The present invention relates to a sound-permeable member equipped with a waterproof sound-permeable membrane and relates to a method of manufacturing the same.
Since electric products, such as a cellular phone, a notebook PC, an electronic notepad and a digital camera, often are used outdoors, it is desirable for these products to have waterproof performance. The portion difficult to give waterproof performance may be a sound emitting portion, such as a loudspeaker and a buzzer, or may be a sound receiving portion, such as a microphone.
For example, a housing of the cellular phone has an opening in the position corresponding to a microphone or a loudspeaker. A balance between sound permeability and waterproofness can be achieved by closing the opening formed in the housing with a sound-permeable member. The sound-permeable member can be a member equipped with a waterproof sound-permeable membrane that allows gas to pass therethrough and blocks liquid. Examples of the waterproof sound-permeable membrane include a polytetrafluoroethylene (PTFE) porous membrane and an ultrahigh-molecular-weight polyethylene (UHMWPE) porous membrane as disclosed in JP 2815618 B and JP 2004-83811 A.
It is known that the waterproofness of the PTFE porous membrane and the UHMWPE porous membrane becomes higher as those average pore sizes become small. However, when the average pore size becomes small, the area density becomes large and sound permeability will deteriorate. That is, there is a trade-off between sound permeability and waterproofness. Therefore, it is not easy to improve waterproofness without reducing sound permeability.
As a standard for waterproofness of common electrical machineries, “JIS C 0920” provides “Waterproof test for electrical machineries and apparatuses and Degrees of protection against solid foreign objects”. In that standard, the class of waterproofness of electrical machineries and apparatuses is shown by nine levels, protection classes 0 to 8. The protection class 7 (immersion proof) indicates machineries and apparatuses having a performance that admits no trace of water ingress even after it has been immersed in water at a depth of one meter for 30 minutes. Machinery and apparatuses with the protection class 6 (water-resistant) or lower are not designed for immersion in water. Accordingly, waterproofness equivalent to the protection class 7 is required to prevent failure of a product even when the product is accidentally dropped in water.
When trying to achieve such a high waterproofness of a product using a sound-permeable member, problems, such as difficulty to hear a sound, degradation of sound quality (deterioration of acoustic characteristics), and disadvantage in power consumption due to the need to make the default sound volume high, occur inevitably. Such problems contribute to difficulty in the widespread use of products with high waterproof performance.
With the foregoing in mind, an object of the present invention is to improve the sound permeability of a sound-permeable member equipped with a waterproof sound-permeable membrane while maintaining high waterproofness.
The present invention provides a sound-permeable member including:
a waterproof sound-permeable membrane that allows sound to pass therethrough and blocks liquid from passing therethrough; and
a main body having an opening for passing sound, the opening being closed by the waterproof sound-permeable membrane,
wherein the waterproof sound-permeable membrane is fixed to the main body in a slack state.
In another aspect, the present invention provides a sound-permeable member including:
a waterproof sound-permeable membrane that allows sound to pass therethrough and blocks liquid from passing therethrough; and
a main body having an opening for passing sound, the opening being closed by the waterproof sound-permeable membrane,
wherein the waterproof sound-permeable membrane is deformed so that at least a part of the waterproof sound-permeable membrane is spaced apart from a base flat plane including a boundary surface between the waterproof sound-permeable membrane and the main body.
In yet another aspect, the present invention provides a method of manufacturing a sound-permeable member including a waterproof sound-permeable membrane that allows sound to pass therethrough and blocks liquid from passing therethrough and a main body having an opening for passing sound, the opening being closed by the waterproof sound-permeable membrane, the method including the steps of:
cutting the waterproof sound-permeable membrane into a predetermined shape applicable to the opening of the main body;
fixing the waterproof sound-permeable membrane that has been cut to the main body; and
deforming the waterproof sound-permeable membrane in advance before fixing to the main body so that when the waterproof sound-permeable membrane is fixed to the main body, at least a part of the waterproof sound-permeable membrane is spaced apart from a base flat plane including a boundary surface between the waterproof sound-permeable membrane and the main body.
