Métamatériaux acoustiquesLes métamatériaux acoustiques sont des matériaux artificiels développés pour contrôler et manipuler les ondes acoustiques pouvant se propager dans des gaz, des liquides ou des solides. Initialement, ce domaine d'étude provient de la recherche de matériaux à indice de réfraction négatifs. Le contrôle des différentes formes d'ondes acoustiques ainsi générées est principalement réalisé grâce au contrôle du module d'élasticité β, de la densité ρ, ou de la .
Negative-index metamaterialNegative-index metamaterial or negative-index material (NIM) is a metamaterial whose refractive index for an electromagnetic wave has a negative value over some frequency range. NIMs are constructed of periodic basic parts called unit cells, which are usually significantly smaller than the wavelength of the externally applied electromagnetic radiation. The unit cells of the first experimentally investigated NIMs were constructed from circuit board material, or in other words, wires and dielectrics.
MétamatériauEn physique, en électromagnétisme, le terme métamatériau désigne un matériau composite artificiel qui présente des propriétés électromagnétiques qu'on ne retrouve pas dans un matériau naturel. Il s'agit en général de structures périodiques, diélectriques ou métalliques, qui se comportent comme un matériau homogène n'existant pas à l'état naturel. Il existe plusieurs types de métamatériaux en électromagnétisme, les plus connus étant ceux susceptibles de présenter à la fois une permittivité et une perméabilité négatives.
Tunable metamaterialA tunable metamaterial is a metamaterial with a variable response to an incident electromagnetic wave. This includes remotely controlling how an incident electromagnetic wave (EM wave) interacts with a metamaterial. This translates into the capability to determine whether the EM wave is transmitted, reflected, or absorbed. In general, the lattice structure of the tunable metamaterial is adjustable in real time, making it possible to reconfigure a metamaterial device during operation.
Metamaterial antennaMetamaterial antennas are a class of antennas which use metamaterials to increase performance of miniaturized (electrically small) antenna systems. Their purpose, as with any electromagnetic antenna, is to launch energy into free space. However, this class of antenna incorporates metamaterials, which are materials engineered with novel, often microscopic, structures to produce unusual physical properties. Antenna designs incorporating metamaterials can step-up the antenna's radiated power.
Metamaterial absorberA metamaterial absorber is a type of metamaterial intended to efficiently absorb electromagnetic radiation such as light. Furthermore, metamaterials are an advance in materials science. Hence, those metamaterials that are designed to be absorbers offer benefits over conventional absorbers such as further miniaturization, wider adaptability, and increased effectiveness. Intended applications for the metamaterial absorber include emitters, photodetectors, sensors, spatial light modulators, infrared camouflage, wireless communication, and use in solar photovoltaics and thermophotovoltaics.
Metamaterial cloakingMetamaterial cloaking is the usage of metamaterials in an invisibility cloak. This is accomplished by manipulating the paths traversed by light through a novel optical material. Metamaterials direct and control the propagation and transmission of specified parts of the light spectrum and demonstrate the potential to render an object seemingly invisible. Metamaterial cloaking, based on transformation optics, describes the process of shielding something from view by controlling electromagnetic radiation.
Nonlinear metamaterialA nonlinear metamaterial is an artificially constructed material that can exhibit properties not yet found in nature. Its response to electromagnetic radiation can be characterized by its permittivity and material permeability. The product of the permittivity and permeability results in the refractive index. Unlike natural materials, nonlinear metamaterials can produce a negative refractive index. These can also produce a more pronounced nonlinear response than naturally occurring materials.
Terahertz metamaterialA terahertz metamaterial is a class of composite metamaterials designed to interact at terahertz (THz) frequencies. The terahertz frequency range used in materials research is usually defined as 0.1 to 10 THz. This bandwidth is also known as the terahertz gap because it is noticeably underutilized. This is because terahertz waves are electromagnetic waves with frequencies higher than microwaves but lower than infrared radiation and visible light.
History of metamaterialsThe history of metamaterials begins with artificial dielectrics in microwave engineering as it developed just after World War II. Yet, there are seminal explorations of artificial materials for manipulating electromagnetic waves at the end of the 19th century. Hence, the history of metamaterials is essentially a history of developing certain types of manufactured materials, which interact at radio frequency, microwave, and later optical frequencies.
