JP2010097144A - Sound absorbing body - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a sound absorbing body wherein an excellent sound absorbing effect is obtained in a low frequency region, and a high average sound absorbing rate is achieved and stability for temperature change is good. <P>SOLUTION: The sound absorbing body includes: a frame body 2 including an aperture 2a; and a sound absorbing material 3 which covers the aperture 2a, wherein a thickness T<SB>2</SB>of the frame 2 is 5 to 20 mm, an inner diameter D of the aperture 2a is 70 to 160 mm, a thickness T<SB>1</SB>of the sound absorbing material 3 is 0.5 to 3 mm, a specific gravity G of the sound absorbing material 3 is 0.9 to 1.6, and a storage elasticity modulus E' of the sound absorbing material 3 is 1×10<SP>8</SP>to 1×10<SP>9</SP>Pa. The sound absorbing material 3 is formed by using a polymeric material(X), wherein the polymeric material (X) includes a melting point of 80°C or more, or a glass transfer point of 80°C or more, and it includes a polymeric material (A) in which a peak temperature of tan δat 20 Hz is 15°C or less, and tan δ at 15°C is 0.2 or more, and a polymeric material (B) in which tan δ at 15°C is less than 0.08. <P>COPYRIGHT: (C)2010,JPO&INPIT

Description

  The present invention relates to a sound absorber.

Noise is a familiar problem with vibration, and the demand for sound absorbers is still high. In addition, there are a wide variety of required characteristics depending on the application and purpose, and recently, a material having high sound absorption performance in a low frequency region is desired.
As conventional sound-absorbing materials, for example, porous materials such as glass wool and rock wool-like fibers formed into a cotton-like or board-like shape, and polymer foam-like materials such as polyurethane foam are known. Yes. When sound waves are incident on these porous materials, the sound waves vibrate the air in the gaps in the materials, so some of the vibration energy is converted into heat energy and dissipated by the viscosity of the air itself and the friction with the surroundings. An effect is obtained.

In particular, as a sound absorber capable of obtaining a good sound absorbing effect in a low frequency region of 500 Hz or less, the present inventors previously covered the opening provided in the frame with a sound absorbing material having a specific storage elastic modulus. A sound absorber having a configuration has been proposed (Patent Document 1).
JP 2008-96826 A

The sound absorption characteristics are represented, for example, by a graph with the horizontal axis representing the frequency and the vertical axis representing the sound absorption rate. In order to obtain a sound absorption effect in the low frequency region, the frequency at which the sound absorption rate peaks (peak frequency) is low, and the sound absorption It is preferable that the peak value of the rate is high.
Further, depending on the installation location of the sound absorber, it is required that the peak shape is broad and the frequency range in which good sound absorption occurs is wide. As the index, when the peak frequency is 500 Hz or less, for example, an average sound absorption coefficient representing the average of the sound absorption coefficient in the range of the peak frequency ± 50 Hz can be used. When the peak value of the sound absorption coefficient is the same, a higher average sound absorption coefficient indicates that the peak shape is broader.
Moreover, since the peak frequency may fluctuate greatly due to fluctuations in the physical properties of the sound absorbing material due to temperature changes, stability against temperature changes is also required depending on the installation location.

  The present invention has been made in view of the above circumstances, and provides a sound absorber that can achieve a good sound absorption effect in a low frequency region, can achieve a high average sound absorption coefficient, and also has good stability against temperature change. Objective.

