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

2.9K
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
2.9K
Maxwell's Equation Of Electromagnetism01:29

Maxwell's Equation Of Electromagnetism

4.1K
James Clerk Maxwell (1831–1879) was one of the major contributors to physics in the nineteenth century. Although he died young, he made major contributions to the development of the kinetic theory of gases, to the understanding of color vision, and to understanding the nature of Saturn's rings. He is probably best known for having combined existing knowledge on the laws of electricity and magnetism with his insights into a complete overarching electromagnetic theory, which is...
4.1K
Symmetry in Maxwell's Equations01:28

Symmetry in Maxwell's Equations

4.2K
Once the fields have been calculated using Maxwell's four equations, the Lorentz force equation gives the force that the fields exert on a charged particle moving with a certain velocity. The Lorentz force equation combines the force of the electric field and of the magnetic field on the moving charge. Maxwell's equations and the Lorentz force law together encompass all the laws of electricity and magnetism. The symmetry that Maxwell introduced into his mathematical framework may not be...
4.2K
Differential Form of Maxwell's Equations01:17

Differential Form of Maxwell's Equations

1.3K
James Clerk Maxwell (1831–1879) was one of the significant contributors to physics in the nineteenth century. He is probably best known for having combined existing knowledge of the laws of electricity and the laws of magnetism with his insights to form a complete overarching electromagnetic theory, represented by Maxwell's equations. The four basic laws of electricity and magnetism were discovered experimentally through the work of physicists such as Oersted, Coulomb, Gauss, and...
1.3K
Lattice Centering and Coordination Number02:33

Lattice Centering and Coordination Number

12.6K
The structure of a crystalline solid, whether a metal or not, is best described by considering its simplest repeating unit, which is referred to as its unit cell. The unit cell consists of lattice points that represent the locations of atoms or ions. The entire structure then consists of this unit cell repeating in three dimensions. The three different types of unit cells present in the cubic lattice are illustrated in Figure 1.
Types of Unit Cells
Imagine taking a large number of identical...
12.6K
Trends in Lattice Energy: Ion Size and Charge02:54

Trends in Lattice Energy: Ion Size and Charge

26.8K
An ionic compound is stable because of the electrostatic attraction between its positive and negative ions. The lattice energy of a compound is a measure of the strength of this attraction. The lattice energy (ΔHlattice) of an ionic compound is defined as the energy required to separate one mole of the solid into its component gaseous ions. For the ionic solid sodium chloride, the lattice energy is the enthalpy change of the process:
26.8K

You might also read

Related Articles

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

Sort by
Same author

Photon-Modulated Bond Covalency of [Sm(II)(η<sup>9</sup>-C<sub>9</sub>H<sub>9</sub>)<sub>2</sub>].

Journal of the American Chemical Society·2024
Same author

[Pager-supported waiting time management in a university hospital ENT outpatient department : A pilot project for more distance and more comfort].

HNO·2021
Same author

Patients with breakthrough tick-borne encephalitis suffer a more severe clinical course and display extensive magnetic resonance imaging changes.

European journal of neurology·2020
Same author

Adenosine stress CMR perfusion imaging of the temporal evolution of perfusion defects in a porcine model of progressive obstructive coronary artery occlusion.

NMR in biomedicine·2019
Same author

Comparison of the lattice-Boltzmann model with the finite-difference time-domain method for electrodynamics.

Physical review. E·2019
Same author

[Determination of hearing thresholds in children using auditory brainstem responses : Influence of sedation and anaesthesia on quality and measurement time].

HNO·2019

Related Experiment Video

Updated: Feb 15, 2026

Indirect Fabrication of Lattice Metals with Thin Sections Using Centrifugal Casting
08:32

Indirect Fabrication of Lattice Metals with Thin Sections Using Centrifugal Casting

Published on: May 14, 2016

13.0K

Stable lattice Boltzmann model for Maxwell equations in media.

A Hauser1, J L Verhey1

  • 1Department of Experimental Audiology, Otto von Guericke University Magdeburg, Leipziger Straße 44, 39120 Magdeburg, Germany.

Physical Review. E
|January 20, 2018
PubMed
Summary

This study presents a stable lattice Boltzmann (LB) method for simulating electromagnetic (EM) waves in complex media. The enhanced model improves stability and accuracy for sharp transitions, offering an easily implemented alternative for EM wave propagation simulations.

More Related Videos

Measuring the Spin-Lattice Relaxation Magnetic Field Dependence of Hyperpolarized [1-13C]pyruvate
11:57

Measuring the Spin-Lattice Relaxation Magnetic Field Dependence of Hyperpolarized [1-13C]pyruvate

Published on: September 13, 2019

7.0K
Trapping of Micro Particles in Nanoplasmonic Optical Lattice
07:20

Trapping of Micro Particles in Nanoplasmonic Optical Lattice

Published on: September 5, 2017

7.0K

Related Experiment Videos

Last Updated: Feb 15, 2026

Indirect Fabrication of Lattice Metals with Thin Sections Using Centrifugal Casting
08:32

Indirect Fabrication of Lattice Metals with Thin Sections Using Centrifugal Casting

Published on: May 14, 2016

13.0K
Measuring the Spin-Lattice Relaxation Magnetic Field Dependence of Hyperpolarized [1-13C]pyruvate
11:57

Measuring the Spin-Lattice Relaxation Magnetic Field Dependence of Hyperpolarized [1-13C]pyruvate

Published on: September 13, 2019

7.0K
Trapping of Micro Particles in Nanoplasmonic Optical Lattice
07:20

Trapping of Micro Particles in Nanoplasmonic Optical Lattice

Published on: September 5, 2017

7.0K

Area of Science:

  • Computational physics
  • Electromagnetism
  • Numerical methods

Background:

  • Existing lattice Boltzmann (LB) models for electromagnetic (EM) wave propagation in homogeneous media exhibit numerical instability at sharp transitions.
  • Previous models struggle to accurately simulate EM wave behavior in media with complex or rapidly changing properties.

Purpose of the Study:

  • To develop a stable and accurate numerical method for simulating electromagnetic waves in homogeneous and complex media using the lattice Boltzmann model.
  • To address the limitations of existing LB models concerning numerical instability in the presence of sharp media transitions.

Main Methods:

  • Utilized an extension of a known lattice Boltzmann model for EM waves in vacuum, separating polarization and magnetization effects.
  • Applied Strang splitting for simulations in conductive media, analyzing the skin effect.
  • Quantified error scaling, stability, accuracy, and time scaling through simulations of EM waves entering different media.

Main Results:

  • The extended LB method demonstrates stable simulations even with sharp media transitions.
  • Error analysis for EM wave propagation and static limits in conductive media showed accuracy less than 1%.
  • The method provides accurate simulations for the skin effect in conductive media.

Conclusions:

  • The presented lattice Boltzmann method offers a stable and easily implementable solution for simulating electromagnetic wave propagation in complex structured media.
  • This approach enhances the accuracy and stability of simulations, particularly for arbitrary transitions in material properties.
  • The method serves as a valuable alternative for researchers and engineers working with electromagnetic wave phenomena in diverse media.