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

Excess Pressure Inside a Drop and a Bubble01:13

Excess Pressure Inside a Drop and a Bubble

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.
Steady, Laminar Flow Between Parallel Plates01:17

Steady, Laminar Flow Between Parallel Plates

Understanding steady, laminar flow between parallel plates is essential for analyzing and designing flow in narrow rectangular channels, commonly found in various water conveyance and drainage systems. The Navier-Stokes equations govern fluid motion and are generally challenging to solve due to their nonlinearity. However, simplifications are possible in certain cases, like the steady laminar flow between parallel plates. For this scenario, we assume steady, incompressible, laminar flow.
Steady, Laminar Flow in Circular Tubes01:23

Steady, Laminar Flow in Circular Tubes

Hagen-Poiseuille flow describes a viscous fluid's steady, incompressible flow through a cylindrical tube with a constant radius R. This flow profile is often applied to understand fluid transport in narrow channels, such as capillaries. It serves as a foundational example of laminar flow. In this model, cylindrical coordinates (r,θ,z) are used to describe the radial (r), angular (θ), and axial (z) dimensions within the tube. For Hagen-Poiseuille flow, the velocity profile is purely axial,...
Fluid Pressure over Flat Plate of Variable Width01:02

Fluid Pressure over Flat Plate of Variable Width

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...
Bernoulli's Equation for Flow Normal to a Streamline01:16

Bernoulli's Equation for Flow Normal to a Streamline

Bernoulli's equation for flow normal to a streamline explains how pressure varies across curved streamlines due to the outward centrifugal forces induced by the fluid's curvature. The pressure is higher on the inner side of the curve, near the center of curvature, and decreases outward to balance these centrifugal forces.
The pressure difference depends on the fluid's velocity and radius of curvature. The pressure variation is minimal in flows with nearly straight streamlines. However, the...
Major Losses in Pipes01:28

Major Losses in Pipes

When a fluid flows through a pipe, it experiences energy losses due to frictional resistance along the pipe walls, known as major losses. These energy losses result in a pressure drop, which varies based on the flow conditions — whether laminar or turbulent — and the specific physical properties of the fluid and pipe.
Fluid flow can be classified as laminar or turbulent, primarily based on the Reynolds number. This dimensionless number reflects the relative influence of inertial to viscous...

You might also read

Related Articles

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

Sort by
Same author

An In Situ Curing, Shear-Responsive Biomaterial Designed for Durable Embolization of Microvasculature.

Advanced healthcare materials·2025
Same author

Point-of-need diagnostics in a post-Covid world: an opportunity for paper-based microfluidics to serve during syndemics.

Lab on a chip·2025
Same author

Mimicking lightning-induced electrochemistry on the early Earth.

Proceedings of the National Academy of Sciences of the United States of America·2024
Same author

Melting of a macroscale binary Coulombic crystal.

Soft matter·2023
Same author

Charge Transport Measured Using the EGaIn Junction through Self-Assembled Monolayers Immersed in Organic Liquids.

The journal of physical chemistry. B·2022
Same author

Programmable soft valves for digital and analog control.

Proceedings of the National Academy of Sciences of the United States of America·2022

Related Experiment Video

Updated: Jul 10, 2026

A Microfluidic System with Surface Patterning for Investigating Cavitation Bubble(s)–Cell Interaction and the Resultant Bioeffects at the Single-cell Level
11:14

A Microfluidic System with Surface Patterning for Investigating Cavitation Bubble(s)–Cell Interaction and the Resultant Bioeffects at the Single-cell Level

Published on: January 10, 2017

The pressure drop along rectangular microchannels containing bubbles.

Michael J Fuerstman1, Ann Lai, Meghan E Thurlow

  • 1Department of Chemistry and Chemical Biology, Harvard University, Cambridge, Massachusetts 02138, USA.

Lab on a Chip
|October 26, 2007
PubMed
Summary

Surfactant concentration significantly impacts pressure drop in microchannels with bubbles. Bubble length dominates at intermediate concentrations, while bubble number is key at low and high concentrations.

More Related Videos

Induction of Microstreaming by Nonspherical Bubble Oscillations in an Acoustic Levitation System
08:19

Induction of Microstreaming by Nonspherical Bubble Oscillations in an Acoustic Levitation System

Published on: May 9, 2021

Related Experiment Videos

Last Updated: Jul 10, 2026

A Microfluidic System with Surface Patterning for Investigating Cavitation Bubble(s)–Cell Interaction and the Resultant Bioeffects at the Single-cell Level
11:14

A Microfluidic System with Surface Patterning for Investigating Cavitation Bubble(s)–Cell Interaction and the Resultant Bioeffects at the Single-cell Level

Published on: January 10, 2017

Induction of Microstreaming by Nonspherical Bubble Oscillations in an Acoustic Levitation System
08:19

Induction of Microstreaming by Nonspherical Bubble Oscillations in an Acoustic Levitation System

Published on: May 9, 2021

Area of Science:

  • Fluid dynamics
  • Microfluidics
  • Surface chemistry

Background:

  • Flow in microchannels is crucial for various applications.
  • Bubbles in microchannels alter flow dynamics and pressure drop.
  • Surfactants are known to modify fluid behavior at interfaces.

Purpose of the Study:

  • To investigate the influence of surfactants on pressure drop in microchannels with bubbles.
  • To quantify the contributions of different channel regions to the overall pressure drop.
  • To understand how bubble characteristics and surfactant concentration affect fluid flow.

Main Methods:

  • Derivation of pressure difference using an indirect method.
  • Analysis of fluid flow in rectangular microchannels containing bubbles.
  • Systematic variation of liquid composition (water, glycerol, surfactants) and bubble presence.

Main Results:

  • Pressure drop is primarily dictated by bubble number at low/high surfactant concentrations.
  • At intermediate surfactant concentrations, aggregated bubble length is the dominant factor.
  • Increased liquid flow in channel 'gutters' at intermediate concentrations explains the difference.

Conclusions:

  • Surfactant concentration is a critical parameter influencing pressure drop in bubbly microchannels.
  • The flow behavior and its impact on pressure drop vary distinctly with surfactant concentration.
  • Understanding these effects is vital for designing and optimizing microfluidic devices.