WO2007091513A1 - スピーカ - Google Patents
スピーカ Download PDFInfo
- Publication number
- WO2007091513A1 WO2007091513A1 PCT/JP2007/051908 JP2007051908W WO2007091513A1 WO 2007091513 A1 WO2007091513 A1 WO 2007091513A1 JP 2007051908 W JP2007051908 W JP 2007051908W WO 2007091513 A1 WO2007091513 A1 WO 2007091513A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- edge
- elastic modulus
- diaphragm
- frame
- damper
- Prior art date
Links
Classifications
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- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
- H04R9/00—Transducers of moving-coil, moving-strip, or moving-wire type
- H04R9/02—Details
- H04R9/04—Construction, mounting, or centering of coil
- H04R9/041—Centering
- H04R9/043—Inner suspension or damper, e.g. spider
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
- H04R7/00—Diaphragms for electromechanical transducers; Cones
- H04R7/16—Mounting or tensioning of diaphragms or cones
- H04R7/18—Mounting or tensioning of diaphragms or cones at the periphery
- H04R7/20—Securing diaphragm or cone resiliently to support by flexible material, springs, cords, or strands
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
- H04R9/00—Transducers of moving-coil, moving-strip, or moving-wire type
- H04R9/06—Loudspeakers
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
- H04R2400/00—Loudspeakers
- H04R2400/07—Suspension between moving magnetic core and housing
Definitions
- the present invention relates to a speaker.
- the conventional speaker is arranged such that the diaphragm 3A and the gap in the magnetic circuit 1A can freely move in amplitude, and is connected to the inner peripheral end of the diaphragm 3A.
- Body 2A, frame 5A connected to the outer peripheral edge of diaphragm 3A via edge 4A, suspension holder 6A disposed on the back surface of diaphragm 3A, and edge connecting suspension holder 6A and frame 5A The structure has 7A.
- the edge 4A and the edge 7A project in opposite directions, the vertical amplitude of the diaphragm 3A is made up and down symmetrically to reduce distortion in the speaker.
- Patent Document 1 is known as prior art document information related to the invention of this application.
- the speaker shown in FIG. 8 uses the suspension holder 6A that supports the diaphragm 3A with force, the mass increases. For low sounds that add high output, the mass itself is rarely a problem, but for medium and high sounds, the problem is that the drive efficiency decreases due to the increase in mass.
- Patent Document 1 Japanese Patent Publication No. 2004-7332
- a speaker includes a frame, a magnetic circuit supported by the frame, a voice coil body arranged so as to freely swing with respect to a magnetic gap provided in the magnetic circuit, and an outer periphery.
- the diaphragm is connected to the frame via the first edge, the inner periphery is connected to the voice coil body, and the diaphragm is provided on the magnetic circuit side.
- the inner periphery is connected to the voice coil body.
- a second edge connecting the outer periphery of the damper to the frame, and the second edge is structured to protrude to the diaphragm side or the opposite side.
- the edge is a speaker in which a third edge having a protruding structure opposite to the protruding direction of the second edge is coupled to the edge.
- FIG. 1 is a cross-sectional view of a speaker according to an embodiment of the present invention.
- FIG. 2 is an enlarged cross-sectional view of the main part of the speaker in one embodiment of the present invention.
- FIG. 3 is a cross-sectional view of a speaker according to another embodiment of the present invention.
- FIG. 4 is a cross-sectional view of a speaker in still another embodiment of the present invention.
- FIG. 5 is a cross-sectional view of a speaker in still another embodiment of the present invention.
- FIG. 6 is a partial cross-sectional view of the coupling edge and its periphery in the speaker of one embodiment of the present invention.
- FIG. 7 is a partial cross-sectional view of a coupling edge and its periphery in a speaker according to another embodiment of the present invention.
- FIG. 8 is a cross-sectional view of a conventional speaker.
- FIG. 1 is a cross-sectional view showing a speaker of the present invention.
- the magnetic circuit 1 arranged in the center of the bottom of the bowl-shaped frame 5 includes a disk-shaped magnet la, a disk-shaped plate lb, and a cylindrical It is formed by combining and adhering together lc.
- a cylindrical magnetic gap 8 opened toward the upper surface side in the magnetic circuit 1 is formed between the inner peripheral side surface of the side wall portion of the yoke lc and the outer peripheral side surface of the plate lb.
- the voice coil body 2 has a structure in which a coil 2b is wound around an outer peripheral portion of a cylindrical main body 2a.
