• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention relates to an elementary cell (1) of acoustic metamaterial comprising: - a solid material body (2), - at least one Fabry-Perot type cavity (3) in said body (2), and - at least a lateral resonant cavity (4) communicating with said Fabry-Pérot type cavity (2). The invention also relates to an acoustic screen comprising such an elementary cell.
    公开号:FR3044813A1
    申请号:FR1561750
    申请日:2015-12-02
    公开日:2017-06-09
    发明作者:Abdelkrim Khelif；Mahmoud Addouche；Ayouch Aliyasin El
    申请人:Centre National de la Recherche Scientifique CNRS；Universite de Franche-Comte；
    IPC主号:
    专利说明:

    The invention relates to the field of acoustic insulators. In particular, the invention relates to an elementary cell of an acoustic metamaterial, and an acoustic screen comprising such a cell.
    Noise pollution in everyday life, for example from the outside environment, such as the proximity of a road or air, or inside as the noise of home appliances, are stressors that deteriorate the comfort of life.
    Noise pollution also exists in the building industry and in various industrial areas.
    In order to regain comfort, it is often necessary to acoustically isolate the source of noise. To do this, solutions to attenuate the propagation of sound waves exist. However, the acoustic insulants known from the state of the art rely on the use of intrinsic characteristics of materials in terms of absorption or reflection of sound waves. The materials conventionally used for this purpose are typically porous materials, such as metal foams or polymeric materials, rockwool, glass, cotton, cork or agglomerated wood fibers.
    A problem with the use of such materials is that the choice of the material to be used is dictated by the intrinsic characteristics of the material, which limits the possibility of choice of material with respect to a given application. In addition, reliance on the intrinsic properties of the material also limits the response frequency range of the material as well as manufacturing techniques.
    In addition, acoustic panels made from such materials are heavy and bulky, especially those used for low frequencies. The objective of the present invention is to solve the problems of acoustic insulation known from the state of the art. In particular, the invention aims to provide an acoustic insulation solution, effective and to have flexibility in the choice of material and the frequency range. The invention also aims to reduce the size and weight of acoustic panels. To this end, the subject of the invention is an elementary cell of acoustic metamaterial comprising: a body made of solid material, at least one cavity of Fabry-Perot type in said body, and at least one lateral resonant cavity communicating with said cavity type Fabry-Perot.
    By Fabry-Perot cavity means a cavity having two open ends. Such a cavity allows a high confinement of the acoustic energy. This cavity being coupled to one or more resonant cavity (s) side (s), a series of antiresonances / resonances replace the classical resonances of simple Fabry-Perot type cavities, inducing an increased effect of reflection of sound waves . Such an effect is obtained independently of the nature of the solid material, which thus makes it possible to dispense with the nature of the material.
    In other words, even using a solid material whose intrinsic reflection properties are not important, the fact of structuring it so as to have a metamaterial comprising a Fabry-Perot type cavity coupled to one or more cavities (s). ) resonant (s) lateral (s) significantly improves the reflection of sound waves by this material.
    In order to have an important reflection, it is preferable that the dimensions of the opening of the Fabry-Perot type cavity, for example the diameter of a cylindrical cavity, are less than the wavelength or the range of lengths. waves that we want to think.
    The lateral resonant cavity may have any shape, the only condition for having sound wave reflection and that the lateral resonant cavity communicates with the Fabry-Perot cavity.
    Advantageously, the lateral resonant cavity is an acoustic resonator, Helmholtz type or quarter-wave type.
    Advantageously, the Fabry-Perot type cavity is a conduit passing through said body of solid material, which is preferably cylindrical. The advantage of having a through conduit lies in the fact that it allows the circulation of air and promotes heat exchange between the two media that the elementary cell separates.
    Preferably the cylindrical duct has a circular section with a diameter smaller than the wavelengths to be reflected. This makes it possible to have a high energy confinement.
    Advantageously, the cell body is parallelepipedal or cylindrical. Such a shape is advantageous because it makes it easy to include the cell in a matrix, for example in a matrix of an absorbent panel or a panel comprising other acoustic elements.
    Advantageously, the through duct is coaxial with the cylindrical cell.
    Advantageously, the Helmholtz resonator is a concentric cylindrical cavity with the conduit passing through and communicating with said conduit through a neck. This configuration favors the interaction between the Fabry-Perot type cavity and the lateral cavity to perform the reflector function. The reflection is particularly favored by the presence of the neck connecting the two cavities.