[1] The sound absorber of the present invention includes a frame having an opening, and a sound absorbing material that covers the opening,
The frame thickness _{T 2} is 5 to 20 mm, an inner diameter D of the opening 70～160Mm, the thickness _{T 1} of the said sound absorbing material is 0.5 to 3 mm, a specific gravity G of the sound absorbing material 0.9. 6. The storage elastic modulus E ′ of the sound absorbing material is 1 × 10 ⁸ to 1 × 10 ⁹ Pa, the sound absorbing material is formed using a polymer material (X), and the polymer material (X) Has a melting point of 80 ° C. or higher or a glass transition point of 80 ° C. or higher, and the polymeric material (X) has a tan δ peak temperature at 20 Hz of 15 ° C. or lower and a tan δ at 20 Hz of 15 ° C. of 0.1. The polymer material (A) is 2 or more and the polymer material (B) whose tan δ at 20 Hz and 15 ° C. is less than 0.08.

[2] In the above [1], when the entire polymer material contained in the sound absorbing material is 100 mass%, the content of the polymer material (A) is 5 to 75 mass%, and the polymer material ( The content of B) is preferably 25 to 95% by mass.
[3] It is preferable that tan δ at 20 Hz and 15 ° C. of the sound absorbing material is 0.07 or more.

  ADVANTAGE OF THE INVENTION According to this invention, while being able to acquire a favorable sound absorption effect in a low frequency area | region, a high average sound absorption rate can be achieved and the stability with respect to a temperature change can also be obtained.

The value of the storage elastic modulus (E ′) in the present invention is a measurement method according to JIS K7244-4 (tensile vibration). The sample size is 40 mm in length, 10 mm in width, and 1 mm in thickness. , A value (unit: Pa) obtained as a distortion amplitude of 6 μm and a measurement frequency of 20 Hz. The measurement temperature is 25 ° C. unless otherwise specified.
Tan δ (loss tangent) is a value represented by the absolute value of the ratio (E ″ / E ′) of the loss elastic modulus (E ″) to the storage elastic modulus (E ′).
The tan δ (loss tangent) of the sound absorbing material and the polymer material in the present invention is a value at 20 Hz and 15 ° C. unless otherwise specified. The storage elastic modulus (E ′) and the measurement frequency of tan δ are generally 20 Hz because they are closer to the actual sound absorption frequency within the measurable range (0.2 to 50 Hz) (in addition, at 50 Hz, 20 Hz because of the large variation in data.) In addition, the viscoelastic property at normal temperature (25 ° C.) in the low frequency region (about 250 to 400 Hz) is similar to the viscoelastic property at 15 ° C. at 20 Hz when estimated based on the master curve. 15 ° C. was adopted.
The peak value and peak temperature of tan δ of the polymer material (A) in the present invention are the peak value and peak obtained when tan δ is measured while changing the temperature at a measurement frequency of 20 Hz and a measurement temperature of −30 to 30 ° C. It is the temperature (peak temperature) showing the value.
The storage elastic modulus (E ′) and tan δ (loss tangent) are values determined by the material.
The storage elastic modulus (E ′) and tan δ (loss tangent) were measured using a viscoelastic spectrometer EXSTAR6000 DMS, model name DMS6100, manufactured by SII Nanotechnology.

The sound absorption coefficient in this specification means “normal incidence sound absorption coefficient”, and is a value measured by setting a sample in an impedance tube having a diameter of 100 mm by a method according to JIS A 1405-2. The sample diameter is a little less than 100 mm, and it is fixed in the impedance tube through a spacer. Changing the back air layer thickness (ie, frame thickness T ₂ ) can be done by adjusting the position of the rigid body (piston) behind the sample. The sample diameter (that is, the inner diameter D of the opening of the frame) can be changed by adjusting the inner diameter of the spacer.
The sound absorption rate is measured while changing the incident frequency, and the frequency at which the sound absorption rate becomes the highest is called the peak frequency.
Further, since the sound absorption by the sound absorber of the present invention is a membrane vibration type sound absorption, the sound absorption is performed at a resonating frequency. Therefore, an average of the sound absorption rate in the range of the peak frequency ± 50 Hz is defined as a value that serves as an index of the range of the frequency range where good sound absorption occurs, and is defined as the average sound absorption rate.