- the voice coil body 2 arranged so as to be movable in the vertical direction with respect to the magnetic gap 8 2 The sound is reproduced by vibrating the thin plate-like diaphragm 3.
- a dust cap 9 is provided at the upper end portion of the voice coil body 2 as a dust-proof measure.
- Diaphragm 3 is a sound source of a speaker, and is made mainly of pulp and rosin that have both high rigidity and appropriate internal loss.
- the outer peripheral end portion of the diaphragm 3 is connected to the open end portion of the frame 5 via a first edge 4 (hereinafter referred to as edge 4) protruding upward, and the inner peripheral end portion of the diaphragm 3 is a voice.
- the coil body 2 is fixed to the outer peripheral side of the main body 2a.
- the edge 4 is formed of a material such as foamed resin, SBR rubber, or cloth so as not to apply a dynamic load to the diaphragm 3. Examples of the foamed resin include foamed urethane resin and foamed rubber.
- the inner peripheral end portion of the damper 10 is on the outer peripheral side of the main body 2a of the voice coil body 2 and on the magnetic circuit 1 side than the portion on which the diaphragm 3 is fixed. Connected to. That is, in FIG. 1, the damper 10 is connected to the lower side of the position where the diaphragm 3 is fixed.
- the outer peripheral end portion of the damper 10 is connected to the frame 5 via a second edge 11a (hereinafter referred to as the edge 11a) separate from the damper 10.
- the damper 10 has a ring-shaped corrugated plate structure, and expands and contracts in accordance with the movement of the voice coil body 2.
- the diaphragm 3 is made of a material such as urethane foam, foam rubber, SBR rubber or cloth so as not to apply a large dynamic load.
- the edge 11a may have a structure that protrudes in either the frame side (that is, the lower side) or the diaphragm 3 side (that is, the upper side). However, edge 11a protrudes in the opposite direction to edge 4.
- the edge 4 has a semicircular cross section that protrudes upward as shown in FIG. 1. Therefore, the edge 11a protrudes downward, that is, toward the frame 5, and has a semicircular cross section.
- edge 11a protrudes from the edge 11a.
- a third edge l ib (hereinafter referred to as edge l ib) having a protruding structure in the direction opposite to the direction is joined.
- This edge 1 lb is also formed of a material such as foamed resin, SBR rubber or cloth so as not to apply a large dynamic load to the diaphragm 3.
- the foamed resin include foamed urethane resin and foamed rubber.
- the edge 11a has a semicircular cross section projecting downward as shown in FIG. 1. Therefore, the edge l ib has a semicircular cross section projecting upward on the opposite side.
- the elastic modulus of each of the first edge 4, the second edge 11a, and the third edge l ib is preferably in the following relationship. That is, the elastic modulus of the first edge 4 is made the smallest, the elastic modulus of the second edge 11a is made the largest, and the elastic modulus of the third edge l ib is made to be the elastic modulus of the first edge 4.
- the middle of the second edge 1 la elastic modulus The reason for this setting will be described in detail later.
- the edge becomes softer as the elastic modulus decreases, and the edge becomes harder as the elastic modulus increases.
- the speaker of the present embodiment when an audio signal is applied to the coil 2 b of the voice coil body 2, it reacts with the magnetic field of the magnetic gap 8, and the voice coil body 2 moves up and down.
- the diaphragm 3 vibrates and generates sound.
- the edge l ib in addition to the edge 11a at the outer peripheral end portion of the damper 10, the distortion of the speaker is suppressed and the driving efficiency of the sound force is increased.
- the damper 10 has its inner peripheral end connected to the voice coil body 2 and its outer peripheral end connected to the frame 5, thereby suppressing rolling during movement of the voice coil body 2. . Therefore, the damper 10 has a ring-like corrugated structure so as to easily follow the movement of the voice coil body 2 and has elasticity.
- the outer peripheral portion of the damper 10 is connected to the frame 5 via the edges 11a and ib.
- the movable width of the voice coil body 2 is increased, and stress is applied to the edges 11a and l ib when the damper 10 becomes a load.
- the cross-sectional shape of the edges 11a and l ib is elastically deformed with a substantially circular state force.
- Etsu 11a, l ib can be elastically deformed, so when the amount of amplitude of the voice coil body 2 becomes large, the presence of the damper 10 makes it difficult for the amplitude to be inhibited, and distortion of the speaker is suppressed. A decrease in drive efficiency is also suppressed at the same time.