It should be noted that these steps may be performed in no particular order or a plurality of the steps may be performed at the same time.
The present inventors diligently studied the sound permeability of a waterproof sound-permeable membrane. And the inventors found that the sound permeability of the waterproof sound-permeable membrane is affected not only by the physical properties of the waterproof sound-permeable membrane but also by how the membrane is fixed to an object (main body), especially by the presence or absence of slack. A mechanism in which sound passes through the waterproof sound-permeable membrane involves both a mechanism in which sound passes through pores of the waterproof sound-permeable membrane and a mechanism in which sound propagates by vibrating the waterproof sound-permeable membrane. In the case of a waterproof sound-permeable membrane with high waterproofness, the mechanism in which sound propagates by vibrating the waterproof sound-permeable membrane becomes dominant because the pores are very small. This is also apparent from the existence of a correlation between the sound permeability and the area density. When the passage of sound is mainly contributed by the vibration of the waterproof sound-permeable membrane, the excellence of sound permeability depends not only on the physical properties of the waterproof sound-permeable membrane but also on how the waterproof sound-permeable membrane is fixed to the object.
Generally, the waterproof sound-permeable membrane is fixed to an object so that it has almost no slack. If the waterproof sound-permeable membrane is tensioned without slack, resonance will occur in the surface of the waterproof sound-permeable membrane, and the distortion of sound will become large, especially at high frequencies. Since the distortion of sound increases the loss of energy, sound permeability deteriorates. On the other hand, when the waterproof sound-permeable membrane is fixed to the object so that it slackens moderately, the energy loss of sound can be suppressed because the above-mentioned phenomenon hardly occurs. As a result, excellent sound permeability can be achieved. Therefore, the present invention makes it possible to improve sound permeability of a sound-permeable member equipped with a waterproof sound-permeable membrane, while maintaining high waterproofness.
In the manufacturing method of the present invention, the waterproof sound-permeable membrane is deformed in advance before fixing to the main body so that at least a part of the waterproof sound-permeable membrane is spaced apart from the base flat plane including the boundary surface between the waterproof sound-permeable membrane and the main body. Therefore, it becomes possible to efficiently manufacture the sound-permeable member in which the waterproof sound-permeable membrane is fixed to the main body in a slack state. Moreover, other steps, such as a step of fixing the waterproof sound-permeable membrane to the main body, are not affected, and there is almost no possibility that the slack deteriorates waterproofness.
Hereinafter, embodiments of the present invention will be described with reference to the accompanying drawings.
As shown in
As shown in
The waterproof sound-permeable membrane 1 may be attached directly to the openings 6 and 7 of the housing 4. In this case, a part of the housing 4 to which the waterproof sound-permeable membrane 1 is attached constitutes a sound-permeable member of the present invention.
As shown in
The waterproof sound-permeable membrane 1 does not necessarily slacken in a form of simple curvature as shown in
A membrane having gas permeability in both thickness direction and in-plane direction can be used as the waterproof sound-permeable membrane 1. Neither structure nor material of the membrane is particularly limited. Resin porous membranes, such as a PTFE porous membrane and a UHMWPE porous membrane, are preferable as the waterproof sound-permeable membrane 1 because these membranes can ensure sufficient gas permeability with small area and have high capability to prevent foreign matters from entering inside the housing 4. The PTFE porous membrane can be produced by uniaxial stretching or biaxial stretching of a PTFE film. A UHMWPE porous membrane can be produced by performing steps of sintering, casting, extruding, and stretching (dry process or wet process) using ultrahigh-molecular-weight polyethylene (UHMWPE) as a raw material. The average molecular weight of UHMWPE is about 1 million, for example.
