JP5940634B2 - Sound transmissive material, and sound adjustment surface structure including architectural use using the material, microphone windshield, protective grill, sound transmissive projection screen and speaker - Google Patents

Description

  The present invention relates to a sound-transmitting material formed by entanglement of fiber materials, and more particularly to a sound-transmitting material having self-supporting properties. Furthermore, the present invention relates to an acoustic adjustment surface structure including a building application to which the sound transmission material is applied, a microphone windshield, a protective grill, a sound transmission projection screen, and a speaker.

  In various fields such as architecture and electronic equipment, materials that transmit sound are required. Examples of the sound transmitting material include a mesh structure such as a speaker salannet, and a perforated plate used for a building wall.

  Unlike these conventional sound-transmitting materials, it has a hard texture and does not have an opening or is not visible even though it does not appear to be transparent, but almost completely transmits sound. As a material, a sound-transmitting plate member or sheet member has been proposed (Patent Document 1).

  In addition, as a plate-like sound-transmitting material, it has been reported that sound transmittance can be obtained by providing a large number of micropores per area on a hard plate that cannot be visually recognized (Patent Documents 1 and 2). Non-patent document 1). Since the sound-transmitting material can provide a hard sound-transmitting material, it has been proposed to apply it as a movie screen and install a speaker on the back of the screen to enhance the sense of reality.

JP 2010-59658 A JP 2010-210778 A

Nakai, Kawakami, Wada, Sano “Acoustic Properties of Perforated Plates”, Acoustical Society of Japan, Architectural Acoustics Study Group (AA2009-18), 2009.03.11

  When a sound transmissive material is erected in an application such as a building material, the sound permeable material itself may be required to be self-supporting in a standing state without providing an auxiliary mechanism. According to the sound-transmitting material of Patent Document 1, if the sound-transmitting material is made self-supporting, there is a problem that the sound-transmitting property is impaired. Moreover, according to the sound-transmitting material of Patent Document 2 and Non-Patent Document 1, although it has self-supporting property, it is necessary to provide a large number of fine holes, so that there is a problem that the manufacturing cost increases due to special drilling techniques and skilled training. there were. Therefore, an object of the present invention is to provide a sound-transmitting material having a self-supporting property and a high-performance sound-transmitting property by using a material formed by entanglement of fibers.

  As a result of examining the fiber material that achieves both self-supporting property and sound transmission property, the present inventor has increased the fiber density to increase the amount of fiber used for the fiber material in an attempt to ensure self-supporting property, and the sound transmission is too high. We have found that the problem is that the fibers are entangled so tightly that they are hindered.

That is, the acoustic energy reflectance | r ² | (where r is the sound pressure reflectance) at the material interface is expressed by the following equation (1).

The acoustic energy reflectivity | r ² | indicates that the normal acoustic impedance Zn of the material surface is Zn = ρc (ρc is the characteristic impedance of air) or the specific acoustic impedance ζ (value obtained by dividing Zn by ρc) is ζ≡Zn / ( When ρc) = 1, the minimum value | r ² | = 0, and all the incident sound energy enters the material, and apparently, the sound absorption coefficient α = 1− | r ² | Basics of sound absorption "Acoustic technology No.71 / sep.1990). This condition, Zn = ρc, is that the material condition is equal to air, and the amount of air contained in the material, that is, porosity (porosity = porosity); the air contained inside the material's apparent volume The amount of incident sound energy into the material increases as the amount increases (the specific definition will be described later). Therefore, if the conditions inside the material, for example, flow resiliency (unit thickness flow resistance) and tortoise (maze degree) (Hiroshi Nakagawa “About Acoustic Materials (Part 3)” Nittobo Engineering Technology News) The amount of energy Eh absorbed is constant, and the amount of acoustic energy that escapes behind the larger the void ratio, that is, the transmittance τ (τ = | t | ² = Et / Ei; the ratio of the transmitted energy Et to the incident energy Ei, t. Is the sound pressure transmittance) (τ ≒ 1), that is, the insertion loss (level difference (dB) when there is no sample) and when there is no sample) can be minimized. It has been found that conditions close to permeability can be realized (see FIG. 12).

  Furthermore, in order to obtain sufficient sound transmission in a material having self-supporting properties, it is found that not only the porosity of the material used but also the relationship with the thickness is important, and the porosity is high. It has been found that a material having a thickness equal to or less than a predetermined value exhibits sufficiently high sound permeability.

That is, the present invention (1) is an acoustically transparent material in which fibers are entangled with each other,
The sound transmitting material is a sound transmitting material having a Taber stiffness of 5 mN · m or more, a bending resistance of 100 mN or more, a porosity of 50% or more, and a thickness of 3 mm or less.

  The present invention (2) is the sound-transmitting material of the invention (1), wherein the fiber is a metal fiber.

  The present invention (3) is the sound transmissive material according to the invention (1) or (2), wherein the insertion loss is 5 dB or less in each 1/1 octave band of 63 Hz to 8 kHz.

  The present invention (4) is the sound transmissive material according to any one of the inventions (1) to (3), wherein the sound transmissive material is a material obtained by compression molding metal fibers.

The present invention (5) includes any one of the sound transmissive materials of the inventions (1) to (4) (for example, the sound transmissive material 2 in FIG. 1),
An acoustic adjustment surface structure (for example, an acoustic adjustment surface structure 1 in FIG. 1) including an acoustic adjustment mechanism (for example, an acoustic adjustment mechanism 3 in FIG. 1) having a sound absorbing structure and / or a reflective structure installed on the back surface thereof. ).

  The present invention (6) is the acoustic adjustment surface structure according to the invention (5), wherein the acoustic adjustment mechanism is a variable acoustic adjustment mechanism capable of changing an arrangement ratio of the sound absorbing structure and / or the reflective structure.

The present invention (7) is an acoustic adjustment surface structure in a building wall and / or ceiling interior,
The sound-transmitting material is disposed so that a space is formed between the wall surface and / or the ceiling of the building (for example, the sound-transmitting material 2 in FIG. 3),
The variable sound adjustment mechanism (for example, the variable sound adjustment mechanism 610) has a curtain or a sound-absorbing blind arranged in the space and configured to be openable and closable (for example, a curtain 613).
The acoustic adjustment surface structure (for example, the reverberation variable wall 600) of the invention (6), wherein the sound absorption characteristics of the surface are adjusted by opening and closing the curtain or the blind.

The present invention (8) is an acoustic adjustment surface structure in the interior of a wall and / or ceiling of a building,
The sound-transmitting material is disposed so that a space is formed between the wall surface and / or the ceiling of the building (for example, the sound-transmitting material 2 in FIG. 4),
The acoustic adjustment mechanism has a sound absorbing structure and / or a reflective structure arranged in the space (for example, a sound absorbing material 701, an air layer 702, a plywood 704, a space A), and the acoustic adjustment of the invention (5). It is a surface structure (for example, reverberation adjusting wall 700).

