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Navier–Stokes Equations01:28

Navier–Stokes Equations

409
For incompressible Newtonian fluids, where density remains constant, stresses show a linear relationship with the deformation rate, defined by normal and shear stresses. Normal stresses depend on the pressure exerted on the fluid and the rate of deformation in specific directions, which determines how fluid flows under varying pressures. Shear stresses, on the other hand, act tangentially across fluid layers. They explain how adjacent fluid layers slide relative to one another, connecting...
409
Van der Waals Equation01:10

Van der Waals Equation

3.9K
The ideal gas law is an approximation that works well at high temperatures and low pressures. The van der Waals equation of state (named after the Dutch physicist Johannes van der Waals, 1837−1923) improves it by considering two factors.
First, the attractive forces between molecules, which are stronger at higher densities and reduce the pressure, are considered by adding to the pressure a term equal to the square of the molar density multiplied by a positive coefficient a. Second, the volume...
3.9K
Real Gases: Effects of Intermolecular Forces and Molecular Volume Deriving Van der Waals Equation04:01

Real Gases: Effects of Intermolecular Forces and Molecular Volume Deriving Van der Waals Equation

34.3K
Thus far, the ideal gas law, PV = nRT, has been applied to a variety of different types of problems, ranging from reaction stoichiometry and empirical and molecular formula problems to determining the density and molar mass of a gas. However, the behavior of a gas is often non-ideal, meaning that the observed relationships between its pressure, volume, and temperature are not accurately described by the gas laws. 
34.3K
Euler's Equations of Motion01:28

Euler's Equations of Motion

404
In fluid mechanics, shear stresses arise from viscosity, which represents a fluid's internal resistance to deformation. For low-viscosity fluids, like water, these stresses are minimal, simplifying flow analysis by allowing the fluid to be treated as inviscid, or frictionless. In an inviscid fluid, shear stresses are absent, leaving only normal stresses, which act perpendicularly to fluid elements. Notably, pressure — defined as the negative of the normal stress — remains...
404
Kinetic Theory of an Ideal Gas01:12

Kinetic Theory of an Ideal Gas

3.4K
A mole is defined as the amount of any substance that contains as many molecules as there are atoms in exactly 12 grams of carbon-12. An Italian scientist Amedeo Avogadro (1776–1856) formed the  hypothesis that equal volumes of gas at equal pressure and temperature contain equal numbers of molecules, independent of the type of gas. Later, the hypothesis was developed to form the SI unit for measuring the amount of any substance.
The number of molecules in one mole is called...
3.4K
The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

41.8K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
41.8K

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Related Experiment Video

Updated: May 29, 2025

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

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Navier-Stokes Equations for Nearly Integrable Quantum Gases.

Maciej Łebek1, Miłosz Panfil1

  • 1University of Warsaw, Faculty of Physics, Pasteura 5, 02-093 Warsaw, Poland.

Physical Review Letters
|February 6, 2025
PubMed
Summary

This study demonstrates how Navier-Stokes equations emerge from quantum many-body systems. It reveals two distinct fluid regimes with unique viscous properties, derived from microscopic interactions.

Area of Science:

  • Quantum many-body physics
  • Hydrodynamics
  • Statistical mechanics

Background:

  • The Navier-Stokes equations are fundamental to fluid dynamics.
  • Understanding their microscopic origins in quantum systems is a key challenge.
  • Integrable quantum systems offer a tractable framework for studying emergent hydrodynamics.

Purpose of the Study:

  • To derive the Navier-Stokes equations from the microscopic dynamics of nearly integrable 1D quantum many-body systems.
  • To investigate the role of non-integrable interactions in shaping hydrodynamic behavior.
  • To compute transport coefficients and identify different fluid regimes.

Main Methods:

  • Extension of hydrodynamics for integrable models to include non-integrable interactions.
  • Analysis of the effective Boltzmann equation with a detailed collision integral.

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  • Computation of transport coefficients for specific quantum many-body systems.
  • Main Results:

    • The Navier-Stokes equations are shown to emerge from the studied quantum systems.
    • Two distinct hydrodynamic regimes with differing viscous properties were identified.
    • Transport coefficients were computed for coupled 1D cold-atomic gases, an experimentally relevant system.

    Conclusions:

    • The work provides a microscopic foundation for Navier-Stokes hydrodynamics in a quantum context.
    • The findings highlight the importance of non-integrable interactions in determining fluid properties.
    • The developed method offers a pathway to study hydrodynamics in various complex quantum systems.