The porous membrane is especially preferable as the waterproof sound-permeable membrane 1 for the following reasons. Generally, materials that are called sound-permeable membranes include porous ones and non-porous ones. When using a non-porous membrane that is made of, for example, polyethylene terephthalate or polyimide, a frequency range where the transmission loss is specifically large or small may generate in accordance with its natural frequency, resulting in a tendency for the original sound not to be transmitted precisely. On the other hand, when using a porous membrane, part of the sound passes through pores. Accordingly, a frequency range where the transmission loss is specifically large or small is not likely to be generated compared with using a non-porous membrane, resulting in a tendency for the original sound to be transmitted precisely. Excellent sound permeability and acoustic characteristics can be obtained because of both the above-mentioned feature of the porous membrane and the advantageous effect due to slack in the waterproof sound-permeable membrane 1.
The shape of the waterproof sound-permeable membrane 1 may be circular as shown in
Moreover, the waterproof sound-permeable membrane may be reinforced with a reinforcing member. Specifically, a waterproof sound-permeable membrane 1b including a resin porous membrane 1 and a reinforcing member 2 integrated with the resin porous membrane 1 as shown in
As shown in
The thickness of the waterproof sound-permeable membrane 1 can be adjusted in the range of 2 μm to 1 mm in view of its strength and ease of fixing to the main body 8. The gas permeability of the waterproof sound-permeable membrane 1 is preferably in the range of 0.1 to 500 sec/100 ml when expressed as the Gurley value obtained using the Gurley method specified by JIS P 8117.
The average pore size of the waterproof sound-permeable membrane 1 (a resin porous membrane 1) is controlled by, for example, adjusting the stretching ratio so that it can withstand water pressure properly. It is preferable to control the average pore size of the waterproof sound-permeable membrane 1 so that the membrane achieves the waterproof protection class 7 and achieves the water pressure resistance of 9.8 kPa that is equivalent to a depth of one meter in water. Although depending also on other conditions such as thickness, it becomes easy to obtain sufficient waterproofness when the average pore size measured with a bubble point method is in the range of 0.05 to 1.0 μm. The bubble point method is a measuring method in which the membrane is soaked with liquid and is subjected to air pressurization, and then the pore size is obtained from the pressure at which the liquid is extruded through the pore. Moreover, it is preferable that the waterproof sound-permeable membrane 1 can withstand higher water pressure as long as the sound permeability does not deteriorate severely. For example, it is ideal that the water pressure resistance of the waterproof sound-permeable membrane 1 be 100 kPa or more, because it allows the waterproof protection class 7 to be achieved by a safe margin.
The surface density of the waterproof sound-permeable membrane 1 is controlled so as to obtain good sound permeability. Specifically, it is preferable that the insertion loss of the waterproof sound-permeable membrane 1 be 2 dBA or less in order to keep good sound permeability in the audible range. Such insertion loss can be achieved easily when the area density is 30 g/m2 or less. On the other hand, it is preferable that the lower limit of the area density of the waterproof sound-permeable membrane 1 be, for example, 2 g/m2 from the point of view of ensuring sufficient strength and good processability. In the case of using the waterproof sound-permeable membranes 1b or lc having the reinforcing members 2 or 3, the area density of the whole including the reinforcing members 2 or 3 is preferably in the above-mentioned range.
The method for allowing the waterproof sound-permeable membrane 1 to slacken is not particularly limited. Performing a step of deforming the waterproof sound-permeable membrane 1 in advance before fixing it to the main body 8 makes it possible easily to slacken the waterproof sound-permeable membrane 1 that have been fixed to the main body 8. Furthermore, a method described below makes it possible to perform, at one time, both a step of cutting the waterproof sound-permeable membrane 1 into a predetermined shape applicable to the opening 8p of the main body 8 and a step of deforming the waterproof sound-permeable membrane 1. In order to conduct this method, a punch die (Thomson die) having a configuration shown in
As shown in
Although a general platen has a flat surface without unevenness, the surface 14p of the platen 14 has a bulge of an appropriate height “h” in this embodiment. When the cutter 12 contacts and cuts the waterproof sound-permeable membrane 1 provided on the platen 14, the bulge in the surface 14p of the platen 14 pushes up the waterproof sound-permeable membrane 1, thereby transferring the shape of the bulge in the surface 14p of the platen 14 to the waterproof sound-permeable membrane 1.