- the voice coil body 2 is supported in the vertical direction by two supports. That is, the first support is composed of the diaphragm 3 and the edge 4, and the second support is a combined body composed of the damper 10, the edge 11a, and the rib.
- the thickness of edge 4 is reduced to reduce its weight, thereby reducing the weight of diaphragm 3 and edge 4, thereby increasing the driving efficiency of diaphragm 3.
- edge 4 If the edge 4 is made thinner, the support strength of the voice coil body 2 decreases. In order to compensate for the decrease, the edges 11a and l ib are made thicker than the edge 4, thereby preventing the support strength of the voice coil body 2 from being lowered. As a result, the elastic modulus of the joined body composed of the damper 10, the edge 11a, and the rib is larger than the elastic modulus of the edge 4, that is, is harder.
- the support of the voice coil body 2 is predominantly supported by the second support body, which is a combined force of the damper 10, the edge 11a and the rib ib. Therefore, in order to suppress the upward and downward distortion of the diaphragm 3, it is necessary to make the vertical loads in the combined body composed of the damper 10, the edge 11a and the rib ib as much as possible.
- edge 11a in the embodiment shown in Fig. 2 has a shape protruding toward the frame side (downward) with respect to the diaphragm 3, the edge in Fig. 2 is deformed in the lower side in Fig. 2 and is immediately upside down, that is, In the direction of the diaphragm 3, it is deformed.
- edge 1 lb a third edge 1 lb (hereinafter referred to as edge 1 lb) is provided to absorb the difference in the vertical deformation of the edge 11a.
- the damper 10 has a ring-shaped corrugated plate structure, and includes a first protrusion 10a protruding toward the diaphragm 3 side and a second protrusion protruding in the opposite direction to the first protrusion 10a.
- Each of the protrusions 10b has a structure having a plurality of protrusions 10b. Basically, the loads in the vertical direction can be made substantially the same.
- edge 11a protrudes only downward, it is easily deformed downward. Yes. Therefore, in the present embodiment, in order to absorb the difference between the upper and lower loads at the edge 11a, an edge 1 lb joined to the edge 1la is provided.
- the edge l ib in the present embodiment is shaped to protrude upward, that is, to the diaphragm 3 side. For this reason, the edge l ib itself is deformed upward in FIG. 2 and is hardly deformed downward. For this reason, if these edges 11a and l ib are combined together so as to have a substantially circular cross section, the magnitudes of the vertical loads of the integrally formed edges 11a and 11b can be made substantially equal.
- the elastic modulus of the third edge l ib is slightly smaller than the elastic modulus of the second edge 11a.
- the edge 4 of the diaphragm 3 connected to the frame 5 has a shape protruding upward as shown in FIG. 1 in this embodiment, so the load difference due to the edge 4 is taken into account. It is also the power.
- the third edge l ib is made of foamed resin, while the second edge 11a is made of rubber material. It is formed with.
- the foamed resin for example, foamed urethane resin can be used, and as the rubber material, for example, SBR rubber can be used.
- the edge 4 is reduced in thickness and weight as described above. As a result, the weight of the diaphragm 3 and the edge 4 is reduced, and the driving efficiency of the diaphragm 3 can be increased. As a result, the magnitude of the load is so large as it moves up and down, but if it still protrudes upwards in Fig. 1, it will still be deformed upwards and will not easily be deformed downwards. However, there is a slight difference in vertical dynamic load.
- the elastic modulus of the edge 1 lb is slightly smaller than the elastic modulus of the edge 1 la, that is, softened.
- edges 4 and l ib are both upwardly convex so that they are more likely to move upward than downward.
- the edge 11a has a convex shape downward so that it can be moved downward rather than upward.
- the damper 10 In the configuration in which the damper 10 is connected to the frame 5 via the edges 11a and l ib in this manner, the ring-like corrugated plate structure is used until the movable width of the voice coil body 2 is increased to some extent.
- the damper 10 can ensure amplitude linearity with respect to speaker input power, that is, power linearity.
- the movable width of the voice coil body 2 exceeds a predetermined value and the power linearity is not secured, the linearity can be compensated by the elasticity of the edges 11a and ib.
- an edge obtained by joining the second edge and the third edge is referred to as a combined edge.
- the coupling edge has a different elastic modulus with respect to the damper 10 and is set so that both function independently depending on the movable width of the voice coil body 2.
