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

Stability01:28

Stability

The time response of a linear time-invariant (LTI) system can be divided into transient and steady-state responses. The transient response represents the system's initial reaction to a change in input and diminishes to zero over time. In contrast, the steady-state response is the behavior that persists after the transient effects have faded.
The stability of an LTI system is determined by the roots of its characteristic equation, known as poles. A system is stable if it produces a bounded...
Lattice Energies of Ionic Crystals01:27

Lattice Energies of Ionic Crystals

Lattice energy represents the energy released when gaseous cations and anions combine to form an ionic solid, reflecting the strength of electrostatic interactions within the crystal. This process is fundamentally governed by Coulombic attraction between oppositely charged ions, where the potential energy varies inversely with the interionic distance and directly with the product of ionic charges. As ions approach one another, the electrostatic energy becomes increasingly negative, indicating a...
Multimachine Stability01:25

Multimachine Stability

Multimachine stability analysis is crucial for understanding the dynamics and stability of power systems with multiple synchronous machines. The objective is to solve the swing equations for a network of M machines connected to an N-bus power system.
In analyzing the system, the nodal equations represent the relationship between bus voltages, machine voltages, and machine currents. The nodal equation is given by:
Bewley Lattice Diagram01:12

Bewley Lattice Diagram

The Bewley lattice diagram, developed by L. V. Bewley, effectively organizes the reflections occurring during transmission-line transients. It visually represents how voltage waves propagate and reflect within a transmission line, making it easier to understand the complex interactions that occur.
The Kinetic Model of Gases01:24

The Kinetic Model of Gases

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.
Linear Approximation in Time Domain01:21

Linear Approximation in Time Domain

Nonlinear systems often require sophisticated approaches for accurate modeling and analysis, with state-space representation being particularly effective. This method is especially useful for systems where variables and parameters vary with time or operating conditions, such as in a simple pendulum or a translational mechanical system with nonlinear springs.
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length, the...

You might also read

Related Articles

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

Sort by
Same author

Consistent lattice Boltzmann equations for phase transitions.

Physical review. E, Statistical, nonlinear, and soft matter physicsยท2014
Same author

Lattice-Boltzmann model based on field mediators for immiscible fluids.

Physical review. E, Statistical, nonlinear, and soft matter physicsยท2003
Same author

Lattice-gas model based on field mediators for immiscible fluids.

Physical review. E, Statistical, nonlinear, and soft matter physicsยท2002
See all related articles

Related Experiment Video

Updated: Jul 6, 2026

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

Lattice Boltzmann equation linear stability analysis: thermal and athermal models.

D N Siebert1, L A Hegele, P C Philippi

  • 1LMPT Mechanical Engineering Department, Federal University of Santa Catarina, 88040-900 Florianopolis, SC, Brazil. diogo@lmpt.ufsc.br

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|March 21, 2008
PubMed
Summary

This study analyzes lattice Boltzmann models for nonisothermal compressible flows. Higher-order approximations improve stability, offering better solutions for complex fluid dynamics simulations.

More Related Videos

Optimization of An Air-Based Heat Management System for Dusty Particulate Matter-Covered Lithium-Ion Battery Packs
10:36

Optimization of An Air-Based Heat Management System for Dusty Particulate Matter-Covered Lithium-Ion Battery Packs

Published on: November 3, 2023

Related Experiment Videos

Last Updated: Jul 6, 2026

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

Optimization of An Air-Based Heat Management System for Dusty Particulate Matter-Covered Lithium-Ion Battery Packs
10:36

Optimization of An Air-Based Heat Management System for Dusty Particulate Matter-Covered Lithium-Ion Battery Packs

Published on: November 3, 2023

Area of Science:

  • Computational Fluid Dynamics
  • Thermodynamics
  • Numerical Analysis

Background:

  • Lattice Boltzmann models (LBM) struggle with nonisothermal compressible flows due to deviations from macroscopic equations and numerical instabilities.
  • Existing thermal LBMs require further development for accurate and stable simulations of such flows.

Purpose of the Study:

  • Investigate sources of instability in recently derived LBMs for nonisothermal compressible flows.
  • Determine stability limits for macroscopic variables in these LBMs.
  • Enhance the stability and accuracy of LBM for complex thermal fluid simulations.

Main Methods:

  • Linear stability analysis of LBMs derived from the continuous Boltzmann equation.
  • Evaluation of two-dimensional (2D) lattices with varying velocities (9, 17, 25, 37).
  • Incorporation of third-order terms into an athermal 2D nine-velocity model to improve accuracy.

Main Results:

  • Increasing the order of approximation in LBMs enhances numerical stability.
  • Specific stability limits for macroscopic variables were identified for different lattice configurations.
  • The modified athermal 2D nine-velocity model shows improved accuracy over the standard D2Q9 model.

Conclusions:

  • Higher-order lattice Boltzmann approximations are crucial for stable nonisothermal compressible flow simulations.
  • The identified stability limits provide practical guidelines for model selection and parameterization.
  • Further development of LBMs, including the incorporation of higher-order terms, is essential for advancing computational fluid dynamics in thermal applications.