Thus, the step of cutting the waterproof sound-permeable membrane 1 and the step of deforming the waterproof sound-permeable membrane 1 can be performed simultaneously by using a die that serves as both a deforming die and a cutting die. Productivity is improved because the number of the steps substantially is reduced by one. Of course, the step of cutting the waterproof sound-permeable membrane 1 and the step of deforming the waterproof sound-permeable membrane 1 may be performed individually and in no particular order.
With the above-mentioned method, the waterproof sound-permeable membrane 1 deformed in advance is provided. Next, a step of fixing the waterproof sound-permeable membrane 1 to the main body 8 is performed as shown in
The waterproof sound-permeable membrane 1 may be provided in the form of an assembly in which a double-stick tape is attached to each of front and rear surfaces of the waterproof sound-permeable membrane 1. As shown in
The separator 32 can be removed from the mounting separator 34 along with the assembly 40. As shown in the plan view of
The separators 32 and 34 may be made of resin, such as polyethylene, polypropylene and polyethylene terephthalate, or may be made of paper. The mounting separator 34 may have an embossed portion on which the assembly 40 is to be mounted. It is preferable that the adhesive strength (180° peel bond strength) between the tabbed separator 32 and the double-stick tape 31 be stronger than the adhesive strength between the mounting separator 34 and the double-stick tape 31. This makes it easier to remove the tabbed separator 32 from the mounting separator 34 along with the assembly 40.
One assembly 40 is equipped with one tabbed separator 32. On the other hand, many assemblies 40 may share the mounting separator 34, or one assembly 40 may be equipped with one mounting separator 34. The latter product is produced by the steps of mounting the tabbed separator 32 on the assembly 40 and punching out the mounting separator 34 larger than the tabbed separator 32.
The shapes of the assembly 40 and the tabbed separator 32 are not particularly limited. The assembly 40 may be circular as shown in
<<Quantification of Slack>>
Quantification of slack in the waterproof sound-permeable membrane 1 can be conducted using a three-dimensional shape measurement system, which is commercially available. The three-dimensional shape measurement system is, for example, a system equipped with a laser displacement sensor that scans a surface of an object with a laser beam and measures the displacement of the object's surface from a base flat plane. The three-dimensional surface shape of the object can be obtained from the displacement measured using the laser displacement sensor.
The slack in the waterproof sound-permeable membrane 1 can be quantified as follows. First, two central lines “VL” and “HL” that pass through the center “O” of the waterproof sound-permeable membrane 1 and cross orthogonally with each other are defined as shown in
R=Dmax/Dm(%) (1)
The base flat plane BF shown in
<<Insertion Loss>>
Although the waterproof sound-permeable membrane 1 has excellent sound permeability, reduction in sound volume and sound distortion are inevitable. A loudness level at a certain frequency is expressed by noise level (unit decibel: dBA). The sound permeability of the waterproof sound-permeable membrane 1 is expressed using insertion loss. The insertion loss is the difference between noise levels before and after a sound passes through the waterproof sound-permeable membrane 1, and is represented by the following formula (2).
Insertion loss(dBA)=|S1−S2| (2)
S1: A noise level (dBA) measured in the absence of the waterproof sound-permeable membrane
S2: A noise level (dBA) measured in the presence of the waterproof sound-permeable membrane
In the formula (2), the insertion loss is expressed by the absolute value of the difference. If a sound attenuates when passing through the waterproof sound-permeable membrane 1, the sound after passing becomes smaller and the insertion loss becomes larger. Moreover, when a sound is distorted due to resonance and the like, the sound after passing may become larger than its original sound at a certain frequency. In any case, when the insertion loss is large, a sound will deviate from its original sound, resulting in difficulty in hearing. When the insertion loss is small, the sound quality will be improved and the output of a loudspeaker can be kept low. Therefore, the amount of the slack in the waterproof sound-permeable membrane 1 preferably is adjusted so that the insertion loss becomes minimal.
