Classifications

• • G—PHYSICS
  • G10—MUSICAL INSTRUMENTS; ACOUSTICS
  • G10K—SOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
  • G10K11/00—Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
  • G10K11/16—Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
  • G10K11/172—Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using resonance effects
• • G—PHYSICS
  • G10—MUSICAL INSTRUMENTS; ACOUSTICS
  • G10K—SOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
  • G10K11/00—Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
  • G10K11/16—Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
  • G10K11/162—Selection of materials
  • G10K11/168—Plural layers of different materials, e.g. sandwiches

Definitions

• the present invention relates to the field of acoustic resonators.
• the present invention relates to a resonator that can be used in an application of acoustic absorption type, for example as an absorbent or silent material, or in an application of the acoustic radiation type, for example of the type of loudspeaker (enclosure "Bass-reflex").
• acoustic absorption type for example as an absorbent or silent material
• the acoustic radiation type for example of the type of loudspeaker (enclosure "Bass-reflex").
• Commonly used materials for achieving acoustic absorption are polyurethane foams, fiberglass-like glass materials, or melamine foams.
• Such porous materials are among the most absorbent materials and are generally effective at absorbing high frequencies, typically above 1 kHz. However, these porous materials are generally not very effective in absorbing low frequencies, typically less than 1 kHz. More generally, a disadvantage of such porous materials is that the absorption efficiency is proportional to the thickness of the material. By way of example, the inventors believe that the same value of the absorption coefficient at a frequency of 500 Hz by a melamine foam would imply a thickness of this foam of several tens of centimeters at least.
• acoustic absorption devices of the type comprising a tunnel adapted to receive and propagate an acoustic wave, and having lateral cavities forming Helmholtz resonators.
• acoustic absorption devices of the type comprising a tunnel adapted to receive and propagate an acoustic wave, and having lateral cavities forming Helmholtz resonators.
• each of the lateral cavities opens onto the tunnel through a point-type orifice pierced in the wall of the tunnel.
• the lateral cavities extend peripherally and parallel to the tunnel (see Fig. 5b of this document).
• systems with Helmholtz resonators are capable of absorbing low frequencies, typically less than 1 kHz.
• the absorption of low frequencies assumes relatively large resonator dimensions.
• the inventors estimate that to obtain a resonance frequency of 500 Hz with a cavity forming a resonator, this cavity should have a length of the order of 17 cm.
• the document LECLAIRE 15 describes a material comprising several main perforations able to receive and propagate an acoustic wave, and having "dead-ends pores" ("dead-ends pores”) side perforations.
• An object of the invention is to provide a thin acoustic resonator capable of absorbing low frequencies, typically less than 1 kHz.
• Another object of the invention is to provide an acoustic resonator that can also operate in an application of acoustic radiation type.
• the invention proposes an acoustic resonator comprising a resonance piece provided with:
• a main perforation traversing the resonance part from one side to the other, the main perforation extending in a direction of propagation, this main perforation being able to receive and propagating at least one acoustic wave in the direction of propagation,
• each lateral cavity extending transversely with respect to the direction of propagation
• the main perforation and the lateral cavities being filled with a fluid, this fluid preferably being air (or alternatively, for example being able to be water),
• the lateral cavities constituting fluid slats so that the resonance piece has a "mille-feuille" structure comprising these fluid slats and layers of a material of the resonance piece separating these fluid slats.
• the resonance piece has a "multilayer” structure, or “multilayer” structure, formed by an alternation of fluid slats and layers of material.
• the resonance piece can be made from a single block of material or by assembly and gluing of several elements, for example machined separately.
• the mille-sheet structure of the resonator according to the invention is therefore characterized by a succession, from one side of the resonance part in the direction of spread, metal layers and air knives.
• the mille-feuille structure would successively comprise: a metal layer, an air space, a metal layer, an air space and a layer of metal.
• Such a resonator provided with such a mille-feuille structure maximizes the exchange surface between the material of the resonance piece and the fluid filling the main perforation and the lateral cavities.
• the thermal exchanges within the fluid slats and the convective exchanges between the main perforation and the lateral cavities cause a considerable increase in the compressibility of the fluid in the perforation. and, in particular, a considerable increase in the acoustic absorption of low frequencies.
• the resonance piece may be made of a metallic material.
• a metallic material facilitates the manufacture of the resonance piece.
• the resonance part may be made of any other material, for example in a plastic material.
• the lateral cavities may be evenly spaced along the direction of propagation. Regular spacing of the lateral cavities, i.e., periodic arrangement of the fluid slats, promotes heat exchange between the main perforation and the lateral cavities, resulting in increased fluid compressibility in the main perforation and makes it possible, in particular, to absorb relatively low frequencies.
