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

Maxwell-Boltzmann Distribution: Problem Solving01:20

Maxwell-Boltzmann Distribution: Problem Solving

1.8K
Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
1.8K
Distribution of Molecular Speeds01:27

Distribution of Molecular Speeds

4.2K
The motion of molecules in a gas is random in magnitude and direction for individual molecules, but a gas of many molecules has a predictable distribution of molecular speeds. This predictable distribution of molecular speeds is known as the Maxwell-Boltzmann distribution. The distribution of molecular speeds in liquids is comparable to that of gases but not identical and can help to understand the phenomenon of the boiling and vapor pressure of a liquid. Consider that a molecule requires a...
4.2K
Bernoulli's Equation for Flow Along a Streamline01:30

Bernoulli's Equation for Flow Along a Streamline

1.1K
Bernoulli's equation relates the energy conservation in a fluid moving along a streamline. The equation applies to incompressible and inviscid fluids under steady flow. For such a flow, Newton's second law is applied to a small fluid element, which experiences forces due to pressure differences, gravity, and velocity variations. The force balance leads to the following form of Bernoulli's equation:
1.1K
Bernoulli's Equation00:59

Bernoulli's Equation

11.0K
In the middle of the nineteenth century, it was observed that two trains passing each other at a high relative speed get pulled towards each other. The same occurs when two cars pass each other at a high relative speed. The reason is that the fluid pressure drops in the region where the fluid speeds up. As the air between the trains or the cars increases in speed, its pressure reduces. The pressure on the outer parts of the vehicles is still the atmospheric pressure, while the resultant...
11.0K
Accelerating Fluids01:17

Accelerating Fluids

1.5K
When a fluid is in constant acceleration, the pressure and buoyant force equations are modified. Suppose a beaker is placed in an elevator accelerating upward with a constant acceleration, a. In the beaker, assume there is a thin cylinder of height h with an infinitesimal cross-sectional area, ΔS.
The motion of the liquid within this infinitesimal cylinder is considered to obtain the pressure difference. Three vertical forces act on this liquid:
1.5K
Bernoulli's Equation for Flow Normal to a Streamline01:16

Bernoulli's Equation for Flow Normal to a Streamline

946
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.
946

You might also read

Related Articles

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

Sort by
Same author

Environmental regulation and agricultural green productivity growth in China: A retest based on 'Porter Hypothesis'.

Environmental technology·2023
Same author

Multifunctional DNA Tetrahedron for Alzheimer's Disease Mitochondria-Targeted Therapy by MicroRNA Regulation.

ACS applied materials & interfaces·2023
Same author

A covalent crosslinking strategy to construct a robust peptide-based artificial esterase.

Soft matter·2023
Same author

Experience of using a virtual reality rehabilitation management platform for breast cancer patients: a qualitative study.

Supportive care in cancer : official journal of the Multinational Association of Supportive Care in Cancer·2023
Same author

Sex differences in patients with heart failure and mildly reduced left ventricular ejection fraction.

Scientific reports·2023
Same author

Deep learning-powered 3D segmentation derives factors associated with lymphovascular invasion and prognosis in clinical T1 stage non-small cell lung cancer.

Heliyon·2023
Same journal

Demonstration of a quantum C-NOT gate in a time-multiplexed fully reconfigurable photonic processor.

Nature communications·2026
Same journal

Nonlinear quantum light source with van der Waals ferroelectric NbOX<sub>2</sub> (X = Br, I).

Nature communications·2026
Same journal

Antagonistic histone H2A variants and autonomous heterochromatin formation shape epigenomic patterns in Arabidopsis.

Nature communications·2026
Same journal

The long tail of nitrate pollution in groundwater challenges governance of global water quality.

Nature communications·2026
Same journal

Select microbial metabolites promote tau aggregation in a murine tauopathy model.

Nature communications·2026
Same journal

Warming climate has lengthened global intense tropical cyclone seasons.

Nature communications·2026
See all related articles

Related Experiment Video

Updated: Sep 15, 2025

Blast Quantification Using Hopkinson Pressure Bars
09:41

Blast Quantification Using Hopkinson Pressure Bars

Published on: July 5, 2016

9.2K

Flow perturbation to accelerate Boltzmann sampling.

Xin Peng1, Ang Gao2

  • 1School of Physical Science and Technology, Beijing University of Posts and Telecommunications, Beijing, China.

Nature Communications
|July 17, 2025
PubMed
Summary
This summary is machine-generated.

We developed a novel flow perturbation method for faster and more accurate Boltzmann sampling in complex systems. This technique significantly speeds up computations for molecular simulations, overcoming previous limitations.

More Related Videos

Three-dimensional Particle Tracking Velocimetry for Turbulence Applications: Case of a Jet Flow
13:02

Three-dimensional Particle Tracking Velocimetry for Turbulence Applications: Case of a Jet Flow

Published on: February 27, 2016

12.4K
Simultaneous Measurement of Turbulence and Particle Kinematics Using Flow Imaging Techniques
10:53

Simultaneous Measurement of Turbulence and Particle Kinematics Using Flow Imaging Techniques

Published on: March 12, 2019

7.2K

Related Experiment Videos

Last Updated: Sep 15, 2025

Blast Quantification Using Hopkinson Pressure Bars
09:41

Blast Quantification Using Hopkinson Pressure Bars

Published on: July 5, 2016

9.2K
Three-dimensional Particle Tracking Velocimetry for Turbulence Applications: Case of a Jet Flow
13:02

Three-dimensional Particle Tracking Velocimetry for Turbulence Applications: Case of a Jet Flow

Published on: February 27, 2016

12.4K
Simultaneous Measurement of Turbulence and Particle Kinematics Using Flow Imaging Techniques
10:53

Simultaneous Measurement of Turbulence and Particle Kinematics Using Flow Imaging Techniques

Published on: March 12, 2019

7.2K

Area of Science:

  • Computational chemistry
  • Statistical mechanics
  • Machine learning

Background:

  • Flow-based generative models are used for Boltzmann sampling.
  • High-dimensional systems present computational challenges due to Jacobian calculation costs.
  • Existing methods like the Hutchinson estimator have limitations.

Purpose of the Study:

  • To introduce a computationally efficient method for Boltzmann sampling.
  • To overcome the bottleneck of Jacobian computation in flow-based models.
  • To accelerate and improve the accuracy of sampling in high-dimensional systems.

Main Methods:

  • Developed a flow perturbation method by injecting stochastic perturbations.
  • Bypassed the need for direct Jacobian computation.
  • Applied the method to Boltzmann sampling of molecular systems.

Main Results:

  • Achieved orders-of-magnitude speed-ups in computations.
  • Demonstrated an inherently unbiased approach for Boltzmann sampling.
  • Significantly accelerated Boltzmann sampling of a Chignolin mutant.
  • Delivered more accurate results compared to the Hutchinson estimator.

Conclusions:

  • The flow perturbation method offers a significant advancement for Boltzmann sampling.
  • This approach effectively addresses computational costs in high-dimensional systems.
  • The method shows promise for applications in molecular dynamics and computational chemistry.