    Advantageously, the body made of solid material comprises two or more Helmholtz resonators having different dimensions. The fact of having several Helmholtz resonators with different dimensions makes it possible to increase the frequency band in which the cell is reflecting, through couplings occurring at different frequencies. Indeed, as the resonators have different dimensions, each has a different resonant frequency. As a result, the coupling of such Helmholtz resonators makes it possible to widen the frequency band in which the cell is reflective.
    According to one embodiment of the invention, the Fabry-Pérot cavity and / or the lateral resonant cavity is (are) folded so as to have at least one inlet, at least one outlet and at least two folds.
    These folds are made by a technique called space folding technique, which reduces the thickness of the cell. Thus, thanks to this folding it is possible to manufacture acoustic cells according to the invention, of small thickness. The invention also relates to an acoustic screen in the form of a panel, comprising at least one elementary cell according to the invention. Such a screen may comprise only reflective elementary cells according to the invention, but it may also comprise other acoustic elements, for example absorbent acoustic cells.
    Advantageously, said acoustic screen comprises a multitude of elementary cells, said cells being arranged in a plane of the panel so that each cell is able to act on another neighboring cell to widen the reflection frequency band.
    In this configuration, increasing the number of cells per unit area, increases the reflection of sound waves.
    By plane of the panel is meant in the sense of the present application the surface of the panel which can be flat or curved.
    Advantageously, said elementary cells are arranged in said plane of the panel periodically, for example according to a particular network of triangular type, square, hexagonal, or honeycomb-shaped. The invention will be better understood on reading the following description of preferred embodiments given by way of illustrative, non-limiting examples, with reference to the drawings in which:
    FIGS. 1a to 1c show a first exemplary embodiment of an elementary cell according to the invention, comprising a Fabry-Perot type cavity and a lateral cavity;
    Figures 2a and 2b show sectional views of two other examples in which the cell comprises a single lateral cavity;
    FIG. 3 represents an exemplary embodiment in which the elementary cell comprises, in addition to the Fabry-Perot type cavity, three lateral cavities;
    Figures 4a to 4c show a first embodiment in which the lateral cavity is folded; FIGS. 5a to 5d show a second exemplary embodiment in which the Fabry-Perot type cavity is folded; FIG. 6 shows the transmission response of an elementary cell according to the invention.
    Figure la represents an isometric view of an elementary cell 1 of acoustic metamaterial according to the invention. FIGS. 1b and 1c respectively represent a view from above and a view of a section along the axis AA of the elementary cell 1.
    The cell 1 comprises a cylindrical solid body 2 comprising a cylindrical duct 3 coaxial and through, forming a Fabry-Perot type cavity. The figure shows that the body 2 also has in its interior a lateral cavity 4 cylindrical and coaxial with the conduit 3 to which it is connected through a neck 5, so as to form a Helmoltz type cavity. As can be seen in FIG. 1c, the neck 5 is located halfway up the cylindrical cavity 4.
    By mid-height means a distance in the middle between the two ends of the duct forming the Fabry-Perot cavity.
    Such structuring of the metamaterial cell 1, in particular thanks to the presence of the neck 5 which connects the two cavities, favors the interaction between the Fabry-Perot type cavity and the lateral cavity to achieve a reflector function.
    The neck 5 may however be replaced by an opening of another type between the through cavity 3 and the lateral cavity 4.
    FIGS. 2a and 2b show sections similar to the section shown in FIG. 1c, of two other exemplary embodiments of elementary cells 1 'and 1 "that differ from the embodiment shown in FIGS. the lateral cavity.
    In the example of FIG. 2a, the lateral cavity 4 'is substantially similar to the cavity 4 of FIG. 1a, nevertheless the neck 5' is not arranged in the solid material body 2 'at the mid-height of the duct. 3 'as in the cell 1 of Figure 1c, but instead shifted to one end of the duct 3'. This offset has the effect of controlling the coupling to optimize reflection.
    In the exemplary embodiment illustrated in FIG. 2b, the lateral cavity 4 "has a width (that is to say the distance between the inner wall I and the outer wall E of the body 2" made of solid material) is much larger. that the width of the cavity 4 of Figure 1a. The neck 5 ", connecting the lateral cavity 4" to the through conduit 3 ", is arranged at mid-height of the conduit 3".
    By modifying the dimensions of the lateral cavity, its resonance frequency and its quality factor are modified. In this way one can adjust the reflection frequency.