  The present invention (9) is an interior structure of a building having the acoustic adjustment surface structure according to any one of the inventions (5) to (8).

The present invention (10) is a windshield for a microphone for reducing wind noise of the microphone.
The windshield has an acoustically transparent material arranged at a position that blocks the wind against the microphone;
The sound-transmitting material is a windshield for a microphone, which is the sound-transmitting material according to any one of the inventions (1) to (4).

The present invention (11) is a protective grill arranged on the front surface of a microphone or a speaker.
The grill is a protective grill made of the sound-transmitting material according to any one of the inventions (1) to (4).

The present invention (12) is an acoustically transmissive projection screen that has a front projection type projection projection surface and is configured to use a speaker arranged behind the image projection surface to emit sound.
At least the video projection surface is an acoustically transmissive projection screen made of the acoustically transmissive material according to any one of the inventions (1) to (4).

The present invention (13) is a speaker having a speaker box and a woofer unit.
The sound-transmitting material according to any one of the inventions (1) to (4), a sound-absorbing material composed of a porous sound-absorbing material disposed behind the sound-transmitting material, and disposed behind the sound-absorbing material The speaker is characterized in that a sound absorbing structure having an air layer is provided in the speaker box, and the sound absorbing structure is provided on an inner wall of the speaker box.

  The present invention (14) is the speaker according to the invention (13), wherein the speaker is a sealed type.

  According to the sound-transmitting material of the present invention, the Taber stiffness is 5 mN · m or more, the bending resistance is 100 mN or more, the porosity is 50% or more, and the thickness is 3 mm or less. A material with high performance sound transmission is obtained.

FIG. 1A is a cross-sectional view of the acoustic adjustment surface structure of the present invention, and FIG. 1B is an exploded view of the acoustic adjustment surface structure of the present invention. FIG. 2 is a schematic configuration diagram illustrating a case where the acoustic adjustment surface structure is used for a building interior. FIG. 3 is a schematic configuration diagram of a reverberation variable wall 600 whose appearance does not change. FIG. 4 is a schematic configuration diagram of a reverberation adjusting wall 700 whose appearance does not change. FIG. 5 is a schematic configuration diagram of a spherical windshield (for a sound field microphone) using a sound-transmitting material. FIG. 6 is a schematic configuration diagram of a surface acoustic pressure measuring microphone device with a cylindrical windshield. FIG. 7 shows an outline of an insertion loss Δ (dB) measurement method for evaluating sound transmission in the measurement method 1. FIG. 8 is an auxiliary explanatory diagram related to the measurement method 2. FIG. 9 shows the results of a comparative test of the sound absorption coefficient α ₀ of the back sound absorbing material (GW) with and without the sound transmitting material (TTP). FIG. 10 shows the results of measuring the sound permeability of each sample in Measurement Method 2. FIG. 11A shows an outline of a system in which the wind noise reduction test was performed, and FIG. 11B is a graph showing the results of the wind noise reduction test. FIG. 12 is a supplementary explanatory diagram regarding the amount of acoustic energy that escapes behind.

  The present invention is an acoustically transparent material in which fibers are entangled with each other. That is, the sound transmission material of the present invention has a Taber stiffness of 5 mN · m or more and a bending resistance of 100 mN or more. By being in this range, the sound-transmitting material has self-supporting properties. In addition, in the sound transmitting material having self-supporting properties, a material having high sound transmitting property can be obtained by setting the porosity to 50% or more and the thickness of 3 mm or less.

  The Taber stiffness of the sound transmitting material of the present invention is 5 mN · m or more, preferably 8 mN · m or more, and more preferably 10 mN · m or more. The upper limit value of the Taber stiffness is not particularly limited, but is, for example, 100 mN · m. By having the Taber stiffness within the range, a material having self-supporting properties can be obtained. Taber stiffness is measured according to JIS-P8125. The Taber stiffness value can be adjusted by the hardness of the fibers used, the density of the sound-transmitting material, and the pressure in compression molding based on the knowledge of those skilled in the art.

  The bending resistance of the sound transmission material of the present invention is 100 mN or more, preferably 150 mN or more, and more preferably 200 mN or more. The upper limit of the bending resistance is not particularly limited, but is, for example, 2000 mN. By having the Taber stiffness within the range, a material having self-supporting properties can be obtained. The bending resistance is a value obtained by measurement according to the Taber stiffness test of JIS-P8125. The value of the bending resistance can be adjusted by the hardness of the fibers used, the density of the sound-transmitting material, and the pressure in compression molding based on the knowledge of those skilled in the art.

  The porosity of the sound transmitting material of the present invention is 50% or more, preferably 60 to 90%, more preferably 70 to 90%. The upper limit of the porosity is not particularly limited, but is 95%, for example. In the material in which the fibers are entangled, by selecting a material whose porosity is included in the range, there is an effect that sound permeability is ensured while having self-supporting property. Moreover, since the porosity is not too high in a preferable range and a more preferable range, even when used as a wall material or the like, the opposite side can be prevented from being seen through the sound transmitting material.

  In consideration of the angle dependency of sound transmission, the porosity of the sound transmission material is particularly preferably 80 to 90%. By setting it as such a range, it is possible to exhibit high sound permeability that hardly depends on the incident angle of sound with respect to the material.

The porosity is a ratio of a space in which no fiber exists with respect to the volume of the sound transmitting material, and is calculated from the volume and weight of the sound transmitting material and the specific gravity of the fiber material.
Porosity (%) = (1−weight of sound transmitting material / (volume of sound transmitting material × specific gravity of fiber)) × 100
The value of the porosity can be adjusted based on the knowledge of those skilled in the art by the thickness and amount of the fibers used, the density of the materials entangled with the fibers, and the pressure in compression molding.

  Here, the thickness of the sound transmitting material is 3 mm or less, more preferably 50 μm to 2000 μm, still more preferably 100 μm to 1500 μm, and particularly preferably 500 μm to 1000 μm. In the material having the above porosity, by setting the thickness within the above range, a material having high sound permeability can be obtained.

  The sound-transmitting material according to the present invention is obtained by interlacing fibers. Examples of the fiber used for the sound transmissive material include metal fibers and fluorine fibers. Among these, it becomes easy to ensure independence by using a metal fiber.

  Although it does not specifically limit as a metal fiber. Examples thereof include one type or a combination of two or more types selected from fibers made of metal materials such as stainless steel, aluminum, brass, copper, titanium, nickel, gold, platinum, and lead.

