Jove
Visualize
Contact Us
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 Concept Videos

Fluid Pressure01:14

Fluid Pressure

1.0K
In mechanical engineering, fluid pressure plays a critical role in designing systems that utilize liquid flow, such as hydraulic systems, pumps, and valves. When designing these systems, engineers must ensure they can withstand the forces created by fluid pressure to avoid damage or failure.
According to Pascal's law, a fluid at rest will generate equal pressure in all directions. This pressure is measured as a force per unit area, and its magnitude depends on the fluid's specific...
1.0K
Excess Pressure Inside a Drop and a Bubble01:13

Excess Pressure Inside a Drop and a Bubble

2.9K
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.
2.9K
Concept of Pressure at a Point01:15

Concept of Pressure at a Point

619
The concept of pressure at a point in a fluid establishes that pressure within a fluid is uniform in all directions at a specific location. This uniformity occurs because fluid molecules exert force evenly across any point due to their random motion and continuous collisions within the fluid. Pressure at a point is determined by the surrounding fluid molecules and is influenced by factors like depth and density, rather than by shape or orientation.
In a fluid at rest, pressure acts equally in...
619
Fluid Pressure over Flat Plate of Variable Width01:02

Fluid Pressure over Flat Plate of Variable Width

2.0K
When a flat plate is submerged in a fluid, the fluid exerts pressure on the plate. This pressure can lead to many different phenomena, including drag and buoyancy. To understand the behavior of the fluid over a flat plate of variable width, it is essential to analyze the distribution of the pressure exerted.
The pressure distribution on the plate can be calculated by determining the force that acts on a differential area strip of the plate. Thus, the magnitude of the force is equal to the...
2.0K
Pressure of Fluids01:14

Pressure of Fluids

21.2K
There are many examples of pressure in fluids in everyday life, such as in relation to blood (high or low blood pressure) and in relation to weather (high- and low-pressure weather systems). A given force can have a significantly different effect, depending on the area over which the force is exerted. For instance, a force applied to an area of 1 mm2 has a pressure that is 100 times greater than the same force applied to an area of 1 cm2. That's why a sharp needle is able to poke through...
21.2K
Pressure Variation in a Fluid at Rest01:11

Pressure Variation in a Fluid at Rest

649
In a fluid at rest, the pressure at any point beneath the fluid surface depends solely on the depth, not on the container's shape or size. This principle, known as hydrostatic pressure, arises because, in stationary fluids, there is no acceleration, meaning the forces within the fluid balance out. Only vertical forces, caused by the weight of the fluid above, contribute to pressure changes with depth.
When measuring pressure at two different levels within the fluid, the difference in...
649

You might also read

Related Articles

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

Sort by
Same author

Advanced coarse-grained model for fast simulation of nascent polypeptide chain dynamics within the ribosome.

Biophysical journal·2025
Same author

Nanopolysaccharide Builder: A User-Friendly Tool for Atomistic Models of Polysaccharide-Based Nanostructures.

Journal of chemical information and modeling·2025
Same author

Interaction between the Polyelectrolytes Unfractionated Heparin and Universal Heparin Reversal Agents.

The journal of physical chemistry. B·2024
Same author

3D Printed Cellulose Nanofiber Aerogel Scaffold with Hierarchical Porous Structures for Fast Solar-Driven Atmospheric Water Harvesting.

Advanced materials (Deerfield Beach, Fla.)·2023
Same author

Geometric differences in the ribosome exit tunnel impact the escape of small nascent proteins.

Biophysical journal·2022
Same author

Competing Effects of Hydration and Cation Complexation in Single-Chain Alginate.

Biomacromolecules·2022
Same journal

Metal-Organic Framework Multizyme Colloids with Joint Antioxidant and Protease Function.

Langmuir : the ACS journal of surfaces and colloids·2026
Same journal

Morphology Engineering of Co<sub>3</sub>O<sub>4</sub> via Cetyltrimethylammonium Bromide-Mediated ZIF-67 Synthesis for Efficient Photo-Assisted Electrooxidation of Methanol.

Langmuir : the ACS journal of surfaces and colloids·2026
Same journal

Speciation of Silanol Groups on Commercial Precipitated Silicas via IR Spectroscopy.

Langmuir : the ACS journal of surfaces and colloids·2026
Same journal

Regenerable PVA Hydrogel-Functionalized Optical Fiber Sensor for Ultra-Trace Detection of Berberine Hydrochloride.