The melting point of the polymer material in the present invention is measured under the conditions of a heating rate of 10 ° C./min, a measurement start temperature of −50 ° C., and a measurement end temperature of 200 ° C. according to the differential scanning calorimetry (DSC) method applied to JIS K 7121. This is the value obtained.
Further, the glass transition point (hereinafter sometimes referred to as Tg) of the polymer material has a measurement frequency of 20 Hz and a measurement temperature of −50 ° C. to 200 ° C. according to a measurement method based on JIS K 7244-3 (tensile vibration). This is a value obtained from the temperature indicating the peak value obtained when tan δ (loss tangent) is measured while increasing the temperature at 2 ° C./min.
When the polymer material has two or more glass transition points, if the at least one glass transition point is 80 ° C. or higher, “has a glass transition point of 80 ° C. or higher”.

1A and 1B show an embodiment of a sound absorber according to the present invention. FIG. 1A is a plan view, and FIG. 1B is a cross-sectional view taken along line BB in FIG. In the figure, reference numeral 1 denotes a sound absorbing body, 2 denotes a frame body, 3 denotes a sound absorbing material, and 4 denotes a construction surface to which the sound absorbing body is attached. The frame body 2 has a through hole that communicates the front surface and the back surface, and an opening 2a is formed on each of the front surface and the back surface. The end surface 2b on the surface side of the frame 2 is a flat surface. The sound absorbing material 3 is laminated and fixed on the end surface 2b on the surface side so as to cover the opening 2a.
The end surface 2c on the back surface side of the frame 2 is also a flat surface. The end surface 2 c on the back surface side is bonded and fixed to the construction surface 4. That is, the opening 2 a on the back side is closed by the construction surface 4, and a back air layer 5 is formed between the sound absorbing material 3 and the construction surface 4.

The frame body 2 of the present embodiment has a circular outer shape and has concentric through holes. The frame body 2 may have any configuration as long as it has an opening 2a on the surface side and a back air layer 5 is formed continuously from the opening 2a. In the present embodiment, the frame body 2 itself may or may not have sound absorption performance. The material of the frame 2 is not particularly limited, but a material having a low specific gravity such as a resin is preferable from the viewpoint of weight reduction.
The thickness T ₂ of the frame body 2 determines the thickness of the back air layer 5 formed on the construction surface 4 side of the sound absorbing material 3. The thickness _{T 2} of the frame 2 in the present invention is 5 to 20 mm, preferably 6 to 15 mm. When the thickness is 5 mm or more, good primary vibration of the sound absorbing material is easily obtained. When it is 20 mm or less, it is easy to realize a reduction in size and weight.
When the thickness of the frame 2 is not uniform in the opening 2a uses the average value as T _2.

The shape of the opening 2a on the surface side of the frame body 2 (the shape of the opening on the end surface 2b on the surface side) is not limited to a circle but may be an arbitrary shape such as a polygon.
In the present invention, the inner diameter D of the opening 2a is 70 to 160 mm, preferably 80 to 135 mm, more preferably 90 to 110 mm. When it is 70 mm or more, the peak frequency tends to be low, and when it is 160 mm or less, it is preferable in terms of miniaturization. When the opening 2a is smaller, the number of openings 2a that can be provided in a certain area is increased, and the sound absorption performance in the certain area is improved.
In the present invention, when the opening 2a is not circular, the value of the inner diameter D of the opening 2a is the diameter of a circle having the same area as the area of the opening 2a.
When the opening 2a is a square, the length of one side is preferably 62 to 142 mm, more preferably 70 to 120 mm, and still more preferably 80 to 97 mm.