  The fluorofiber is preferably selected from thermoplastic fluororesins, such as polytetrafluoroethylene (PTFE), tetrafluoroethylene (TFE), perfluoroether (PFE), tetrafluoroethylene and hexafluoropropylene. Copolymer (FEP) with tetrafluoroethylene and ethylene or propylene (ETFE), vinylidene fluoride resin (PVDF), polychlorotrifluoroethylene resin (PCTFE), and vinyl fluoride resin (PVF). It is done.

  Moreover, the diameter of the fiber used for the sound-transmitting material of the present invention is not particularly limited. For example, 0.1 to 100 μm is preferable, 0.5 to 50 μm is more preferable, and 1 to 40 μm is more preferable. Is preferred. By setting the fiber diameter in such a range, it is possible to increase the strength of the fiber and to easily obtain an appropriate sound transmittance.

  The sound-transmitting material can be obtained by a method of compression-molding a fiber, or by papermaking a raw material including the fiber by a wet papermaking method.

When the acoustically transparent material of the present invention is produced using metal fibers or fluorine fibers by compression molding, the webs are first formed by collecting and preliminarily compressing the fibers. Or in order to provide the coupling | bonding between fibers, you may impregnate a binder between fibers. The binder is not particularly limited. For example, in addition to organic binders such as acrylic adhesives, epoxy adhesives, and urethane adhesives, inorganic adhesives such as colloidal silica, water glass, and sodium silicate are used. Can be used. Instead of impregnating with the binder, the surface of the fiber may be preliminarily coated with a heat-adhesive resin, and an assembly of metal fibers may be laminated and then heated and bonded. The amount of the binder impregnated is preferably 5 to 130 g and more preferably ²⁰ to 70 g with respect to the sheet surface weight of 1000 g / m ² .

  A sheet is formed by pressing an aggregate of metal fibers under heating. The heating conditions are set in consideration of the drying temperature and curing temperature of the binder and the thermoadhesive resin to be used, and the heating temperature is usually about 50 to 1000 ° C. The pressurizing pressure is adjusted in consideration of the elasticity of the fiber, the thickness of the sound transmitting material, and the light transmittance of the sound transmitting material. In the case where the binder is impregnated by the spray method, it is preferable to form the metal fiber layer to a predetermined thickness by press working or the like before spraying.

  In the case of using a metal fiber, the sound-transmitting material can form a slurry of a metal fiber-containing slurry by a wet papermaking method. In addition, when producing a slurry containing metal fibers, the dispersibility of the metal fibers in water may deteriorate, so a polymer aqueous solution such as polyvinylpyrrolidone, polyvinyl alcohol, or carboxymethylcellulose (CMC) having a thickening action may be used. A small amount may be added. In addition, as a papermaking method, various methods such as long net papermaking, circular net papermaking, and inclined wire papermaking can be employed as necessary.

  When the wet papermaking method is used, it is preferable that the metal fiber is formed through a fiber entanglement treatment step in which the metal fibers forming a sheet containing moisture on the net are entangled with each other. Here, as the fiber entanglement treatment step, for example, it is preferable to employ a fiber entanglement treatment step of injecting a high-pressure jet water flow onto the metal fiber sheet surface after papermaking, specifically, a direction orthogonal to the sheet flow direction. By arranging a plurality of nozzles at the same time and simultaneously injecting a high-pressure jet water stream from the plurality of nozzles, the metal fibers can be entangled over the entire sheet.

  Further, the method for producing a metal fiber material may include a sintering step in which the obtained metal fiber material is sintered at a temperature below the melting point of the metal fiber in a vacuum or in a non-oxidizing atmosphere after the wet papermaking step described above. preferable. Since the metal fibers are entangled, the strength of the sintered metal fiber material can be increased.

  The method for producing sound-transmitting material using fluorine fibers is to mix fluorine fiber and a material having a self-adhesive function by wet papermaking and then drying the fluorine fiber mixed paper material. After thermocompression bonding as described above, the fibers of the fluorine fibers are thermally fused together, and then the substance having a self-adhesive function is dissolved and removed with a solvent and, if necessary, dried again. Here, as a substance having a self-adhesive function, natural pulp made of plant fibers such as wood, cotton, hemp, straw, etc., usually used for papermaking, polyvinyl alcohol (PVA), polyester, aromatic polyamide, acrylic, polyolefin Synthetic pulp and synthetic fibers made of thermoplastic synthetic polymers, and paper-making paper strength enhancers made of natural polymers and synthetic polymers can be used, but they have a self-adhesive function and are mixed with fluorine fibers. And if it can disperse | distribute to water, it will not be limited to these.

(Physical properties)
Sound transmission material The sound transmission material according to the present invention has a frequency characteristic difference (hereinafter referred to as “insertion loss”) measured according to the following measurement method 1 and each 1/1 octave band having a center frequency of 63 Hz to 8 kHz. And within 5 dB (preferably within 2 dB). The sound-transmitting material is preferably within 6 dB (preferably within 3 dB) in each 1/3 octave band with a center frequency of 31.5 Hz to 16 kHz. When a continuous sine wave sweep is used, it is based on the case where the evaluation is performed in the 1/3 octave band.

  Various methods are envisaged as an evaluation method for sound transmission. More specifically, in the anechoic room or highly sound-absorbing room, the microphone and the speaker are directly in the direct sound area of the former with respect to the latter (the direct sound area is sufficiently close to the indirect sound (reflected sound / reverberant sound)). The level difference of the response of the microphone to the speaker (dB) when the sample is placed at a right angle to the reference line (line connecting the microphone and the speaker) and when the sample is not placed. ) Is evaluated as insertion loss Δ (dB). Incidentally, the signal generated from the speaker may be a sine wave, pink noise, or a tremor (FM sound), the duration may be either continuous or short, and the filter for band limiting is a sound source. Either the side or the receiving side, or a short sound or a continuous frequency sweep sound may be used. At the same time, the position of the sample may be just before the speaker, just before the microphone, or between the two, and these have the same result as long as the measurement system is regarded as a linear system. Incidentally, here, it is defined that the sample is evaluated at a right angle to the reference line, but if necessary, the sample may be installed at an angle with respect to the reference line, and the angle dependence thereof may be evaluated. In addition, when a difference arises in a result according to the measurement method, priority is given to the result obtained by the method of the following measurement method 1 in the sound transmittance in the specification.