• the lateral cavities preferably extend perpendicular to the direction of propagation.
• each layer of material separating the fluid blades may have a thickness equal to a lateral cavity thickness.
• This characteristic makes it possible to optimize the heat exchange effects of the mill-sheet structure for a reduced total dimension of the resonance part in the direction of propagation.
• each of the lateral cavities and / or each layer of material separating the fluid blades may have a thickness of less than 3 mm, preferably less than 2 mm, preferably less than or equal to 1 mm.
• each of the lateral cavities and / or each layer of material separating the fluid slats can thus have a thickness of a few hundred micrometers.
• each of the lateral cavities, or fluid slats may have a thickness defined by two transverse planes parallel to each other and not parallel to the direction of propagation.
• these transverse planes may be perpendicular to the direction of propagation, so that the lateral cavities extend perpendicular to the direction of propagation.
• each of the lateral cavities may form a defined volume: by two first lateral planes parallel to the direction of propagation and parallel to each other, these two first lateral planes defining a lateral cavity height,
• two second lateral planes parallel to each other and perpendicular to the first lateral planes, these two second lateral planes defining a lateral cavity width, the lateral cavity width being preferably equal to the lateral cavity height,
• the ratio of the height to the lateral cavity thickness, and / or the ratio of the width to the lateral cavity thickness may preferably be greater than 15, preferably greater than 20, preferably 25.
• each of the lateral cavities may form a non-parallelepipedal volume, for example a disk, a straight or curved hexagonal prism, etc.
• the ratio of the cross section of each of the lateral cavities to the section of the main perforation may be greater than 75, preferably greater than 125, preferably between 150 and 160.
• section means a shape defined by the intersection of a volume with a plane.
• cross section of a lateral cavity designates the shape defined by the intersection of this lateral cavity with a median plane of this lateral cavity intersecting the direction of propagation at the corresponding section of the main perforation.
• the cross section of a lateral cavity is the shape defined by the intersection of this lateral cavity with a plane perpendicular to the direction of propagation.
• the section of the main perforation is the shape defined by the intersection of a volume constituted by this perforation with a plane perpendicular to the direction of propagation, this plane passing through one of said layers of material.
• the height and / or the lateral cavity width may be greater than or equal to 25 mm, preferably greater than 30 mm, preferably equal to 50 mm.
• the main perforation may have a square section.
• the section of the main perforation can be round or any other shape.
• the main perforation may have, in one embodiment, a section smaller than 24 mm 2 , preferably less than 9 mm 2 , preferably equal to 4 mm 2 .
• Such geometry and / or dimensions of the lateral cavities and / or of the resonance part favor the thermal and convective effects within the resonator.
• relatively large airlocks of lateral dimensions D1 and D2 constitute relatively large heat exchange surfaces.
• the resonator according to the invention makes it possible to achieve acoustic absorption of low frequencies, typically less than 1 kHz, for a reduced total dimension of the resonance part, at least in the direction of propagation.
• the total thickness of the resonance part in the direction of propagation may in particular be less than 4 cm, which is a relatively small thickness compared to the sound absorption capabilities of the resonator.
• the resonator according to the invention also makes it possible to produce acoustic radiation for a reduced total dimension of the resonance part, at least in the direction of propagation.
• FIGURE 1 is a perspective view in section of a resonator according to the invention showing a series of five lateral cavities;
• FIGURE 2 is a front view of the resonator of FIGURE 1;
• FIGURE 3 is a side view in section of a resonator according to the invention showing a series of fifteen lateral cavities extending perpendicular to a direction of propagation;
• FIGURE 4 is a side view in section of a resonator according to the invention showing a series of four lateral cavities extending obliquely with respect to a direction of propagation;
• FIGURE 5 presents experimental results obtained by the inventors with resonators according to the invention.
• variants of the invention comprising only a selection of characteristics described, isolated from the other characteristics described (even if this selection is isolated within a sentence including these other characteristics), if this selection of features is sufficient to confer a technical advantage or to differentiate the invention from the state of the prior art.
• This selection comprises at least one characteristic, preferably functional without structural details, or with only a part of the structural details if this part alone is sufficient to confer a technical advantage or to differentiate the invention from the state of the prior art .
• FIGURES 1 and 2 show an acoustic resonator according to the invention.
• This resonator comprises a resonance part 1 consisting, in this example, of a block of parallelepiped shape.
• the resonance part 1 is preferably made of a metallic material or any other material.
