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

Shock Waves01:16

Shock Waves

While deriving the Doppler formula for the observed frequency of a sound wave, it is assumed that the speed of sound in the medium is greater than the source's speed through it. When this condition is breached, a shock wave occurs.
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high pressures...
Surface Tension01:24

Surface Tension

Surface tension is defined as the force per unit length (γ) acting along the surface of a liquid. It arises due to strong intermolecular forces of attraction. A molecule located inside the bulk of the liquid is surrounded by other molecules and experiences equal forces in all directions. However, a molecule at the surface experiences unbalanced forces because there are more neighboring molecules below than above. This creates a net inward force that pulls surface molecules toward the interior,...
Surface Tension of Fluid01:22

Surface Tension of Fluid

Surface tension is a fundamental property of fluids, occurring at the boundary between a liquid and a gas or between two immiscible liquids. This phenomenon arises from the cohesive forces between molecules at the fluid's surface, creating an effect similar to a stretched elastic membrane. Inside each fluid, molecules are equally attracted in all directions by neighboring molecules, but surface molecules experience a net inward force, resulting in surface tension.
Surface tension varies with...
Hydrostatic Pressure Force on a Plane Surface01:04

Hydrostatic Pressure Force on a Plane Surface

When a plane surface is submerged in a fluid, hydrostatic forces develop on the surface due to the fluid's pressure. For horizontal surfaces, the pressure exerted by the fluid is uniform because the depth remains constant. The resultant force is determined by the pressure at the given depth multiplied by the area of the surface, and it acts through the centroid of the surface. For vertical surfaces, the pressure varies with depth, increasing as the distance from the fluid's free surface...
Hydrostatic Pressure Force on a Curved Surface01:04

Hydrostatic Pressure Force on a Curved Surface

Hydrostatic pressure on curved surfaces is a fundamental concept in fluid mechanics with broad applications in the civil engineering field. When fluid is in contact with a curved surface, as in a reservoir, dam, or storage tank, it exerts pressure that varies in magnitude and direction along the curved surface. To assess the total hydrostatic force exerted by the fluid on a curved structure, engineers typically isolate the fluid volume adjacent to the surface and analyze the forces acting on...
Rapidly Varying Flow01:24

Rapidly Varying Flow

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...

You might also read

Related Articles

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

Sort by
Same author

Gapless tunable intense terahertz pulse generation in strained diamond.

Light, science & applications·2026
Same author

Spatiotemporal Cooling and Diffusion of Hot Interlayer Excitons in Moiré-Potential-Suppressed WSe<sub>2</sub>/WS<sub>2</sub> Heterostructures.

ACS nano·2025
Same author

Pressure-Driven One-Dimensional Superlattices in Monolayer Crystals on a Vicinal Surface.

Nano letters·2025
Same author

A novel scheme for ultrashort terahertz pulse generation over a gapless wide spectral range: Raman-resonance-enhanced four-wave mixing.

Light, science & applications·2023
Same author

Biochemical and histopathological evaluation of changes in sled dog paw skin associated with physical stress and cold temperatures.

Veterinary dermatology·2021
Same author

Elastic ice microfibers.

Science (New York, N.Y.)·2021

Related Experiment Video

Updated: Jul 9, 2026

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

Ultrafast vibrational dynamics at water interfaces.

John A McGuire1, Y Ron Shen

  • 1Department of Physics, University of California, Berkeley, CA 94720, USA.

Science (New York, N.Y.)
|September 30, 2006
PubMed
Summary

Ultrafast vibrational dynamics at water interfaces were studied using time-resolved sum-frequency vibrational spectroscopy. Findings show sub-picosecond relaxation for bonded OH stretches, similar to bulk water, and 1.3 picosecond relaxation for dangling OH stretches.

Area of Science:

  • Physical Chemistry
  • Spectroscopy
  • Interface Science

Background:

  • Water's unique hydrogen-bonding network influences its properties.
  • Understanding interfacial water dynamics is crucial for various chemical and biological processes.
  • Ultrafast dynamics at interfaces remain less explored than bulk water dynamics.

Purpose of the Study:

  • To investigate the ultrafast vibrational dynamics of neat water interfaces.
  • To characterize the relaxation behavior of interfacial OH stretch modes.
  • To compare interfacial water dynamics with bulk water.

Main Methods:

  • Utilized time-resolved sum-frequency vibrational spectroscopy (TR-SFVS).
  • Focused on interfacial bonded and dangling OH stretch modes.

More Related Videos

Measurement of Dynamic Force Acted on Water Strider Leg Jumping Upward by the PVDF Film Sensor
07:17

Measurement of Dynamic Force Acted on Water Strider Leg Jumping Upward by the PVDF Film Sensor

Published on: August 3, 2018

Impacts of Free-falling Spheres on a Deep Liquid Pool with Altered Fluid and Impactor Surface Conditions
08:49

Impacts of Free-falling Spheres on a Deep Liquid Pool with Altered Fluid and Impactor Surface Conditions

Published on: February 17, 2019

Related Experiment Videos

Last Updated: Jul 9, 2026

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

Measurement of Dynamic Force Acted on Water Strider Leg Jumping Upward by the PVDF Film Sensor
07:17

Measurement of Dynamic Force Acted on Water Strider Leg Jumping Upward by the PVDF Film Sensor

Published on: August 3, 2018

Impacts of Free-falling Spheres on a Deep Liquid Pool with Altered Fluid and Impactor Surface Conditions
08:49

Impacts of Free-falling Spheres on a Deep Liquid Pool with Altered Fluid and Impactor Surface Conditions

Published on: February 17, 2019

  • Analyzed spectral diffusion, vibrational relaxation, and dephasing times.
  • Main Results:

    • Interfacial bonded OH stretch modes exhibit sub-picosecond relaxation, mirroring bulk water behavior.
    • Dephasing of excitation occurs within 100 femtoseconds.
    • Dangling OH stretch population relaxation shows a time constant of 1.3 picoseconds.

    Conclusions:

    • TR-SFVS provides insights into ultrafast interfacial water dynamics.
    • Interfacial water relaxation processes are comparable to those in bulk water.
    • The study highlights the role of the hydrogen-bonding network in interfacial water dynamics.