The sound absorbing material 3 varies in specific gravity G, storage elastic modulus E ′ and tan δ depending on the material.
In the present invention, the specific gravity G of the sound absorbing material 3 is 0.9 to 1.6, preferably 1.0 to 1.4. When the specific gravity G is 0.9 or more, it is easy to obtain a good sound absorption effect in the low frequency region. It is preferable from the point of weight reduction that it is 1.6 or less.
In the present invention, the storage elastic modulus E ′ of the sound absorbing material 3 is 1 × 10 ⁸ to 1 × 10 ⁹ Pa, and preferably 1 × 10 ^{8 to} 5 × 10 ⁸ .
When the storage elastic modulus E ′ is 1 × 10 ⁸ Pa or more, it is easy to obtain a good primary vibration of the sound absorbing material, and a good sound absorbing effect in a low frequency region is easily obtained. If it is 1 × 10 ⁹ Pa or less, the peak frequency tends to be low.
In the present invention, the tan δ of the sound absorbing material 3 is preferably 0.07 or more. If it is 0.07 or more, the average sound absorption coefficient is remarkably improved. The upper limit of tan δ is not particularly limited, but is preferably 0.3 or less in order to satisfy a preferable range of other parameters.

[Polymer material (X)]
The sound absorbing material 3 is formed using a polymer material (X). Preferably, it is formed using a polymer material (X) and a filler. For example, the sound absorbing material 3 is made of a mixture of a polymer material (X) and a filler. The polymer material (X) may be a combination of two or more polymer materials.
The polymer material (X) has a melting point of 80 ° C. or higher or a glass transition point of 80 ° C. or higher.
The temperature below 80 ° C. assumes the normal operating temperature of the sound absorber. A polymer material having a melting point or glass transition point higher than the operating temperature range has a crystal structure or a glassy substance in the operating temperature range, and is excellent in heat resistance. A sound absorbing material made of a material that has neither a crystal structure nor a glassy substance at the operating temperature is prone to deformation due to its own weight, and this deformation greatly changes the sound absorption characteristics (mainly largely shifted to the high frequency side). It is not preferable because there is a risk of

The polymer material (X) has a tan δ peak temperature at 20 Hz of 15 ° C. or lower and a tan δ at 20 Hz and 15 ° C. of 0.2 or higher, and a tan δ at 20 Hz and 15 ° C. of 0. Polymer material (B) which is less than 0.08.
Here, the polymer material in the present invention is preferably a material composed only of the target polymer compound, but when obtained from a commercial product, the target polymer compound is the main component and other additives are included. It may be a composition. In the case of a composition, the physical property value and molecular structure in the state of the composition are regarded as the physical property value and molecular structure of the polymer material.
The blending when preparing the polymer material (X) is preferably such that the tan δ of the sound absorbing material 3 to be obtained is 0.07 or more.

[Polymer material (A)]
The peak temperature of tan δ at 20 Hz of the polymer material (A) is 15 ° C. or lower, and preferably −30 ° C. to 15 ° C. The tan δ at 20 Hz and 15 ° C. of the polymer material (A) is 0.2 or more, preferably 0.4 to 1.5.
As described above, by using the polymer material (A) having a low tan δ peak temperature and a high tan δ at 20 Hz and 15 ° C., the temperature stability near normal temperature is improved and a high average sound absorption coefficient is obtained.
The polymer material (A) is preferably a styrene isoprene styrene block copolymer or a hydrogenated product thereof (hereinafter collectively referred to as SIS). Various grades of SIS are commercially available, and those having a tan δ peak temperature at 20 Hz of 15 ° C. or lower and a tan δ value at 20 Hz of 15 ° C. of 0.2 or higher are selected and used. it can. For example, a high blur 5125, a high blur 7125, a high blur 7311 (all of which are product names, manufactured by Kuraray Co., Ltd.) can be used. The polymer material (A) may be used alone or in combination of two or more.

[Polymer material (B)]
The polymer material (B) is a polymer material having a tan δ of less than 0.08. Specific examples of the polymer material (B) include PE (polyethylene) such as LLDPE (linear low density polyethylene), HDPE (high density polyethylene), and LDPE (low density polyethylene); PP (polypropylene), PS (polystyrene). ), PC (polycarbonate), PET (polyethylene terephthalate), polylactic acid, EBR (ethylene butene copolymer), EOR (ethylene, octene copolymer), and other ethylene-α olefin copolymers.
The polymer material (B) may be one type or two or more types.

