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Laminar and Turbulent Flow01:07

Laminar and Turbulent Flow

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Fluid dynamics is the study of fluids in motion. Velocity vectors are often used to illustrate fluid motion in applications like meteorology. For example, wind—the fluid motion of air in the atmosphere—can be represented by vectors indicating the speed and direction of the wind at any given point on a map. Another method for representing fluid motion is a streamline. A streamline represents the path of a small volume of fluid as it flows. When the flow pattern changes with time, the...
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Turbulent Flow01:24

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Turbulent flow is characterized by unpredictable fluctuations in velocity and pressure, which result in a chaotic fluid movement distinct from the orderly patterns of laminar flow. While laminar flow is governed by smooth, parallel layers with minimal mixing, turbulent flow exhibits highly irregular, three-dimensional patterns. This behavior arises due to instabilities in the fluid's velocity profile, and amplifies as the flow velocity increases. Minor disturbances, known as turbulent...
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Entropy02:39

Entropy

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Salt particles that have dissolved in water never spontaneously come back together in solution to reform solid particles. Moreover, a gas that has expanded in a vacuum remains dispersed and never spontaneously reassembles. The unidirectional nature of these phenomena is the result of a thermodynamic state function called entropy (S). Entropy is the measure of the extent to which the energy is dispersed throughout a system, or in other words, it is proportional to the degree of disorder of a...
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The Kinetic Model of Gases01:24

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The kinetic model of gases explains the properties of a perfect gas using three main assumptions: molecules move in ceaseless random motion, their size is negligible compared to the distances between them, and they do not interact except during perfectly elastic collisions. The total energy of a gas is the sum of the kinetic energies of all its constituent molecules. The pressure exerted by the gas arises from the continual bombardment of the container walls by billions of colliding molecules.
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Boundary Layer Characteristics01:18

Boundary Layer Characteristics

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When a fluid encounters a solid surface, a boundary layer forms due to the interaction between the fluid's motion and the stationary surface. This phenomenon is characterized by a thin region adjacent to the surface where viscous forces dominate, influencing the fluid's velocity profile. The development of the boundary layer begins at the leading edge of the surface and evolves as the fluid moves downstream.As the fluid flows over the surface, friction between the fluid and the wall slows down...
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Poiseuille's Law and Reynolds Number01:10

Poiseuille's Law and Reynolds Number

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Any fluid in a horizontal tube can flow due to pressure differences—fluid flows from high to low pressure. The flow rate (Q) is the ratio of pressure difference and resistance through a horizontal tube. The greater the pressure difference, the higher the flow rate. The flow resistance is expressed as:
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Related Experiment Video

Updated: Mar 30, 2026

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

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Entropic multirelaxation lattice Boltzmann models for turbulent flows.

Fabian Bösch1, Shyam S Chikatamarla1, Ilya V Karlin1

  • 1Department of Mechanical and Process Engineering, ETH Zurich, 8092 Zurich, Switzerland.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|November 14, 2015
PubMed
Summary

This study presents stable 3D lattice Boltzmann models for turbulent flows. The entropic stabilizer ensures accurate simulations, showing promise for engineering and scientific applications.

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Area of Science:

  • Computational physics
  • Fluid dynamics
  • Numerical methods

Background:

  • Lattice Boltzmann methods (LBM) are powerful for simulating fluid dynamics.
  • Recent advancements introduced a new class of LBM with an entropic stabilizer.
  • Assessing the performance and stability of these models in 3D is crucial.

Purpose of the Study:

  • To present and analyze three-dimensional realizations of a novel lattice Boltzmann model.
  • To investigate the role and effectiveness of the entropic stabilizer in these models.
  • To evaluate the model's performance for high-Reynolds-number and turbulent flows.

Main Methods:

  • Developed three-dimensional lattice Boltzmann models with an entropic stabilizer.
  • Performed simulations using both coarse- and fine-grid approaches.
  • Utilized the Kida vortex flow benchmark for validation.
  • Analyzed homogeneous isotropic decaying turbulence for statistical quantities.

Main Results:

  • Demonstrated outstanding numerical stability and performance, independent of moment representation for high-Reynolds-number flows.
  • Achieved accurate results for low-order moments and second-order grid convergence in turbulence simulations.
  • Confirmed convergence to the lattice Bhatnagar-Gross-Krook model with increased resolution.
  • Observed reduced compressibility effects and maintained correct energy/enstrophy dissipation due to the entropic stabilizer.

Conclusions:

  • The presented 3D lattice Boltzmann models offer excellent numerical stability and efficiency.
  • The entropic stabilizer is key to achieving accurate and robust simulations of turbulent flows.
  • These models are promising for advanced engineering and scientific applications involving highly turbulent regimes.