Measurement method 1: The most simple method of measuring insertion loss is an axis connecting a speaker and a microphone (hereinafter referred to as “speaker-microphone axis”) in an anechoic chamber or a highly sound-absorbing chamber equivalent thereto. Assuming that the angle θ = 0 ° formed by the normal direction of the sound transmission material (the state shown in FIG. 7 is an angle θ = 0), a continuous sine wave sweep sound between 20 Hz and 20 kHz (with respect to background noise) (Sound of 20 dB or more in S / N ratio), and after receiving the sound with a microphone or a sound level meter, etc., located several tens of centimeters to several meters (preferably about 30 cm to 5 m) away from this speaker, Measure the difference between the frequency response characteristics when recorded on a level recorder, etc., and the frequency response characteristics when the member is installed immediately before or between the speakers or microphone, and insert this Loss △ and (dB).

  The sound transmission material according to the present invention can be evaluated by the insertion loss measured according to the following measurement method 2 to evaluate the dependency of the sound incident angle.

Measurement method 2: An angle θ formed by the speaker-microphone axis and the normal direction of the sound transmission material (the state shown in FIG. 7 is assumed to be an angle θ = 0), and θ = 0 to 90 degrees for each arbitrary angle Or the average insertion loss Δ (−) for each angle with an average energy value (dB average) of n insertion losses included in adjacent ± Δθ for each representative angle θi. i (dB) can also be used (FIG. 8). This makes it possible to evaluate the dependence of the insertion loss on the angle. For example, when taking an energy average value (dB average) of three angles every ± 10 degrees adjacent to each angle of i = 15 degrees, 45 degrees, and 75 degrees, the following formulas (a) to (c) or (d) It can obtain | require by (f).
(In the above formulas (e) to (f), L′ 5, L5, etc. are the frequency response (dB) of the microphone when the member is installed at θ = 5 degrees, and the frequency response (dB) before installation, respectively. In this example, the evaluation can be performed from various angles, which is suitable for the evaluation of the material according to the present invention.

Wind noise reduction effect In the wind noise reduction effect evaluation method, the windshield according to the present invention preferably has a wind noise reduction effect of Δ20 dBA or more in a 1/1 octave band with respect to a wind having a wind speed of 2.7 m / s. It is. Here, in the wind noise reduction effect evaluation test, wind was blown from an air blower or the like in an anechoic chamber at a wind speed of 2.7 m / s (where wind noise was observed or wind noise reduction could be observed). When the response measured with the windshield attached is reduced by S (dBA) in the noise level (dBA) with respect to the microphone output response observed without feeding and windshield, the wind noise reduction effect ΔS (dBA) To do.

(Sound adjustment surface structure used for the inner wall of buildings)
FIG. 1 is a schematic configuration diagram of the acoustic adjustment surface structure of the present invention. FIG. 1A is a cross-sectional view of the acoustic adjustment surface structure of the present invention, and FIG. 1B is an exploded view of the acoustic adjustment surface structure of the present invention. The acoustic adjustment surface structure 1 of the present invention includes the above-described sound-transmitting material 2 formed into a plate shape used as a decorative board, and a sound-absorbing structure and / or a reflecting structure disposed behind the sound-transmitting material. And an acoustic adjustment mechanism 3 having By using the sound-transmitting material of the present invention as a decorative plate having a sound-adjusting surface structure, not only the sound-transmitting properties but also the material itself is self-supporting, so the surface exhibits the same texture as a hard non-porous plate. It provides the result of so-called “hard sound absorbing material” and can be applied to the walls of museums to form a quiet space. Further, if necessary, reinforcement may be performed behind the sound-transmitting material by a material / structure that does not affect sound-transmitting properties such as a honeycomb structure or a metal mesh such as an expanded metal.

  The sound absorbing structure in the acoustic adjustment mechanism 3 can be realized by arranging a sound absorbing material, for example. As the sound absorbing material, known materials can be used, and for example, glass wool, needle felt, urethane foam, sponge, rock wool board and the like can be used. The sound absorbing structure may have a sound absorbing material and an air layer disposed behind the sound absorbing material. By providing the air layer in this way, it is possible to extend the sound absorption force to the low sound range.

  The reflective structure in the acoustic adjustment mechanism 3 can be realized by disposing nothing or a reflecting material, for example. A known material can be used as the reflecting material, and examples thereof include a board in which no hole is formed, such as a plywood board, a gypsum board, a concrete board, and a flexible board.

  In order to support the structure, these acoustic adjustment surface structures have a skeleton 4 having a space 41 in which the acoustic adjustment mechanism 3 is accommodated and a support column 42 in which a fixing surface 421 for fixing the acoustically transmissive material 2 is formed. It is preferable to further include (FIG. 1B). Such a panel makes it possible to easily attach to a room where an acoustic disturbance such as a crying dragon is occurring, for example, and solve the problem.

  When the skeleton 4 is provided, the acoustic adjustment surface structure 1 is attached to the skeleton 4, the acoustic adjustment mechanism 3 housed in the space 41 of the skeleton 4, and the fixed surface 421 of the skeleton support 42. And sound transmissive material 2. If necessary, the skeleton 4 may be provided with a trunk edge 43 and a spacer 44 in the middle to reinforce the entire structure (see FIG. 2). In this case as well, an air layer may be provided as appropriate behind the sound absorbing material.

  As an operation of the acoustic adjustment surface structure of the present invention, sound reaches the acoustic adjustment surface structure of the present invention, passes through the sound-transmitting material, and reaches the sound-absorbing structure to be absorbed, or is a reflective structure. To reach and be reflected. At this time, by using the sound-transmitting material of the present invention, it is possible to prevent the sound from rebounding on the wall surface, so that it is easy to reflect the acoustic characteristics of the object placed behind the sound-transmitting material, It can be effectively used as an acoustic improvement panel that can easily solve acoustic disturbances in conference rooms in office buildings and a sound field adjustment panel in audio rooms and AV rooms in houses.

  The acoustic adjustment surface structure 1 of the present invention provides, for example, a “hard sound absorbing surface” that has never existed by using it as an interior structure of a building, and effectively absorbs sound in a space that requires a flat and hard interior surface. Can be processed.

  FIG. 2 is a diagram showing a schematic configuration of an interior structure of a building using the acoustic adjustment surface structure 1 of the present invention. The interior structure 6 has a structure in which the acoustic adjustment surface structures 1 are arranged side by side, and may be provided with a body edge 43 and an intermediate column 44 in the middle to reinforce the entire structure as necessary. An air layer may be provided behind the material to increase the sound absorption force toward the low frequency side.

  The interior structure 6 can constitute a wall surface, for example, and the height of the acoustic adjustment surface structure 1 may be the length from the floor end F to the ceiling end R of the wall surface. Even when the continuously formed surface becomes large by using the sound-transmitting material of the present invention, it is easy to construct because of its independence, and wrinkles and tarmi are also formed after construction. It becomes difficult.

