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

Steady, Laminar Flow in Circular Tubes01:23

Steady, Laminar Flow in Circular Tubes

318
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...
318
Uniform Depth Channel Flow01:27

Uniform Depth Channel Flow

126
Uniform depth channel flow keeps fluid depth consistent along channels such as irrigation canals. In natural channels, such as rivers, approximate uniform flow is often assumed. This condition occurs when the channel’s bottom slope matches the energy slope, balancing potential energy lost from gravity with head loss due to shear stress. This balance prevents depth changes along the channel length, resulting in a steady, uniform flow.Uniform flow in open channels with a constant cross-section...
126
Uniform Depth Channel Flow: Problem Solving01:18

Uniform Depth Channel Flow: Problem Solving

116
To calculate the flow rate for a trapezoidal channel, first, identify the bottom width, side slope, and flow depth of the channel. The cross-sectional area (A) corresponding to the depth of flow (y), channel bottom width (B), and side slope (θ) is determined by:Next, calculate the wetted perimeter, which includes the bottom width and the sloped side lengths in contact with the water. Using the values of the cross-sectional area and the wetted perimeter, determine the hydraulic radius by...
116
Steady, Laminar Flow Between Parallel Plates01:17

Steady, Laminar Flow Between Parallel Plates

286
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.
286
Couette Flow01:22

Couette Flow

393
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...
393
Rapidly Varying Flow01:24

Rapidly Varying Flow

121
Rapidly varying flow (RVF) in open channels is characterized by abrupt changes in flow depth over a short distance, with the rate of depth change relative to distance often approaching unity. These flows are inherently complex due to their transient and multi-dimensional nature, making exact analysis difficult. However, approximate solutions using simplified models provide valuable insights into their behavior.Key Features of Rapidly Varying FlowRVF is commonly observed in scenarios involving...
121

You might also read

Related Articles

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

Sort by
Same author

A machine learning-based framework to design capillary-driven networks.

Lab on a chip·2022
Same author

Flow-induced self-sustained oscillations in a straight channel with rigid walls and elastic supports.

Bioinspiration & biomimetics·2022
Same author

Ventilator output splitting interface 'ACRA': Description and evaluation in lung simulators and in an experimental ARDS animal model.

PloS one·2021
Same author

Exhalatory dynamic interactions between patients connected to a shared ventilation device.

PloS one·2021
Same author

Three-dimensional confocal Raman temperature characterization of electrokinetically pumped microchannels.

Applied optics·2019
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: Aug 24, 2025

Fabrication, Operation and Flow Visualization in Surface-acoustic-wave-driven Acoustic-counterflow Microfluidics
12:26

Fabrication, Operation and Flow Visualization in Surface-acoustic-wave-driven Acoustic-counterflow Microfluidics

Published on: August 27, 2013

17.3K

Capillary Flow Dynamics in Composite Rectangular Microchannels with Rough Walls.

Pedro Manuel Garcia Eijo1, Juan Martín Cabaleiro1, Guillermo Artana1

  • 1Laboratorio de Fluidodinámica, Facultad de Ingeniería, Universidad de Buenos Aires, C1063ACVBuenos Aires, Argentina.

Langmuir : the ACS Journal of Surfaces and Colloids
|October 21, 2022
PubMed
Summary
This summary is machine-generated.

This study models fluid capillary transport in rectangular microchannels, finding that aspect ratio significantly impacts fluid motion. Rough surfaces reduce the effective contact angle, with effects diminishing after approximately 1 second.

More Related Videos

Development of a Microfluidics-Based Approach for Investigating Microtubule Polymer Mechanics
06:03

Development of a Microfluidics-Based Approach for Investigating Microtubule Polymer Mechanics

Published on: May 30, 2025

271
Procedure for the Development of Multi-depth Circular Cross-sectional Endothelialized Microchannels-on-a-chip
10:55

Procedure for the Development of Multi-depth Circular Cross-sectional Endothelialized Microchannels-on-a-chip

Published on: October 21, 2013

14.0K

Related Experiment Videos

Last Updated: Aug 24, 2025

Fabrication, Operation and Flow Visualization in Surface-acoustic-wave-driven Acoustic-counterflow Microfluidics
12:26

Fabrication, Operation and Flow Visualization in Surface-acoustic-wave-driven Acoustic-counterflow Microfluidics

Published on: August 27, 2013

17.3K
Development of a Microfluidics-Based Approach for Investigating Microtubule Polymer Mechanics
06:03

Development of a Microfluidics-Based Approach for Investigating Microtubule Polymer Mechanics

Published on: May 30, 2025

271
Procedure for the Development of Multi-depth Circular Cross-sectional Endothelialized Microchannels-on-a-chip
10:55

Procedure for the Development of Multi-depth Circular Cross-sectional Endothelialized Microchannels-on-a-chip

Published on: October 21, 2013

14.0K

Area of Science:

  • Physics
  • Materials Science
  • Fluid Dynamics

Background:

  • Capillary transport in microchannels is crucial for microfluidic devices.
  • Microchannel geometry and surface properties, like roughness, influence fluid behavior.
  • Understanding these factors is key to controlling fluid flow at the microscale.

Purpose of the Study:

  • To develop a model for fluid capillary transport in rectangular microchannels with varying wall materials and roughness.
  • To investigate the influence of microchannel aspect ratio on fluid motion during initial viscous regimes.
  • To determine the effective static contact angle and friction coefficient for different aspect ratios and surface roughness.

Main Methods:

  • Development of a fluid capillary transport model for horizontally positioned rectangular microchannels.
  • Utilizing an effective static contact angle and an effective friction coefficient averaged over the cross-section.
  • Conducting extensive experimental investigations with various microchannels to obtain coefficients for different aspect ratios.

Main Results:

  • Lower aspect ratios result in smaller effective contact angles and larger effective friction coefficients.
  • Surface roughness, particularly pinning-depinning events, significantly reduces the effective static contact angle, even at high aspect ratios.
  • Effective friction coefficient values align well with existing literature for both rough and smooth surfaces.

Conclusions:

  • A nondimensional time parameter was proposed to identify when contact angle effects dominate fluid dynamics.
  • Contact angle effects become negligible for times exceeding approximately 1 second for the studied materials and fluid properties.
  • The findings provide insights into optimizing microchannel design for controlled capillary-driven fluid transport.