    The embodiment of FIG. 3 differs from the examples of FIGS. 2a and 2b in that the cell body 20 comprises three concentric lateral cavities 41, 42, 43 of the through conduit 30 to which they are connected. The cavities 41 and 42 are cylindrical and each is connected to the through duct 30 by a neck 51, 52.
    The three cavities 41, 42, 43 as they have different shapes and / or dimensions, their resonance frequencies are also different. As a result, the reflection frequency band of the elementary cell 10 is larger than that of the elementary cell 1, which comprises a single lateral cavity 4 as shown in FIG.
    Figures 4a, 4b and 4c respectively show an isometric view, a top view and a view of a section along the axis BB, of an elementary cell 100 according to another embodiment.
    FIG. 4c shows that the body 200 of the elementary cell 100 comprises a folded lateral cavity 400 so as to have several folds, connected to a cylindrical through conduit 300 via the neck 500.
    The folding of the lateral cavity 400 makes it possible to considerably reduce the thickness of the cell 100 while retaining the efficiency of reflection.
    FIG. 5a represents an isometric view of a parallelepipedal elementary cell 100 'comprising a parallelepiped solid cell body 200' and a duct 300 'forming a Fabry-Perot cavity. Figures 5b to 5d respectively show a top view, a view of a section along the axis CC and a view of a section along the axis DD, of the cell 100 '.
    Figure 5c shows that the duct 300 'is folded and communicates via a neck 500' with a cylindrical cavity 400 'coaxial with a segment of said duct 300' as shown in Figure 5d.
    The parallelepipedal shape of the elementary cell 100 'has the advantage of allowing a better filling of the surface of an acoustic panel.
    According to one variant, the Fabry-Pérot type cavity and the lateral cavity are folded. The invention also relates to an acoustic screen comprising one or more elementary cells in accordance with the invention and as described above.
    FIG. 6 illustrates the transmission response of an elementary cell according to the embodiment shown in FIGS. Said cell is cylindrical with a radius of 14.5 mm and comprises a Fabry-Perot type through cavity with a length of 60 mm and a radius of 2 mm. A lateral neck 4 mm wide and concentric with the Fabry-Perot type cavity is positioned at mid-height between the two ends of the Fabry-Perot type cavity. To this neck is connected a lateral cavity 36 mm long and 4 mm wide, also concentric with the Fabry-Perot type cavity.
    This cell was manufactured by the Project SD3500 3D printer, whose characteristics of the Visijet Crystal resin used are presented below: - Density (g / cm): 1.02 (liquid, at 80 °) - Young's modulus: 1463 MPa - Stress-bending: 49 MPa
    The characterization presented and which makes it possible to study the acoustic properties of said cell for the audible frequencies, is obtained thanks to a stationary wave tube provided with 4 microphones. We used a 4206-T type transmission tube kit from Brüel & Kjær.
    The diameter of transmission tube used is 29 mm, which allows measurements to be made for the frequency range of [500: 6400] -Hz.
    A loudspeaker, placed at one end of the tube, generates white noise on the frequency band of interest.
    The pressure measurements are performed using two terminations provided different impedance.
    As shown in the transmission spectrum shown in Figure 6, we obtain an attenuation centered around 3kHz up to 40dB (sometimes 50dB), over a relative bandwidth of 133%.
    This result represents an improvement of 15 to 20 dB compared to the reflection of a cell simply provided with a Fabry-Perot type cavity, and for a frequency ranging from 1 to 5 kHz.
    In the description below, we designate the body of solid material indifferently body by solid material, solid body, cell body or simply body.
    权利要求:
    Claims (11)
    [1" id="c-fr-0001]
    An elementary cell (1; 1 '; 1 "; 10; 100; 100') of acoustic metamaterial comprising: - a body of solid material (2; 2 '; 2"; 20; 200; 200'); at least one Fabry-Perot cavity (3; 3 '; 3 "; 30; 300; 300') in said body (2; 2 '; 2"; 20; 200; 200'), and - at least one cavity lateral resonant (4; 4 '; 4 "; 41,42,43; 400; 400') communicating with said Fabry-Perot cavity (3; 3 '; 3"; 30; 300; 300').
    [2" id="c-fr-0002]
    The cell (1; 1 '; 1 "; 10; 100; 100') according to claim 1, wherein the lateral resonant cavity (4; 4 '; 4' '; 41,42,43; 400; 400'); ) is a Helmholtz or quarter-wave type acoustic resonator.
    [3" id="c-fr-0003]
    3. Cell (1; 1 '; 1 "; 10; 10 0; 100') according to any one of claims 1 and 2, wherein the cavity of Fabry-Perot type (3; 3 '; 3"; 300; 300 ') is a conduit passing through said body (2; 2'; 2 "; 200; 200 ').
