluid interface evolution.
  • To develop a theoretical model explaining the observed phenomena and crossover dynamics.

Main Methods:

  • Experimental study using a horizontal Hele-Shaw cell.
  • Controlled variation of injection rates and viscosity ratios.
  • Analysis of fluid-fluid interface evolution over time.
  • Development and validation of a theoretical model.

Main Results:

  • Two distinct regimes of interface evolution were observed: an early-time linear growth (Saffman-Taylor instability) and a later-time slower growth (∼t(1/2)).
  • The crossover time between these regimes unexpectedly decreases with increasing injection rate.
  • A theoretical model was developed, consistent with experimental data, explaining the observed scalings and crossover behavior.

Conclusions:

  • The competition between advection and diffusion time scales at the displacement front dictates the observed interface dynamics.
  • The findings provide insights into the transition from unstable to stable displacement in radial Hele-Shaw flows.
  • The developed model and analysis are applicable to other interfacial evolution problems, including Rayleigh-Bénard-Darcy instability.