Related Experiment Video
Updated: Dec 30, 2025

09:39
Characterizing Dissipative Elastic Metamaterials Produced by Additive Manufacturing
Published on: June 28, 2024
1.4K
Digitally virtualized atoms for acoustic metamaterials
Choonlae Cho1,2, Xinhua Wen1, Namkyoo Park2
1Department of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Hong Kong, China.
Nature Communications
|January 16, 2020
Summary
Virtualized metamaterials use digital signal processing to control acoustic properties, overcoming physical limitations. This software-defined approach enables on-demand tuning of bulk modulus and mass density for advanced material applications.
Area of Science:
- Acoustic metamaterials
- Solid-state physics
- Materials science
Background:
- Metamaterials offer unique properties by structuring atoms, enabling parameters beyond natural material limits.
- Tuning metamaterial properties typically requires physical modification or external circuits, limiting real-time applications.
Purpose of the Study:
- To introduce virtualized metamaterials that decouple constitutive parameters from physical structure.
- To demonstrate software-controlled tunability of acoustic metamaterial properties.
Main Methods:
- Replacing physical resonant structures with mathematical convolution kernels and digital signal processing circuits.
- Implementing software-defined frequency dispersion for dynamic control of material parameters.
Main Results:
- Achieved decoupled, on-demand control of effective bulk modulus and mass density in acoustic metamaterials.
- Demonstrated software-reconfigurable amplitude, center frequency, and bandwidth of frequency dispersion.
Conclusions:
- Virtualized metamaterials offer a new paradigm for designing advanced acoustic systems.
- This approach enables time-varying, non-reciprocal, non-Hermitian, and topological acoustic systems.
Related Concept Videos
The de Broglie Wavelength
32.7K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
32.7K
Standing Waves in a Cavity
1.4K
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
1.4K
Sound Waves: Interference
4.4K
Sound waves can be modeled either as longitudinal waves, wherein the molecules of the medium oscillate around an equilibrium position, or as pressure waves. When two identical waves from the same source superimpose on each other, the combination of two crests or two troughs results in amplitude reinforcement known as constructive interference. If two identical waves, that are initially in phase, become out of phase because of different path lengths, the combination of crests with troughs...
4.4K
Sound as Pressure Waves
4.3K
Sound waves, which are longitudinal waves, can be modeled as the displacement amplitude varying as a function of the spatial and temporal coordinates. As a column of the medium is displaced, its successive columns are also displaced. As the successive displacements differ relatively, a pressure difference with the surrounding pressure is created. The gauge pressure varies across the medium.
The pressure fluctuation depends on the difference in displacements between the successive points in the...
The pressure fluctuation depends on the difference in displacements between the successive points in the...
4.3K
Electromagnetic Waves in Matter
3.8K
Electromagnetic waves can travel in the vacuum as well as in matter. For example light, which is an electromagnetic wave, can travel through air, water, or glass.
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the medium, μ.
Furthermore,...
Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the medium, μ.
Furthermore,...
3.8K