The insertion loss can be measured using a measuring system shown in
“Noise level (dBA)” is described in detail as follows. The amount of the pressure change caused by a sound wave that propagates in a fluid is called sound pressure. Human perception of sound is approximately proportional to the logarithm of the sound pressure. Generally, the value “Lp” (unit: dB) defined by the following formula (3) is called the sound pressure level. “p” indicates the sound pressure and “p0” indicates the reference sound pressure (2×5−5 Pa). The loudness perceived by a human listener also is affected by frequency. The sound pressure level that has been subjected to frequency weighting based on human auditory characteristics is called noise level (A-weighted sound pressure level).
L
p=20 log(p/p0) (3)
Hereafter, the present invention will be described more specifically by way of samples that actually were prepared. However, the present invention is not limited by the following examples.
First, a PTFE porous membrane (NTF1026 manufactured by NITTO DENKO CORP.) having a surface on which a nonwoven fabric (a reinforcing member) was laminated was provided as a waterproof sound-permeable membrane that had not been deformed. The characteristics of the waterproof sound-permeable membrane were as follows. Gas permeability was measured using the Gurley method mentioned above. Water pressure resistance was measured according to the water penetration test (high pressure method) specified by JIS L 1092. However, the membrane was deformed largely when following the specified area of JIS L 1092. Therefore, measurement was made while a stainless steel mesh (aperture size: 2 mm) was placed at the opposite side of the pressurized side of the membrane in order to suppress the deformation.
Area density: 9 g/m2
Gas permeability: 10 sec/100 ml
Water pressure resistance: 240 kPa
Next, the waterproof sound-permeable membrane was punched out into circular shape having a diameter of 15 mm using the Thomson die described with
Next, the amounts of slack in Samples 1 to 4 were measured using the method described with
Next, the insertion losses of Samples 1 to 4 were measured using the system described with
Analyzer: Multi-analyzer System Type 3560 (Pulse) made by B&K Precision Corp.
Generator: 4/2-ch Input/Output Module Type 3109 made by B&K Precision Corp.
Microphone: Type 4190 made by B&K Precision Corp.
Conditioning amplifier: Conditioning Amplifier NEXUS made by B&K Precision Corp.
Cellular phone: G′z One W42CA made by CASIO COMPUTER CO., LTD.
The insertion losses of Sample 1 at 3000 Hz and 4000 Hz were small, but its insertion losses at 400 Hz and 800 Hz were large. With respect to Sample 2 and Sample 3, there was no frequency at which the insertion loss was particularly large. All the insertion losses of Sample 2 and Sample 3 were less than 2.0 dBA. Even if the insertion loss is small at a certain frequency, the sound will deviate from its original sound when the insertion loss is large at other frequencies. It is preferable for the improvement of acoustic characteristics that the insertion loss be small throughout the whole audible region. In view of that, Sample 2 and Sample 3 were excellent. On the other hand, the insertion loss of Sample 4 was large on the whole. It is thought that excessive energy will be needed for vibrating the waterproof sound-permeable membrane when the slack is too large, and thus the insertion loss becomes larger.
According to the above results, it is preferable that the maximum value Dmax of the amount of the slack be in the range of 0.2% to 1.0% of the diameter Dm of the waterproof sound-permeable membrane. When deforming the sound-permeable membrane in advance (in other words, designing the platen) so as to meet such a condition, the reduction of the insertion loss can be optimized and thus the waterproof sound-permeable member (housing) having excellent sound permeability and acoustic characteristics can be realized.
Number | Date | Country | Kind |
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2007-263158 | Oct 2007 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/JP2008/068240 | 10/7/2008 | WO | 00 | 4/2/2010 |