- the elastic modulus in the connection region 12 between the damper 10 and the edge 11a, l ib, more specifically in the connection region 12 between the damper 10 and the edge 11a, l ib is determined by the elastic modulus of the damper 10 and the edge 11a, l ib.
- the edge 1 la, and the edge 1 lb for example, the kind of the adhesive that bonds the edge 11a, ib and the damper 10 together It is preferable to use a hard adhesive such as acrylic, or attach a reinforcing material to the connection region 12.
- FIGS. 3 to 5 show other embodiments, respectively, in which only the damper 10 and the edges 11a and l ib in FIGS. 1 and 2 are changed.
- the other parts are in the same state as in FIG. 1.
- FIGS. 3 to 5 the same parts as those in FIGS. 1 and 2 are denoted by the same reference numerals to simplify the description.
- a third edge 11c (hereinafter referred to as an edge 11c) is provided in place of the edge l ib in FIGS.
- This edge 11c has a corrugated shape with two projecting shapes projecting to the diaphragm 3 side and one projecting shape in the opposite direction in a cross-sectional state. ing.
- the edge 11c is also formed of a material such as foamed urethane resin, foamed rubber, SBR rubber or cloth so as not to apply a large dynamic load to the diaphragm 3.
- edge 11c Since the edge 11c has two protruding shapes on the upper side and one protruding shape on the opposite side, the edge 11c is deformed upward in FIG. 3 and is hardly deformed downward. Yes. Therefore, if these edges 11a and 11c are combined together as shown in FIG. 3, the magnitudes of the vertical loads on the integrated edges 11a and 11c can be made substantially equal.
- edges 11a and 11c will be described in further detail.
- the edge 11c has a slightly smaller elastic modulus than the edge 11a. The reason is that the edge 4 connecting the outer peripheral end of the diaphragm 3 to the frame 5 has a shape protruding upward as shown in FIG. 1 in this embodiment as well, so the difference in load due to this edge 4 mm is taken into account. That's it.
- the thickness of the edge 4 is reduced and the weight is reduced to reduce the weight of the diaphragm 3 and the edge 4, thereby increasing the driving efficiency of the diaphragm 3.
- the magnitude of the load is so large. Even so, the edge 4 protrudes upward, so that it is also deformed upward and is not easily deformed downward. Therefore, there is a slight difference between the upper and lower dynamic loads.
- the edge 11c has a slightly lower elastic modulus than the edge 11a.
- the edge 4 has a single convex upward
- the edge 11c has a cross-sectional shape having two convex upwards, so that the edge 11c moves upward rather than immediately below
- the wedge 11a has a downwardly projecting cross-sectional shape, so that it is easier to move downward than upward. From the above, it is necessary to optimize the edge 11c and the edge 4 as a pair for one edge 11a. For these reasons, the edge 11c has a slightly smaller elastic modulus than the edge 11a.
- the vertical amplitude of the diaphragm 3 becomes substantially symmetrical in the vertical direction, and distortion in the speaker can be reduced. Since the edge 4 is lighter than the edge 4, a speaker with high driving efficiency can be provided even for medium and high sounds.
- edge l id is a corrugated shape having one projecting shape on the upper side, that is, on the diaphragm 3 side, and two projecting shapes on the lower side in a cross-sectional state.
- this edge id is also formed of a material such as urethane foam, foam rubber, SBR rubber or cloth so as not to apply a large dynamic load to the diaphragm 3.
- the edge id in this embodiment has one protruding shape on the upper side and two protruding shapes on the lower side. It is becoming difficult to do. For this reason, if these edges l id and l ib are combined together as shown in FIG. 4, the magnitudes of the vertical loads of the edges l id and l ib combined can be made substantially the same.
- edges l id and l ib will be described in more detail.
- the edge l ib has a slightly smaller elastic modulus than the edge l id.
- the reason is that the edge 4 connecting the outer peripheral edge of the diaphragm 3 to the frame 5 has a shape protruding upward as shown in FIG. 1 in this embodiment, so the difference in load due to the edge 4 mm is taken into consideration. That's what I did.
- the edge 4 is thin and lightweight, thereby reducing the weight of the diaphragm 3 and the edge 4 and increasing the driving efficiency of the diaphragm 3. Therefore, the load for vertical movement is not so large. Nevertheless, due to the difference in shape in the vertical direction, the difference in dynamic load between the top and bottom tends to occur.
- the edge l ib has an elastic modulus slightly smaller (softer) than the edge l id.