• the resonance part 1 comprises a main perforation 2 passing through the resonance part 1 from one side to the other.
• the main perforation 2 extends in a direction of propagation 21.
• the orthogonal coordinate system of FIG. 1 represents the direction of propagation 21, a first lateral direction 311 and a second lateral direction 312, these three directions 21, 311 and 312 being perpendicular to one another.
• the main perforation 2 is able to receive and propagate at least one acoustic wave 9 in the direction of propagation 21.
• such an acoustic wave 9 can be received in the resonance room 1 by the opening formed by the main perforation 2 at a receiving surface 11 of the resonance part 1 exposed to a surrounding space in which the at least one acoustic wave 9 propagates.
• the at least one acoustic wave 9 can propagate in the resonant part 1 through the main perforation 2, typically so as to pass right through the resonance part 1.
• the at least one acoustic wave 9 can be generated by any system or means not subject of the present invention.
• the resonance part 1 is further provided with a series of lateral cavities 3 communicating with the main perforation 2 so as to form acoustic resonators.
• lateral cavities 3 typically make it possible to attenuate frequencies of the at least one acoustic wave 9 during its propagation in the main perforation 2.
• each lateral cavity 3a, 3b, 3c ... is made inside the resonance part 1.
• each lateral cavity 3a, 3b, 3c ... forms a volume inside the sound room 1.
• the main perforation 2 and the lateral cavities 3a, 3b, 3c ... are filled with a fluid.
• this fluid is air.
• This fluid also occupies said surrounding space in which the at least one acoustic wave 9 propagates.
• each lateral cavity 3a, 3b, 3c ... extends transversely with respect to the direction of propagation 21.
• the lateral cavities 3a, 3b, 3c ... extend perpendicular to the direction of propagation 21.
• the lateral cavities 3a, 3b, 3c and 3d extend obliquely with respect to the direction of propagation 21.
• the lateral cavities 3a, 3b, 3c ... can be machined directly in the resonance part 1, for example using 3D printing, structural bonding and assembly techniques.
• the resonance part 1 can be made from a single block of material or by assembly and gluing of several elements, for example machined separately.
• each lateral cavity 3a, 3b, 3c ... opens on the main perforation 2 by the entire periphery of a respective section of this main perforation 2.
• the drawings thus show, for example in FIGURE 2, that the main perforation 2 is geometrically contained in the series of lateral cavities 3 relative to the first 311 and the second 312 lateral direction.
• this section D3 representing the thickness of the lateral cavity 3a according to the direction of propagation 21, it results from geometric construction that the lateral cavity 3a opens on the main perforation 2 by the entire periphery of the section D3 of the main perforation 2.
• the lateral cavities 3 constitute fluid slats so that the resonance part 1 has a "mille-feuille" structure, or multilayer structure, comprising these fluid slats and layers. the material of the resonance part 1 separating these fluid slides.
• the multilayer or multilayer structure has an alternation, on the one hand, of blades of the fluid filling the main perforation 2 and the lateral cavities 3a, 3b, 3c ... and, on the other hand, of layers of the material forming the resonance part 1.
• the series of lateral cavities 3 comprises at least three lateral cavities.
• the embodiment illustrated in FIG. 3 represents a resonance part 1 provided with a series of fifteen lateral cavities 3a, 3b, ... 3o.
• the lateral cavities 3a, 3b, 3c ... can be arranged in a periodic manner, that is to say that they can be regularly spaced along the direction of propagation 21. Such a periodic arrangement favors thermal exchanges between the lateral cavities 3a, 3b, 3c ... and the main perforation 2, and results in an increase in the compressibility of the fluid in the main perforation 2.
• the thickness D3 of each lateral cavity is identical for all the lateral cavities.
• the thickness D4 of each layer of material separating the fluid slats is identical for all pairs of adjacent lateral cavities.
• each layer of material separating the fluid blades has a thickness D4 equal to the lateral cavity thickness D3.
• the lateral cavities 3a, 3b, 3c ... form a parallelepipedal volume.
• Such a volume can be geometrically defined as follows.
• Each of the lateral cavities 3a, 3b, 3c ..., or fluid slats has a thickness D3 defined by two transverse planes parallel to each other, and not parallel to the direction of propagation 21. In the embodiments of FIGURES 1 and 3, these two transverse planes are perpendicular to the direction of propagation 21.
• Each of the lateral cavities 3a, 3b, 3c forms a defined volume: - by two first lateral planes parallel to the direction of propagation 21 and parallel to each other, these two first lateral planes defining a height D1 of lateral cavity,
• FIGURE 1 is a sectional view of the resonance part 1 showing, only for the lateral cavity 3a, the half-width D21 of this lateral cavity 3a.