  As a matter of course, the surface of the acoustic adjustment surface structure may be continuous. Reflective structure (see FIG. 9 (0)) having the same surface using the sound-transmitting material of the present invention in the middle and having no sound-absorbing material behind it, or sound-transmitting according to the present invention as a surface decorative material Depending on the usage of the room without changing the room design at all, by adjusting the total sound absorption capacity of the room by arranging a reflective structure, such as a plywood or gypsum board, behind the functional material. The optimum reverberation characteristics can be provided.

  Further, the sound absorbing material behind the interior structure 6 is omitted, and it is composed only of a surface material, that is, the sound transmitting material of the present invention as shown in FIG. 3, and a variable sound absorbing mechanism such as a curtain and a sound absorbing blind (sound absorbing louver) is provided behind. The reverberation variable wall or the reverberation variable ceiling may be configured without changing the indoor design at all, and the reverberation characteristics in the room may be freely changed. Since the room design does not change, it does not give a sense of incongruity to the occupants and the audience and performers (such as in the case of a hall).

  More specifically, FIG. 3 shows a reverberation variable wall 600 as an application example of the sound adjustment surface structure using the sound transmission material of the present invention as a surface material. FIG. 3 is an example of a reverberation variable wall intended for use in a hall, a residential AV room, a recording studio, a music rehearsal room, or the like. Since the sound transmitting member of the present invention is used as the surface member, the sound absorption force of the wall surface and ceiling surface is changed by operating the variable acoustic adjustment mechanism at the back without changing the design of the surface, and the reverberation time characteristic of the room is changed. Can be changed. According to the said structure, there exists an effect that the design of a surface does not change, although acoustic conditions change.

  More specifically, FIG. 3 shows a schematic configuration diagram of the reverberation variable wall 600, which is a cross-sectional view seen from the upper viewpoint of the room. The reverberation variable wall 600 includes the sound transmissive material 2 provided on the entire wall surface, and a variable sound adjustment mechanism 610 disposed behind the sound transmissive material.

  The variable sound adjusting mechanism 610 includes, for example, a sound absorbing curtain 613 attached to a curtain rail provided in a ceiling portion of the space behind the sound transmissive material 2, and a curtain box 615 for storing the curtain. Have. The curtain 613 may have an opening / closing mechanism that can be opened / closed electrically.

  The variable acoustic adjustment mechanism 610 can change the acoustic characteristics of the wall surface by opening and closing the curtain 613 disposed behind the sound transmission material. That is, the appearance of the wall is not changed due to the presence of the sound-transmitting material, but the area occupied by the sound-absorbing material changes when the curtain is opened and closed. Changes. That is, conventionally, in order to change the acoustic characteristics, a sound absorbing material and a reflective material have to be installed, and the appearance has changed greatly. However, the acoustic characteristics can be changed without changing the appearance. The reverberation variable wall 600 exhibits a high effect particularly in a space constrained by the appearance design such as a concert hall or a movie theater.

  A reverberation adjusting wall is shown as an application example of the sound adjusting surface structure using the sound transmitting material of the present invention as a surface material. FIG. 4 is a schematic configuration diagram of a reverberation adjusting wall 700 according to the present invention. With this configuration, it is possible to provide a complete reflection surface to a complete sound absorption surface with the surface design unified.

  The reverberation adjusting wall 700 includes a sound transmissive material 2 disposed in a space in front of the wall, and a sound absorbing structure and / or a reflective structure disposed in the space formed behind the sound transmissive material. And have. For example, a sound absorbing surface can be formed by arranging a sound absorbing structure including a sound absorbing material 701 and an air layer 702 behind the sound transmitting material 2. In addition, a highly reflective surface can be formed by arranging a reflective structure made of the plywood 704 behind the acoustically transparent material 2. Alternatively, a weak reflective surface can be formed by arranging a space A (the back material is omitted) as a reflective structure behind the sound transmitting material 2. By selecting the material behind the sound transmitting material in this way, it is possible to realize free sound absorption characteristics without considering design. Note that an air layer may or may not be provided behind the sound absorbing surface, but the sound absorbing property of the sound absorbing surface can be extended to a lower sound range by providing the air layer.

(Microphone windshield)
The sound-transmitting material of the present invention is a high-pass filter that effectively blocks the wind corresponding to the DC component of the electrical signal and allows the acoustic signal corresponding to the AC signal to pass through without loss due to its special structure. Since there is such a function, a windscreen for a microphone can be effectively constructed. The structure of the windshield for the microphone is not particularly limited as long as the windshield for the microphone is blocked. The sound-transmitting material of the present invention can achieve both self-sustainability and sound-transmitting properties by having Taber stiffness, bending resistance, porosity, and thickness within a predetermined range, but this effectively reduces wind noise. be able to. Furthermore, since the material is self-supporting, the present invention is applied to the surface of a spherical shape, a rectangular parallelepiped shape, a conical shape, a spherical shape, a streamline shape, etc., instead of the conventional filling type windshield (made of sponge or urethane). A windshield having a hollow structure can be formed by arranging the sound transmitting material.

  FIG. 5 shows a schematic configuration diagram of the windshield 200 having a hollow structure. The windshield 200 having a hollow structure includes a screen portion 210 made of a sound transmissive material according to the present invention and a cap portion 220 for waterproof protection. Thus, the windshield 200 is comprised combining the screen part 210 and the waterproof protection cap part 220 (FIG.5 (b)). With this configuration, a microphone is inserted into the waterproof protection cap portion 220 for use.

  The waterproof protection cap portion 220 is composed of a tip cap portion 221 that covers the sound collection portion of the microphone composed of the sound transmitting material according to the present invention, a hard cylindrical material such as a metal tube, and And a body cap portion 222 that is in close contact with the body portion of the microphone. In addition, a circular rod 223 for determining the position of the screen unit 210 may be provided around the body cap unit 222.

  The microphone device 250 using the windshield has a cylindrical body part 2511, a microphone 251 having a sound collecting part 2512 formed at the tip of the body part, a waterproof protection cap part 220 that covers the microphone, and , A hollow screen portion 210 covering at least the sound collection portion 2512; the screen portion 210; an airtight rubber packing 253 for providing airtightness inside the screen; the screen portion 210; and a waterproof cap portion 220. And a metal plate 254 that is fixed via the rubber packing (FIG. 5A).

  Further, when the sound transmitting material according to the present invention is used, a hollow windshield utilizing self-sustainability can be configured as described above, and in particular, it is used as a windshield for a surface sound pressure measurement microphone. Is preferred. By using the sound-transmitting material of the present invention, it is possible to effectively reduce and block wind intrusion without flaking or resonating on the surface even under strong winds with high wind speeds. It is most suitable for constituting a windshield in a low sound range and a windshield used under strong winds.