Since the polymer material (X) has a melting point of 80 ° C. or higher or a glass transition point of 80 ° C. or higher, at least a part of the polymer material (B) has a melting point of 80 ° C. or higher or a glass transition point of 80 ° C. or higher. Those having the following are preferred.
For example, a crystalline polymer having a melting point of 80 ° C. or higher (LLDPE, HDPE, LDPE, PP), or an amorphous polymer having a glass transition temperature (Tg) of 80 ° C. or higher ( PS, PC, PET, polylactic acid, etc.) are preferably used.
For example, vinyl chloride resin (PVC) has a glass transition temperature higher than 80 ° C., but commercially available soft PVC contains a plasticizer and has a glass transition temperature lower than 80 ° C.

When the total amount of the polymer material (X) contained in the sound absorbing material 3 is 100% by mass, the content of the polymer material (A) is 5 to 75% by mass, and the content of the polymer material (B) is 25 to 25%. It is preferably 95% by mass. Within this range, good temperature stability and a high average sound absorption rate can be easily obtained.
More preferable ranges of the content are 5 to 50% by mass of the polymer material (A), 50 to 95% by mass of the polymer material (B), and more preferably 7 to 40% of the polymer material (A). The mass% and the polymer material (B) are 60 to 93 mass%.

[Filler]
An inorganic filler and / or an organic filler can be used as the filler.
Examples of the inorganic filler include mica, talc, calcium carbonate, magnesium hydroxide, barium sulfate and the like.
When the inorganic filler is blended, the blending amount is not particularly limited as long as the specific gravity G, storage elastic modulus E ′, and tan δ of the sound-absorbing material can be obtained in good ranges. From the point of mechanical strength, 80 mass% or less is preferable in the constituent material of the sound-absorbing material 3, and 60 mass% or less is more preferable.
Examples of organic fillers include 3,3 ′, 3 ″, 5,5 ′, 5 ″ -hexa-tert-butyl-a, a ′, a ″-(mesitylene-2,4,6-triyl ) Tri-p-cresol (for example, product name: ADK STAB AO-330, manufactured by ADEKA), tris (2,4 di-tert-butylphenyl) phosphite (for example, product name: Irg168, Ciba Specialty Chemicals) Product).
When the organic filler is blended, the blending amount is not particularly limited as long as the specific gravity G, the storage elastic modulus E ′, and the tan δ of the sound absorbing material can be obtained within a preferable range. From the viewpoint of mechanical strength, 50% by mass or less is preferable in the constituent material of the sound absorbing material 3, and 30% by mass or less is more preferable.

In the present invention, the thickness T ₁ of the sound absorbing material 3 is 0.5 to 3 mm, and preferably 0.6 to 2 mm. When the thickness is 0.5 mm or more, good primary vibration of the sound absorbing material is easily obtained. It is preferable from the point of weight reduction that it is 3 mm or less.
If the thickness of the sound absorbing material 3 is not uniform, using an average value as T _1.

  As a means for fixing the sound absorbing material 3 to the frame body 2, an adhesive means such as an adhesive or a double-sided tape may be used, and it may be fixed by pressure bonding or melt pressure bonding.

  Further, another sound absorbing layer (not shown) may be laminated on the surface of the sound absorbing material 3 (on the side opposite to the frame 2 side). The material of the other sound absorbing layer is not particularly limited, and a known material can be appropriately used as a conventional sound absorbing material. For example, a sound absorbing effect can be obtained as a whole of the sound absorber 1 by providing a sound absorbing layer on the sound absorbing material 3 so as to have a sound absorbing effect in a higher frequency region than in a frequency region where the sound absorbing effect can be obtained by the sound absorbing material 3. The frequency region can be made wider. Examples of the material of the other sound absorbing layer include foamed resin, felt, fiber material, glass wool, rock wool, and wood powder cement. Particularly preferred are foamed resin, felt, fiber material, and glass wool.