Langmuir : the ACS journal of surfaces and colloids·2026
Same journal

Hydrogen Plasma-Driven Surface Defect Engineering of ZnO Nanorods: Correlating Electronic Structure and Photoelectrochemical Performance.

Langmuir : the ACS journal of surfaces and colloids·2026
Same journal

Cooperative Self-Assembly of Nanoparticle-Encapsulating Hybrid Protein Cages.

Langmuir : the ACS journal of surfaces and colloids·2026
See all related articles

Related Experiment Video

Updated: Dec 18, 2025

Microtensiometer for Confocal Microscopy Visualization of Dynamic Interfaces
08:05

Microtensiometer for Confocal Microscopy Visualization of Dynamic Interfaces

Published on: September 9, 2022

2.7K

Negative Pressure within a Liquid-Fluid Interface Determines Its Thickness.

Simcha Srebnik1, Abraham Marmur2

  • 1Department of Chemical and Biological Engineering, University of British Columbia, Vancouver, British Columbia V6T 1Z4, Canada.

Langmuir : the ACS Journal of Surfaces and Colloids
|June 20, 2020
PubMed
Summary
This summary is machine-generated.

The study reveals that the high stress difference in fluid interfaces, previously unexplained, is due to negative interfacial stresses. This finding reconciles theoretical predictions with experimental observations of interface thickness.

More Related Videos

Studying Surfactant Effects on Hydrate Crystallization at Oil-Water Interfaces Using a Low-Cost Integrated Modular Peltier Device
06:31

Studying Surfactant Effects on Hydrate Crystallization at Oil-Water Interfaces Using a Low-Cost Integrated Modular Peltier Device

Published on: March 18, 2020

6.7K
Visualization of High Speed Liquid Jet Impaction on a Moving Surface
08:34

Visualization of High Speed Liquid Jet Impaction on a Moving Surface

Published on: April 17, 2015

11.9K

Related Experiment Videos

Last Updated: Dec 18, 2025

Microtensiometer for Confocal Microscopy Visualization of Dynamic Interfaces
08:05

Microtensiometer for Confocal Microscopy Visualization of Dynamic Interfaces

Published on: September 9, 2022

2.7K
Studying Surfactant Effects on Hydrate Crystallization at Oil-Water Interfaces Using a Low-Cost Integrated Modular Peltier Device
06:31

Studying Surfactant Effects on Hydrate Crystallization at Oil-Water Interfaces Using a Low-Cost Integrated Modular Peltier Device

Published on: March 18, 2020

6.7K
Visualization of High Speed Liquid Jet Impaction on a Moving Surface
08:34

Visualization of High Speed Liquid Jet Impaction on a Moving Surface

Published on: April 17, 2015

11.9K

Area of Science:

  • Physical Chemistry
  • Thermodynamics
  • Materials Science

Background:

  • Fluid interfaces exhibit gradual density changes over nanometer scales.
  • Existing models like the Bakker equation predict unrealistically large interface thicknesses when assuming ambient pressure stress differences.
  • Experimental data suggest interface thicknesses are typically 10 nm or less, implying significant interfacial stress.

Purpose of the Study:

  • To investigate the discrepancy between theoretical predictions and experimental observations of fluid interface thickness.
  • To explain the origin of the surprisingly high average stress difference within fluid interfaces.
  • To demonstrate that negative stresses are responsible for the observed interfacial properties.

Main Methods:

  • Analysis of the Bakker equation and its implications for interfacial stress and thickness.
  • Theoretical modeling incorporating negative stress components within the interface.
  • Comparison of theoretical predictions with experimental data on fluid interfaces.

Main Results:

  • Theoretical calculations indicate that negative stresses within the interface are essential for reconciling predicted and observed thicknesses.
  • The Bakker equation, when accounting for negative stresses, yields interface thicknesses consistent with experimental measurements.
  • A high average stress difference (∼5 × 10^6 N/m^2) is shown to arise from these negative stress contributions.

Conclusions:

  • Negative stresses within fluid interfaces are a critical factor in determining their thickness.
  • The presence of negative stresses resolves the conflict between thermodynamic theory and experimental findings regarding interfacial properties.
  • This work provides a more accurate theoretical framework for understanding the behavior of fluid interfaces.