(Microphone device for surface sound pressure measurement with cylindrical windshield)
FIG. 6 is a schematic configuration diagram of a microphone device 300 for measuring the surface sound pressure with a cylindrical windshield according to the present invention. The surface acoustic pressure measurement microphone device 300 according to the present invention includes a windshield 320 having a frame body 321 and a sound-transmitting material 322 formed on the upper surface of the frame body, and a microphone 330 provided inside the windshield. And have. Further, a streamline edge portion 323 may be provided on the outer edge of the frame body 321 in order to make the wind flow smoothly. Here, the shape of the frame body 321 is not particularly limited, and examples thereof include a cylindrical shape. The height h of the frame body 321 is not particularly limited, but previous studies (Fukuji Kawakami, Susumu Inamoto, Shinichi Teramata, Yasuo Inoue, Takayuki Sano “Development of a waterproof windshield for low frequency sound measurement” Proceedings of the annual meeting of the academic conference, 2011.03, page 36, (1-12-23)) to circular (in the case of a spherical body) and the diameter d of the cylinder have an optimal balance, and d when the height is h = 10 mm It has been found that about 70 mm is optimal. If you want to extend the windshield effect to the low range, unless there is any other reason, d and h are 1 octave (extension effect to the low range) while maintaining this basic balance (height h: diameter d = 1: 7) It is preferable to increase the size in such a manner that it doubles.

  For general applications, the height h of the cylinder is preferably in the range of 1 mm to several tens of mm, more preferably in the range of 1 mm to 50 mm, and even more preferably in the range of 10 mm to 30 mm. On the other hand, when the height h is lower than 1 mm, the effect of preventing wind noise is not sufficiently obtained, which is not preferable. When the height h is higher than several tens of centimeters, a new wind noise is generated due to air turbulence around the windshield, and there is no path difference in the so-called barrier effect (soundproof effect). A difference in distance from the sound source to the sound receiving point) occurs, and the insertion loss increases, or the sound source position, that is, the incident angle varies, resulting in directivity. For this reason, it is preferable that the shape of the peripheral part is a streamlined cross section like a streamline edge 323 in FIG. 6 by a filling type inclined material such as clay having a right triangle or a quarter circle cross section through caulking treatment. . When this measure is taken, in particular, by setting the height of the frame to around 10 mm or more, an appropriate space is formed between the microphone and the windshield, and wind noise is significantly reduced. It has been confirmed. Moreover, the said height can be adjusted by overlapping the frame body 321 which concerns on this invention (FIG. 6 (a)-(c)).

  The shape of the frame is preferably cylindrical, and the diameter d of the cylinder is not particularly limited. However, as described above, the shape (reducing low-frequency wind noise) is maintained while maintaining a substantially similar shape according to the height h. It is preferable to change according to the limit. Generally, 5 mm or more is preferable, 30 mm or more is more preferable, and 70 mm or more is more preferable. However, it is preferable to increase the height h as the diameter increases. Although the upper limit of a cylindrical diameter is not specifically limited, For example, it is about 200 mm.

  The surface microphone device 300 according to the present invention can be attached to the surface B of a body such as an automobile or an airplane, or a vehicle body, and can measure noise during movement. Since the duct propagation noise can be picked up without being influenced by the above, it is possible to provide effective control and a large noise reduction effect when used for ANC (active noise control) or the like.

  The sound-transmitting material according to the present invention can be used as a protective grill disposed on the front surface of a microphone or a speaker. Moreover, when arrange | positioning in a front surface to a speaker, you may use as a decorative board which hides not only a speaker but the hole of the baffle port etc. which are formed in a front baffle, and the knob of a variable attenuator.

  In addition, the sound transmission material according to the present invention can be used as a movie screen by utilizing sound transmission and self-supporting properties. In this case, it is preferable to use a sound projection material according to the present invention by forming a front projection type projection projection surface and arranging a speaker behind the sound transmission material. In this way, even if the speaker is arranged on the back of the screen, the sound is transmitted without transmitting sound by using the sound transmitting material according to the present invention, so that the sound localization is improved.

  By using the sound transmitting material according to the present invention, a sound absorbing structure in a low sound range can be constructed. That is, the sound absorbing structure includes the sound transmitting material of the present invention, a sound absorbing material made of a porous sound absorbing material arranged behind the sound transmitting material, and an air layer arranged behind the sound absorbing material. . Conventional glass wool alone has been difficult to absorb in the low sound range, but by having such a structure, it is possible to absorb sound up to the low sound range. Examples of the porous sound absorbing material include glass wool and urethane foam.

  In a speaker having a sealed type or a speaker box of a form similar to this, a hollow structure is used with the sound transmitting material of the present invention instead of the sound absorbing material in the box that has conventionally only contributed to sound absorption in the middle and high range such as glass wool, Alternatively, by adopting a structure filled with porous sound absorbing material such as glass wool, the sound quality (sound quality) and volume (volume) emitted from the front surface with a large sound absorbing power mainly in the low frequency range can be improved. Can be planned. Here, the low frequency range is a range of sound emitted from the speaker, and in particular, a sound emitted from the front surface of the speaker unit (for example, a woofer unit) (here, assumed to be normal phase sound) and a sound emitted from the rear surface of the speaker unit. (Here, it is assumed that the sound is a reverse phase sound) means a sound range in which cancellation due to interference becomes a problem, and more specifically, for example, a sound range of 500 Hz or less. In this way, in the low sound range, the reverse phase sound emitted from the back of the speaker is said to be emitted to the front through elements such as the cone of the speaker unit due to sound reflection and wraparound in the sealed speaker box. ing. In this case, the normal phase sound emitted from the front surface of the speaker unit and the reverse phase sound intersect to cancel the sound. By arranging the sound absorbing structure according to the present invention in the speaker box, the reverse phase sound is absorbed, so that cancellation due to interference with the normal phase sound can be prevented, and the volume and quality of the sound can be improved. Become.

  More specifically, in a speaker box and a speaker having a woofer unit, the sound-transmitting material of the present invention, a sound-absorbing material made of a porous sound-absorbing material disposed behind the sound-transmitting material, and the sound-absorbing material A sound absorbing structure having an air layer disposed behind the material is provided in the speaker box. The sound absorbing structure is provided on the inner wall of the speaker box, and the air layer, the sound absorbing material, and the sound transmitting material are laminated in this order from the inner wall of the speaker.

  In addition, the sound transmitting material according to the present invention can be used in various fields by utilizing the sound transmitting property.

Example 1
A fiber having a wire diameter of 30 μm made of stainless steel AISI 316L was used, and the fibers were overlapped to form a cotton-like web. The web was weighed so that the basis weight was 950 g / m ² and compressed between flat plates so that the thickness was 800 μm. This compressed and plate-shaped product was put in a sintering furnace, heated to 1100 ° C. in a vacuum atmosphere, and sintered to obtain a sample.