    [4" id="c-fr-0004]
    4. Cell (1; 1 '; 1 "; 10; 10 0; 100') according to claim 3, wherein the through duct (3; 3 '; 3"; 30; 30,0; 3 0 0') is cylindrical.
    [5" id="c-fr-0005]
    5. Cell (1; 1 '; 1 "; 10; 100; 100') according to one of claims 1 to 4, wherein the cell body (2; 2 '; 2"; 20; 200; 200'); ) is parallelepipedal or cylindrical.
    [6" id="c-fr-0006]
    6. Cell (1; 1 '; 1 "; 10; 100; 100') according to one of claims 3 to 5, wherein the Helmholtz resonator is a cylindrical cavity (4; 4 '; 4"; , 42, 43; 400; 400 ') concentric with the through conduit (3; 3'; 3 "; 30; 30; 30 °) and communicating with said conduit (3; 3 '; 3"; 30; 300; 300 ') by a neck (5; 5'; 5 "; 50; 500; 500 ').
    [7" id="c-fr-0007]
    7. Cell (10) according to one of claims 1 to 6, wherein the body of solid material (20) comprises two Helmholtz resonators (41, 42, 43) or more, having different dimensions.
    [8" id="c-fr-0008]
    8. Cell (100; 100 ') according to any one of claims 1 to 7, wherein the Fabry-Pérot cavity (300') and / or the lateral resonant cavity (400) is (are) folded (s) of so as to have at least one entrance, at least one exit and at least two folds.
    [9" id="c-fr-0009]
    9. Acoustic display in the form of a panel comprising at least one elementary cell (1; 1 '; 1 "; 10; 100; 100') according to any one of claims 1 to 8.
    [10" id="c-fr-0010]
    10. An acoustic display according to claim 9, comprising a multitude of elementary cells (1; 1 '; 1 "; 10; 10 0; 10 0'), said cells being arranged in a plane of the panel so that each elementary cell ( 1; 1 "; 10; 10 0; 100 ') is able to act on another neighboring elementary cell (1; 1'; 1"; 10; 100; 100 ') to widen the reflection frequency band; .
    [11" id="c-fr-0011]
    The acoustic display of claim 10 wherein the elementary cells (1; 1 '; 1 "; 10; 10 0; 100') are arranged in said panel plane periodically.
    类似技术:
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    同族专利:
    公开号 | 公开日
    WO2017093690A1|2017-06-08|
    EP3384486A1|2018-10-10|
    FR3044813B1|2018-11-02|
    EP3384486B1|2021-07-28|
    ES2894800T3|2022-02-15|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    CN110609086A|2019-09-24|2019-12-24|哈尔滨工程大学|Experimental device for super material plate structure of acoustics|
    KR101825480B1|2016-04-29|2018-03-23|서울대학교산학협력단|Meta atom controlling acoustic parameters and metamaterials comprising the same|
    WO2018146489A1|2017-02-09|2018-08-16|The University Of Sussex|Acoustic wave manipulation by means of a time delay array|
    法律状态:
    2016-11-16| PLFP| Fee payment|Year of fee payment: 2 |
    2017-06-09| PLSC| Publication of the preliminary search report|Effective date: 20170609 |
    2017-10-19| PLFP| Fee payment|Year of fee payment: 3 |
    2019-12-27| PLFP| Fee payment|Year of fee payment: 5 |
    2020-12-22| PLFP| Fee payment|Year of fee payment: 6 |
    2021-01-15| CL| Concession to grant licences|Name of requester: SATT SAYENS, FR Effective date: 20201207 |
    2021-01-15| AU| Other action affecting the ownership or exploitation of an industrial property right|Effective date: 20201209 |
    2021-12-30| PLFP| Fee payment|Year of fee payment: 7 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1561750|2015-12-02|
    FR1561750A|FR3044813B1|2015-12-02|2015-12-02|REFLECTOR ACOUSTIC METAMATERIAL|FR1561750A| FR3044813B1|2015-12-02|2015-12-02|REFLECTOR ACOUSTIC METAMATERIAL|
    PCT/FR2016/053187| WO2017093690A1|2015-12-02|2016-12-02|Reflective acoustic metamaterial|
    ES16819152T| ES2894800T3|2015-12-02|2016-12-02|reflective acoustic metamaterial|
    EP16819152.6A| EP3384486B1|2015-12-02|2016-12-02|Reflective acoustic metamaterial|
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