  According to the sound absorber 1, it is small and light, the peak frequency of the sound absorption rate is 500 Hz or less, preferably 450 Hz or less, the sound absorption rate (peak value) at the peak frequency is 0.5 or more, and the average sound absorption rate A sound absorber having a high sound absorption effect in a low frequency region such that is not less than 0.4, preferably 0.45 or more, and excellent in stability against temperature change can be obtained.

Note that the sound absorber of the present invention is not limited to the form shown in FIG. 1 and may have various configurations as long as the structure includes a frame having an opening and a sound absorbing material that covers the opening. . For example, as shown in FIG. 2, a plurality of openings 22 a are provided in the plate-like frame 22, and a sound absorbing material is provided on one surface of the frame 22 so as to cover the plurality of openings 22 a collectively. The sound absorber 21 may have a configuration in which 23 is stacked and fixed. FIG. 2 is a perspective view of the sound absorber 21 as viewed from the frame body 22 side.
Thus, when the frame body 22 is provided with a plurality of openings 22a, the shapes and sizes of the plurality of openings 22a may be uniform or different.
Moreover, although arrangement | positioning of this some opening part 22a is arbitrary, the efficiency of the sound absorption in the sound-absorbing body 21 becomes high, so that the distance d of the adjacent opening parts 22a is small.
Similarly, the sound absorber 21 having such a configuration is also small and light, has a high sound absorption effect in a low frequency region, has a high average sound absorption coefficient, and has good stability against temperature change. .

Hereinafter, the present invention will be described in more detail with reference to examples, but the present invention is not limited to these examples.
(Examples 1-5)
Using a film material (mixture of polymer material and filler) having the composition shown in Table 1, a film-like sound absorbing material 3 was produced.
Examples 1 to 3 are examples, Example 4 is a comparative example using SIS having a high peak temperature instead of the polymer material (A), and Example 5 is a comparative example not containing the polymer material (A). In Examples 1 to 4, when the total of the polymer material (X) contained in the sound absorbing material, that is, the total of the polymer material (A) and the polymer material (B) is 100% by mass, the polymer material (A) The total content of the polymer material (B) is 85.7% by mass. The melting point of the polymer material (X) was measured by the method described above. As the DSC apparatus, DSC Q1000 manufactured by TA Instruments Japan Co., Ltd. was used.
The thickness T ₁ of the sound absorbing material 3 was set to the values shown in Table 1. Table 1 shows the specific gravity of the material constituting the sound absorbing material 3. About the obtained sound-absorbing material, the storage elastic modulus E ′ (20 Hz) at 0 ° C., 25 ° C. and 30 ° C., and the sound absorption characteristics were measured by the measurement method described above. The thickness of the frame (T ₂ ) was 10 mm, and the inner diameter (D) of the opening was 90 mm. Table 1 shows the measurement results. In the column of storage elastic modulus E ′, “3E + 08” represents “3 × 10 ⁸ ”.
The column of “0 ° C./30° C.” for the storage elastic modulus E ′ in the table is the relative value of the storage elastic modulus E ′ at 0 ° C. when the storage elastic modulus E ′ at 30 ° C. is 1.