Example 2
Using stainless steel AISI 316L fibers having a diameter of 6.5 μm and 12 μm, a web was prepared in the same manner as in Example 1. The web is mated to the front and back at a weight ratio of 7: 3. The webs with the front and back surfaces were weighed so that the basis weight was 850 g / m ² and compressed between flat plates so that the thickness was 400 μm. A sample was prepared in the same process as in Example 1 except for these conditions.

Example 3
A web was prepared in the same manner as in Example 1 using a copper wire having a diameter of 30 μm. The web was weighed so that the basis weight was 1100 g / m ² and compressed between flat plates so that the thickness was 800 μm. This compressed and plate-shaped product was put in a sintering furnace, heated to 900 ° C. in a vacuum atmosphere, and sintered to obtain a sample.

Example 4
A web was prepared in the same manner as in Example 1 using aluminum fiber having a wire diameter of 30 μm. The web was weighed so that the basis weight was 800 g / m ² and compressed between flat plates so that the thickness was 1000 μm. This compressed and plate-shaped product was put in a sintering furnace, heated to 800 ° C. in a hydrogen atmosphere, and sintered to obtain a sample.

Comparative Example 1
Using aluminum as a raw material, a fiber having a wire diameter of 100 μm is prepared by a melt spinning method. In the case of this fiber, since it becomes cottony at the time of fiber preparation, the cottony material is weighed so that the basis weight is 1650 g / m ^2. The sample was compressed between rolls so as to have a thickness of 5000 μm.

Comparative Example 2
A web was prepared in the same manner as in Example 1 using 100 μm aluminum fiber. The web was weighed so that the basis weight was 1500 g / m ² and compressed between flat plates so that the thickness was 1000 μm. This compressed and plate-shaped product was put in a sintering furnace, heated to 900 ° C. in a vacuum atmosphere, and sintered to obtain a sample.

Comparative Example 3
Fluorine fiber sheet “TOMY FILEC F” R-250 (manufactured by Shinyodogawa Paper) was used as a sample.

Comparative Example 4
A stainless fiber sheet “TOMY FILEC SS” SS8-50M (manufactured by Shinyodogawa Paper) was used as a sample.

(Autonomy)
Holding the end of a 5 cm square sample, the opposite end was lifted, and when it did not bend, it was evaluated as being “self-supporting”, and when it was bent, it was evaluated as being “self-supporting”.

(Taber stiffness / bending resistance)
It measured according to the Taber stiffness test (JIS-P8125).

(Thickness)
Measured with a micrometer.

(Porosity)
From the volume calculated from the outer dimensions of the sample, the mass of the entire sample, and the specific gravity of the fiber, the porosity was calculated from the following formula.
Porosity (%) = (1−weight of sound transmitting material / (volume of sound transmitting material × specific gravity of fiber)) × 100

(Sound transmission)
Measurement method 1
Based on the measuring method 1 demonstrated in this-application specification, the sound transmittance was evaluated. For transmission frequency characteristics, there are various methods such as continuous sine wave sweep, FM short sound, steady-state pink noise, and FM seismic sound. Here, as shown in FIG. A continuous sine wave sweep sound is emitted from the attached sound generating device of about 2250 cm ³ , and the sound transmitting material b of each example and each comparative example is installed on the front surface thereof, and is installed at a position of about 1500 mm from the front surface of the speaker a. The effective value of the sound pressure response measured by the microphone c was recorded as a transmission frequency characteristic on a level recorder or the like. In this state, the change with and without the sound transmitting material b was measured and confirmed as an insertion loss Δ (dB). As a sound source emitted from the speaker a, a continuous sine wave sweep without frequency modulation from 20 Hz to 20 kHz was used as a signal. The sound used here was 20 dB or more in S / N ratio with respect to background noise. The insertion loss was determined by the following formula.
Insertion loss Δ (dB) = frequency response of microphone without sample (dB) −frequency response with sample placed (dB)

  Here, the sound transmissivity is the case where the insertion loss Δ (dB) is within 2 dB in each 1/1 octave band of the center frequency 63 Hz to 8 kHz, or each 1/3 octave band of the center frequency 31.5 Hz to 16 kHz. In the case of 3 dB or less, “good”, in each case within 5 dB or 6 dB, “slightly inferior”, and in the case of exceeding 5 dB or 6 dB, respectively, “inferior”. In addition, since a continuous sine wave sweep was used, evaluation was performed in the 1/1 and 1/3 octave bands.

Measurement method 2
Evaluation of sound permeability at an angle θ = 0 °, 15 ° between the speaker-microphone axis and the normal direction of the sound transmission material is the same as the measurement method 1 except that FM short sound is used as the angle and the sound source. Under the conditions, the following sound transmission materials P to R were used. The results are shown in FIG. The details of the sound-transmitting materials P to R used here are as follows.

P: The sound-transmitting material of Example 1 was used.
Q: An acoustically transmissive material produced by the same method as in Example 1 was used except that the porosity was 74% and the thickness was 1.10 mm.
S: The sound transmitting material of Example 2 was used.
R: An acoustically transmissive material prepared in the same manner as in Example 1 was used except that the porosity was 65% and the thickness was 1.03 mm.

  In addition, about the sample described above as Q and R, the material which stuck and reinforced the metal mesh was used in addition to the sound permeable material.

  As a result of the sound permeability evaluation by the measuring method 2, it was found that the sample P exhibits high sound permeability even when θ = 15 °. That is, it was found that the material of Example 1 shows almost no dependence on the incident angle of sound in sound transmission.

(Implementation test of sound absorbing structure: Comparison of sound absorption coefficient α ₀ of sound absorbing material (GW) with and without sound transmitting material (TTP))
The sample was subjected to a sound absorption test using an acoustically transparent material (Example 4) having a thickness of about 1 mm and glass wool (GW). The results are shown in FIG. Here, the horizontal axis represents frequency (Hz) and the vertical axis represents normal normal incidence sound absorption coefficient α ₀ .
[A] shows the α ₀ measured value of 30 mm thick glass wool (GW) as a single sound transmitting material (TTP) without (1) and with (2).
[B] shows the α ₀ actual measurement value of Tmm without (1 ′) / with (2 ′) TTP of 25 mm thick glass wool (GW) alone. Here, in this structure, an air layer of 5 mm was formed between TTP and GW.
According to these results, the values (2) and (2 ′) in which the sound transmitting material (TTP) of the present invention is arranged on the surface are equal to or higher than those of (1) and (1 ′) of the GW alone. Indicating that it has total sound transmission. Incidentally, (0) is 0.2 or less TTP single alpha _0, available reverberation variable as sites reflective.