Plasmonic metamaterialA plasmonic metamaterial is a metamaterial that uses surface plasmons to achieve optical properties not seen in nature. Plasmons are produced from the interaction of light with metal-dielectric materials. Under specific conditions, the incident light couples with the surface plasmons to create self-sustaining, propagating electromagnetic waves known as surface plasmon polaritons (SPPs). Once launched, the SPPs ripple along the metal-dielectric interface. Compared with the incident light, the SPPs can be much shorter in wavelength.
Haut-parleurvignette|Un haut-parleur électrodynamique. vignette|Schéma de coupe d'un haut-parleur électrodynamique. Un haut-parleur, ou hautparleur, est un transducteur électroacoustique destiné à produire des sons à partir d'un signal électrique. Il est en cela l'inverse du microphone. Par extension, on emploie parfois ce terme pour désigner un appareil complet destiné à la reproduction sonore (voir Enceinte). Quatre types de haut-parleurs, électrodynamique, électrostatique, piézoélectrique et isodynamique, représentent les technologies actuelles les plus courantes.
Transformation opticsTransformation optics is a branch of optics which applies metamaterials to produce spatial variations, derived from coordinate transformations, which can direct chosen bandwidths of electromagnetic radiation. This can allow for the construction of new composite artificial devices, which probably could not exist without metamaterials and coordinate transformation. Computing power that became available in the late 1990s enables prescribed quantitative values for the permittivity and permeability, the constitutive parameters, which produce localized spatial variations.
Crossover (audio)Le crossover est un filtre utilisé en sonorisation pour séparer des plages de fréquences d'un signal audio. Cet effet entre dans une catégorie de filtres électroniques conçus spécifiquement pour des utilisations dans des applications audio. Un crossover est un filtre séparant deux bandes de fréquences, soit pour des hautparleurs, soit pour des traitements différenciés du signal audio. L'utilisation principale est pour séparer les sons les plus graves d'un signal (généralement inférieurs à 120 Hz) afin de les diriger spécialement vers un subwoofer (ampli+sub).
Diaphragm (acoustics)In the field of acoustics, a diaphragm is a transducer intended to inter-convert mechanical vibrations to sounds, or vice versa. It is commonly constructed of a thin membrane or sheet of various materials, suspended at its edges. The varying air pressure of sound waves imparts mechanical vibrations to the diaphragm which can then be converted to some other type of signal; examples of this type of diaphragm are found in microphones and the human eardrum. Conversely a diaphragm vibrated by a source of energy beats against the air, creating sound waves.
Circuit RLCEn électrocinétique, un circuit RLC est un circuit linéaire contenant une résistance électrique, une bobine (inductance) et un condensateur (capacité). Il existe deux types de circuits RLC, série ou parallèle selon l'interconnexion des trois types de composants. Le comportement d'un circuit RLC est généralement décrit par une équation différentielle du second ordre (là où des circuits RL ou circuits RC se comportent comme des circuits du premier ordre).
Analogie de MaxwellL'analogie d'impédance ou analogie de Maxwell est une méthode de représentation d'un système mécanique par un système électrique analogue. L'avantage de celle-ci est qu'il existe un grand nombre de théories et de techniques d'analyse concernant les systèmes électriques complexes, en particulier dans le domaine des filtres. En convertissant vers une représentation électrique, ces outils du domaine électrique peuvent être directement appliqués à un système mécanique sans modification.
Electrodynamic speaker driverAn electrodynamic speaker driver, often called simply a speaker driver when the type is implicit, is an individual transducer that converts an electrical audio signal to sound waves. While the term is sometimes used interchangeably with the term speaker (loudspeaker), it is usually applied to specialized transducers which reproduce only a portion of the audible frequency range. For high fidelity reproduction of sound, multiple loudspeakers are often mounted in the same enclosure, each reproducing a different part of the audible frequency range.
Coaxial loudspeakerA coaxial loudspeaker is a loudspeaker system in which the individual driver units radiate sound from the same point or axis. Two general types exist: one is a compact design using two or three speaker drivers, usually in car audio, and the other is a two-way high-power design for professional audio, also known as single-source or dual-concentric loudspeakers. The design is favored for its compactness and behavior as an audio point source. Coaxial loudspeakers in professional audio enable sound from two drivers to come from one source.
Electrical resonanceElectrical resonance occurs in an electric circuit at a particular resonant frequency when the impedances or admittances of circuit elements cancel each other. In some circuits, this happens when the impedance between the input and output of the circuit is almost zero and the transfer function is close to one. Resonant circuits exhibit ringing and can generate higher voltages or currents than are fed into them. They are widely used in wireless (radio) transmission for both transmission and reception.