The materials used are as follows.
[Polymer material (A)]
SIS (1): Hibler 5125 (product name, manufactured by Kuraray Co., Ltd.). tan δ peak temperature: 3 ° C., tan δ (20 Hz, 15 ° C.): 0.76.
SIS (2): Hibler 7125 (product name, manufactured by Kuraray Co., Ltd.) tan δ peak temperature: 7 ° C., tan δ (20 Hz, 15 ° C.): 1.10.
SIS (3): Hiblar 7311 (product name, manufactured by Kuraray Co., Ltd.). tan δ peak temperature: −5 ° C., tan δ (20 Hz, 15 ° C.): 0.42.
[Comparative polymer material]
-SIS (4): Hibler 5127 (product name, manufactured by Kuraray Co., Ltd.). tan δ peak temperature: 28 ° C., tan δ (20 Hz, 15 ° C.): 0.36.
[Polymer material (B)]
PP: Japan BC8 (product name, manufactured by Nippon Polypro Co., Ltd.) tan δ (15 ° C., 20 Hz) 0.03, melting point 164 ° C.
EBR: ENR7270 (product name, manufactured by Dow Chemical Japan). tan δ (15 ° C., 20 Hz) 0.07.
-LLDPE: UF240 (product name, manufactured by Nippon Polyethylene). tan δ (15 ° C., 20 Hz) 0.03, melting point 124 ° C.
[Filler]
Barium sulfate: Barium sulfate BA (product name, manufactured by Sakai Chemical Co., Ltd.), specific gravity 4.5.

As shown in Table 1, the peak frequencies of Examples 1 to 5 are all 400 Hz or less, and there is a sound absorbing effect in the low frequency region. In Examples 1 to 3 using the polymer material (A) and the polymer material (B), the average sound absorption coefficient is as high as 0.44 or more, the peak shape is broad, and the frequency range in which good sound absorption occurs is wide. Recognize.
On the other hand, instead of the polymer material (A), Example 4 using SIS (4) having a high peak temperature of tan δ of 28 ° C. shows that the storage elastic modulus E ′ at 0 ° C. is the storage elastic modulus at 30 ° C. The value was 2.6 times that of E ′. If the structure of the sound absorbing body is the same, the sound absorbing frequency is determined by the storage elastic modulus E ′. Therefore, if the sound absorbing frequency fluctuates 2.6 times, the sound absorbing frequency fluctuates greatly.
In Example 5, since the polymer material (A) is not used, “0 ° C./30° C.” of the storage elastic modulus E ′ is small, but the average sound absorption coefficient is low.

An embodiment of the sound absorber of the present invention is shown, in which (a) is a plan view and (b) is a cross-sectional view taken along the line BB in (a). It is a perspective view which shows other embodiment of the sound-absorbing body of this invention.

Explanation of symbols

1, 21 ... Sound absorber,
2, 22 ... Frame,
2a, 22a ... opening,
3, 23 ... Sound absorbing material,
5 ... Back air layer.

Claims (3)

A frame having an opening and a sound absorbing material covering the opening;
The frame thickness _{T 2} is 5 to 20 mm, an inner diameter D of the opening 70～160Mm, the thickness _{T 1} of the said sound absorbing material is 0.5 to 3 mm, a specific gravity G of the sound absorbing material 0.9. 6. The storage elastic modulus E ′ of the sound absorbing material is 1 × 10 ⁸ to 1 × 10 ⁹ Pa, the sound absorbing material is formed using a polymer material (X), and the polymer material (X) Has a melting point of 80 ° C. or higher or a glass transition point of 80 ° C. or higher, and the polymeric material (X) has a tan δ peak temperature at 20 Hz of 15 ° C. or lower and a tan δ at 20 Hz of 15 ° C. of 0.1. A sound absorber comprising a polymer material (A) of 2 or more and a polymer material (B) having a tan δ of less than 0.08 at 20 Hz and 15 ° C.   When the entire polymer material contained in the sound absorbing material is 100% by mass, the content of the polymer material (A) is 5 to 75% by mass, and the content of the polymer material (B) is 25 to 95%. The sound absorber according to claim 1, wherein the sound absorber is mass%.   3. The sound absorber according to claim 1, wherein tan δ at 20 Hz and 15 ° C. of the sound absorbing material is 0.07 or more.

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