(Wind noise reduction test)
A wind noise reduction test was conducted with the system shown in FIG. Here, the wind speed was 2.7 m / s. Here, in the wind noise reduction effect evaluation test, with respect to the microphone output response observed without a windshield, the wind is sent from the blower (FAN) at a position away from the wall to such an extent that the bounce of the wind in the room can be ignored. The response reduction degree S (dB) measured with the windshield made of the sound transmitting material is mounted is obtained for each 1/1 octave band, and this is indicated as wind noise reduction effect ΔS (dBA). did. The results are shown in FIG. Moreover, the wind noise reduction test was similarly conducted on the samples of Examples 1 to 4 and Comparative Examples 1 to 4 using the system shown in (b1). In the evaluation in Table 1, “excellent” was Δ30 dBA or more, “good” was Δ20 dBA or more, and “inferior” was less than Δ20 dBA.

  According to the present invention, since a material having high sound permeability while having self-supporting properties can be obtained, it can be used as a surface member having a sound-absorbing wall structure. As an example of industrial applicability, a windshield for a microphone, a protective grill, an acoustically transmissive projection screen and a speaker are shown.

1: Sound adjustment surface structure 2: Sound transmission material 3: Sound adjustment mechanism 4: Frame 41: Space 42: Support column 421: Fixed surface 6: Interior structure 300: Microphone device 600 for measuring surface sound pressure: Reverberation variable wall 700: Reverberation adjustment wall

Claims (14)

An acoustically transmissive material that is a material in which fibers are entangled with each other, has a Taber stiffness of 5 mN · m or more, a bending resistance of 100 mN or more, a porosity of 60% or more and 95% or less, and a thickness of 3 mm or less. When,
An acoustic adjustment surface structure comprising an acoustic adjustment mechanism having a sound absorbing structure and / or a reflective structure installed on the back surface thereof.   The acoustic adjustment surface structure according to claim 1, wherein the acoustic adjustment mechanism is a variable acoustic adjustment mechanism capable of changing an arrangement ratio of the sound absorbing structure and / or the reflective structure. An acoustically transmissive material in which fibers are entangled with each other, the Taber stiffness is 5 mN · m or more, the bending resistance is 100 mN or more, the porosity is 50% or more, and the thickness is 3 mm or less;
An acoustic adjustment mechanism having a sound-absorbing structure and / or a reflective structure installed on its back surface,
An acoustic adjustment surface structure in the interior of the wall and / or ceiling of the building,
The acoustic adjustment mechanism is a variable acoustic adjustment mechanism capable of changing the arrangement ratio of the sound absorbing structure and / or the reflective structure,
The sound transmitting material is arranged so that a space is formed between the wall surface and / or the ceiling of the building,
The variable acoustic adjustment mechanism has a curtain or a sound-absorbing blind arranged in the space and configured to be openable and closable,
An acoustic adjustment surface structure that adjusts the sound absorption characteristics of the surface by opening and closing the curtain or blind. An acoustically transmissive material in which fibers are entangled with each other, the Taber stiffness is 5 mN · m or more, the bending resistance is 100 mN or more, the porosity is 50% or more, and the thickness is 3 mm or less;
An acoustic adjustment mechanism having a sound-absorbing structure and / or a reflective structure installed on its back surface,
An acoustic adjustment surface structure in the interior of the wall and / or ceiling of the building,
The sound transmitting material is arranged so that a space is formed between the wall surface and / or the ceiling of the building,
The acoustic adjustment mechanism is an acoustic adjustment surface structure having a sound absorbing structure and / or a reflective structure arranged in the space.   The interior structure of a building which has the acoustic adjustment surface structure as described in any one of Claims 1-4. In the windshield for microphones to reduce the wind noise of the microphone,
The windshield has an acoustically transparent material arranged at a position that blocks the wind against the microphone;
The sound transmitting material is a material in which fibers are entangled with each other, the Taber stiffness is 5 mN · m or more, the bending resistance is 100 mN or more, the porosity is 60% or more and 95% or less, and the thickness is 3 mm or less. A windshield for microphones. In the protective grill placed on the front of the microphone or speaker,
The grill is
An acoustically transmissive material that is a material in which fibers are entangled with each other, has a Taber stiffness of 5 mN · m or more, a bending resistance of 100 mN or more, a porosity of 60% or more and 95% or less, and a thickness of 3 mm or less. The protective grille consists of In an acoustically transmissive projection screen that has a front projection type image projection surface and is configured to use a speaker arranged behind the image projection surface to emit sound,
At least the image projection surface is
An acoustically transmissive material that is a material in which fibers are entangled with each other, has a Taber stiffness of 5 mN · m or more, a bending resistance of 100 mN or more, a porosity of 60% or more and 95% or less, and a thickness of 3 mm or less. Sound-transparent projection screen composed of In a speaker box and a speaker having a woofer unit,
An acoustically transmissive material that is a material in which fibers are entangled with each other, has a Taber stiffness of 5 mN · m or more, a bending resistance of 100 mN or more, a porosity of 60% or more and 95% or less, and a thickness of 3 mm or less. ,
A sound-absorbing material made of a porous sound-absorbing material disposed behind the sound-transmitting material; and
A sound absorbing structure having an air layer disposed behind the sound absorbing material is provided in the speaker box,
The speaker according to claim 1, wherein the sound absorbing structure is provided on an inner wall of the speaker box.   The speaker according to claim 9, wherein the speaker is a sealed type. The fibers of the acoustically transparent material are metal fibers;
An acoustic adjustment surface structure according to claims 1 to 4, an interior structure according to claim 5, a windshield for a microphone according to claim 6, a protective grill according to claim 7, an acoustically transmissive projection screen according to claim 8, or a claim. Item 9. The speaker according to item 9-10. The insertion loss of the sound transmitting material is 5 dB or less in each 1/1 octave band of 63 Hz to 8 kHz.
An acoustic adjustment surface structure according to claims 1 to 4, an interior structure according to claim 5, a windshield for a microphone according to claim 6, a protective grill according to claim 7, an acoustically transmissive projection screen according to claim 8, or a claim. Item 9. The speaker according to item 9-10 . The sound transmission material is a material obtained by compression molding metal fibers,
An acoustic adjustment surface structure according to claims 1 to 4, an interior structure according to claim 5, a windshield for a microphone according to claim 6, a protective grill according to claim 7, an acoustically transmissive projection screen according to claim 8, or a claim. Item 9. The speaker according to item 9-10. The fibers of the acoustically transparent material are heat-treated, and the fibers are sintered or fused together.
An acoustic adjustment surface structure according to claims 1 to 4, an interior structure according to claim 5, a windshield for a microphone according to claim 6, a protective grill according to claim 7, an acoustically transmissive projection screen according to claim 8, or a claim. Item 9. The speaker according to item 9-10.