• the dimensional characteristics of the lateral cavities 3a, 3b, 3c ... and / or of the main perforation 2 can also contribute, in the case of an application of acoustic absorption type, to achieve absorption of low frequencies, typically less than 1 kHz, while producing a resonator of small thickness, in particular of small dimension of resonance part 2 according to the direction of propagation 21.
• the lateral cavity thickness D 3 is less than 3 mm, preferably less than 2 mm, preferably less than or equal to 1 mm;
• the thickness D4 of the layer of material separating the fluid slats is less than 3 mm, preferably less than 2 mm, preferably less than or equal to 1 mm; the ratio of the height D1 to the thickness D3, and / or the ratio of the width D2 to the thickness D3, is greater than 15, preferably greater than 20, preferably equal to 25;
• the ratio of the cross section of each of the lateral cavities, defined by the product of the height D1 and the lateral cavity width D2, on the section of the main perforation 2, defined by the product of the dimensions D5 and D6 represented in FIG. FIGURE 2 is greater than 75, preferably greater than 125, preferably between 150 and 160;
• the height D1 and / or the width D2 of the lateral cavity is greater than or equal to 25 mm, preferably greater than 30 mm, preferably equal to 50 mm.
• the main perforation 2 has a square section. This square section is defined by two sides D5 and D6. In an alternative embodiment, the main perforation 2 has a circular section.
• each lateral cavity 3a, 3b, 3c ... is cylindrical (not shown).
• the cross section of each of the lateral cavities is circular.
• the main perforation 2 may have a section less than 24 mm 2 , preferably less than 9 mm 2 , preferably equal to 4 mm 2 .
• the inventors have made eight acoustic resonators according to the invention to test their capacities in an application of acoustic absorption type.
• the main perforation 2 had a square section of 4 ⁇ 4 mm
• Impedance tube tests were performed to measure the sound absorption coefficient of these resonators.
• FIG. 5 shows the absorption coefficient curves obtained during these tests (one curve per resonator tested), VAL1 on the ordinate representing the absorption coefficient, VAL2 on the abscissa representing the frequency in Hz.
• the inventors have made an acoustic resonator according to the invention to test its capabilities in an application of acoustic absorption type and in an acoustic radiation type application.
• the main perforation 2 was of circular section and had a diameter of 6.5 mm.
• the resonance part 1 was provided with a series of fifteen lateral cavities of circular section having a diameter of 21.3 mm and a thickness D3 of 1 mm.
• the thickness D4 of each layer of material separating the lateral cavities was 1.2 mm.
• the total thickness of the resonant part 1 according to the direction of propagation was 35.3 mm.
• the sound absorption coefficient of the resonator placed in an acoustic tube and subjected to a plane wave acoustic excitation the sound absorption coefficient of the resonator placed in an acoustic tube and subjected to a plane wave acoustic excitation
• the acoustic radiation of the resonator placed in a box with absorbent materials and excited by an air jet.
• this resonator makes it possible to obtain resonance frequencies close to the frequency values of the absorption peaks, in particular a frequency on the main resonance close to 1000 Hz in radiation and absorption, for a total thickness of the resonance part 1 according to the direction of propagation of 35.3 mm.
• the researchers estimate that the absorption or radiation of such a frequency would involve respectively a cavity or a tube of 85.8 mm length.
• the resonance part 1 may be provided with secondary perforations parallel to the perforation
• the various features, shapes, variants and embodiments of the invention may be associated with each other in various combinations to the extent that they are not incompatible or exclusive of each other.

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• Physics & Mathematics (AREA)
• Engineering & Computer Science (AREA)
• Acoustics & Sound (AREA)
• Multimedia (AREA)
• Soundproofing, Sound Blocking, And Sound Damping (AREA)

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• 2016
  • 2016-02-05 FR FR1650926A patent/FR3047599B1/fr not_active Expired - Fee Related
• 2017
  • 2017-02-01 WO PCT/EP2017/052183 patent/WO2017134125A1/fr active Application Filing
  • 2017-02-01 US US16/075,093 patent/US20190035377A1/en not_active Abandoned
  • 2017-02-01 SG SG11201806610WA patent/SG11201806610WA/en unknown
  • 2017-02-01 EP EP17706165.2A patent/EP3411874A1/de not_active Withdrawn
  • 2017-02-01 CN CN201780010064.1A patent/CN108885863A/zh active Pending
  • 2017-02-01 JP JP2018541121A patent/JP2019505016A/ja active Pending

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