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

Equations of Wave Motion01:02

Equations of Wave Motion

Mathematically, the motion of a wave can be studied using a wavefunction. Consider a string oscillating up and down in simple harmonic motion, having a period T. The wave on the string is sinusoidal and is translated in the positive x-direction as time progresses. Sine is a function of the angle θ, oscillating between +A and −A and repeating every 2π radians. To construct a wave model, the ratio of the angle θ and the position x is considered.
Electromagnetic Wave Equation01:24

Electromagnetic Wave Equation

Maxwell's equations for electromagnetic fields are related to source charges, either static or moving. These fields act on a test charge, whose trajectory can thus be determined using suitable boundary conditions. The objective of electromagnetism is thus theoretically complete.
However, although electric and magnetic fields were first introduced as mathematical constructs to simplify the description of mutual forces between charges, a natural question emerges from Maxwell's equations: What...
Equation of the Elastic Curve01:23

Equation of the Elastic Curve

The concept of curvature in plane curves, crucial in structural engineering, defines how sharply a beam bends under load. This curvature is determined using the curve's first and second derivatives.
Consider a cantilever beam with a point load at its free end (for instance, a diving board). When analyzing beam deflection with small slopes, the shape of the beam's elastic curve becomes key. The governing equation for this analysis involves the bending moment and the beam's flexural rigidity,...
Partial Differential Equations01:21

Partial Differential Equations

A stone dropped into a still pond generates waves that propagate outward in circular patterns, creating a dynamic surface whose elevation depends on both position and time. At any given location, the water level oscillates as the wave passes, while at any fixed moment, the surface exhibits smooth, curved structures extending across space. This dual dependence requires a mathematical description that accounts for variation in multiple variables simultaneously.At a fixed point on the water...
Bessel Function of Order Zero01:20

Bessel Function of Order Zero

A common physical example of wave propagation with radial symmetry is the ripple formed when a stone is dropped into a still pond. The disturbance originates at a central point and travels outward as a circular wave. As the radius of the wavefront increases, the same initial energy is distributed along a progressively larger circumference. Consequently, the amplitude, or height, of the wave decreases with distance from the center. This decay behavior cannot be captured by simple sine or cosine...
Poisson's And Laplace's Equation01:25

Poisson's And Laplace's Equation

The electric potential of the system can be calculated by relating it to the electric charge densities that give rise to the electric potential. The differential form of Gauss's law expresses the electric field's divergence in terms of the electric charge density.

You might also read

Related Articles

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

Sort by
Same author

Concurrent control of natural and robotic limbs through a tactile-encoded brain-computer interface.

Nature communications·2026
Same author

Jasmonate, salicylate, and ethylene-responsive transcriptomics discovery in spikelets of three wheat genotypes reveals a rapid and conserved response for jasmonate signaling.

Plant signaling & behavior·2026
Same author

Assessing different Protein A resins' homodimer separation potentials through processing a two-antibody-containing artificial mixture.

Protein expression and purification·2026
Same author

Reply to "Letter to the editor: methodological considerations in the benchmarking of AI-based protein-aptamer complex prediction".

Briefings in bioinformatics·2026
Same author

EEG Ensemble Learning Framework for Prognostic Prediction of Post-rTMS Motor Recovery in Stroke.

IEEE transactions on bio-medical engineering·2026
Same author

Long-term outcomes for neoadjuvant versus adjuvant chemotherapy in operable breast cancer patients with hormone receptor-positive, HER2-negative.

Frontiers in oncology·2026
Same journal

High-resolution depth estimation for multiple wideband sources in deep sea via sparse Bayesian learninga).

The Journal of the Acoustical Society of America·2026
Same journal

Depression markers in speech: An approach based on tract variables dynamics.

The Journal of the Acoustical Society of America·2026
Same journal

The oyster toadfish (Opsanus tau) alters active and diurnal calling amid vessel noise in New York City.

The Journal of the Acoustical Society of America·2026
Same journal

Experimental noise characterisation of phase-locked tandem-rotor in edgewise flight.

The Journal of the Acoustical Society of America·2026
Same journal

The tune-text-temporal synergy: Prosodic effects of final segmental weakening in Neapolitan.

The Journal of the Acoustical Society of America·2026
Same journal

Monitoring vessel movement above critical offshore infrastructure using distributed acoustic sensing.

The Journal of the Acoustical Society of America·2026
See all related articles

Related Experiment Video

Updated: Jun 14, 2026

Lens-free Video Microscopy for the Dynamic and Quantitative Analysis of Adherent Cell Culture
09:04

Lens-free Video Microscopy for the Dynamic and Quantitative Analysis of Adherent Cell Culture

Published on: February 23, 2018

Convolutional perfectly matched layer for elastic second-order wave equation.

YiFeng Li1, Olivier Bou Matar

  • 1Joint European Laboratory LEMAC, Institut d'Electronique, de Microelectronique et de Nanotechnologie, IEMN-DOAE-UMR CNRS 8520, Ecole Centrale de Lille, 59651 Villeneuve d'Ascq, France.

The Journal of the Acoustical Society of America
|March 25, 2010
PubMed
Summary
This summary is machine-generated.

This study introduces a novel convolutional perfectly matched layer (C-PML) method to improve simulations of acoustic wave propagation in elastic media. The C-PML effectively absorbs surface waves, outperforming traditional perfectly matched layers (PML) in complex scenarios.

Related Experiment Videos

Last Updated: Jun 14, 2026

Lens-free Video Microscopy for the Dynamic and Quantitative Analysis of Adherent Cell Culture
09:04

Lens-free Video Microscopy for the Dynamic and Quantitative Analysis of Adherent Cell Culture

Published on: February 23, 2018

Area of Science:

  • Computational physics
  • Wave propagation modeling
  • Numerical methods

Background:

  • Simulating wave propagation in unbounded elastic media requires effective absorbing boundary conditions (ABC).
  • Traditional perfectly matched layers (PML) can exhibit spurious reflections, particularly for surface waves at oblique incidence.
  • Existing methods struggle with numerical instabilities in anisotropic media.

Purpose of the Study:

  • To extend the convolutional perfectly matched layer (C-PML) for simulating acoustic wave propagation in elastic media.
  • To enhance the attenuation of outgoing surface waves compared to classical PML.
  • To address and stabilize absorbing layers in anisotropic solids.

Main Methods:

  • Developed a C-PML method for second-order acoustic wave equations.
  • Implemented C-PML within finite element method (frequency domain) and pseudo-spectral (time domain) algorithms.
  • Investigated C-PML performance for oblique incidence and anisotropic media.

Main Results:

  • The C-PML ABC demonstrates superior attenuation of outgoing surface waves compared to classical PML.
  • The proposed method is more effective than classical PML at oblique incidence, reducing spurious reflections.
  • A modified C-PML formulation enhances stability in anisotropic solids.

Conclusions:

  • The C-PML is a more effective ABC for simulating acoustic wave propagation in elastic media.
  • This method offers improved accuracy and stability, especially for surface waves and anisotropic materials.
  • The C-PML provides a robust solution for truncating unbounded domains in wave propagation simulations.