- the edges 4 and l ib have an upwardly convex cross-sectional shape, so that the edge l id is a cross-section having two protrusions below.
- the shape makes it easier to move downward than above. From the above, it is necessary to optimize the edge l ib and the edge 4 as one set for one edge l id. For these reasons, the edge l ib has a slightly smaller elastic modulus than the edge l id.
- the vertical amplitude of the diaphragm 3 becomes substantially symmetrical in the vertical direction, and distortion in the speaker can be reduced. Since the edge 4 is lighter than the edge 4, a speaker with high driving efficiency can be provided even for medium and high sounds.
- the edge l ie instead of the edges 11a and l ib in FIGS. 1 and 2, the edge 11d and the third edge l ie (hereinafter referred to as edge l ie) in FIG. 4 are used. It is provided.
- the edge l id has a corrugated shape having one protruding shape protruding upward and two downward protruding shapes opposite to each other in the cross-sectional state.
- the edge lie has a corrugated shape having two protruding shapes that protrude upward and one downward protruding shape opposite to the protruding shape.
- edges l id and l ie are also formed of a material such as foamed urethane resin, foamed rubber, SBR rubber or cloth so as not to apply a large dynamic load to the diaphragm 3.
- the edge id in this embodiment has one protruding shape on the upper side and two protruding shapes on the lower side. Therefore, the edge l id is deformed downward in FIG. It is becoming difficult to do. Further, since the edge lie has two protruding shapes on the upper side and one protruding shape on the lower side, it is deformed upward in FIG. 5 and is hardly deformed downward.
- edges l id and l ie will be described in more detail.
- the edge l ie has a slightly smaller elastic modulus than the edge l id.
- the reason is that the edge 4 connecting the outer peripheral end portion of the diaphragm 3 to the frame 5 has a shape protruding upward as shown in FIG. 1 in this embodiment, so the load difference due to the edge 4 is taken into account. It depends.
- the edge 4 is thin and light, thereby reducing the weight of the diaphragm 3 and the edge 4 and increasing the driving efficiency of the diaphragm 3. Therefore, although the magnitude of the load for vertical movement is not so large, the difference in the vertical load is likely to occur due to the difference in shape in the vertical direction.
- the edge l ie has a slightly smaller (softer) elastic modulus than the edge l id.
- the voice coil body 2 moves upward rather than downward due to the shape of the edge 4, l ie, but immediately moves upward due to the shape of the edge id. It is easier to move downward. From the above, since it is necessary to optimize the edge l ie and the edge 4 as a set for one edge l id, the edge l ie is more elastic than the edge l id. Is slightly smaller.
- a mode has been described in which the third edges l lb, 11c, and l ie are created separately from the second edges l la and l id.
- a joint edge in which the second edge of the protruding structure protruding downward with respect to the surface of the damper 10 and the third edge of the protruding structure protruding upward is integrally formed in advance is used. You can also Examples of this are shown in Figs. 6 and 7 are diagrams for explaining the cross-sectional shapes of the integrally formed coupling edges 1 If and 11m, respectively.
- the connecting edge 1 If in Fig. 6 has, in cross-sectional shape, one upward projecting structure llg and two downward projecting structures lh.
- the connecting edge 1 If is fixed to the damper 10 in the connection region 12.
- the protruding structure l lg and the protruding structure l lh are opposed to each other with a gap therebetween.
- the connecting edge 11m of Fig. 7 has one upward projecting structure 1In and two downward projecting structures 1lp in cross-sectional shape. Protruding structure 1 In protrudes above the damper surface AA.
- the connecting edge 11 m is fixed to the damper 10 in the connection region 12. The bonding edge 11m can be easily formed by hot pressing a single sheet.
- the coupling edge 1 If in FIG. 6 is an example in which the coupling edge composed of the second edge l id and the third edge 1 lb as shown in FIG. Similarly, the joint edges shown in FIGS. 2, 3, and 5 can be formed as a single-piece joint edge.
- the number of the protruding structures 1In upward may be larger than the number of the protruding structures 1lp downward depending on the protruding shape and the number of protruding portions.
- the protruding edges l If and 11m above the connecting edges 1 lg and 1 In have an elastic modulus greater than that of the first edge 4 Edge 1 If and 1 lm downward projecting structure 1 lh, preferably less than 1 lp elastic modulus.
- the upper and lower amplitudes of diaphragm 3 can be made substantially symmetrical in the vertical direction, and at the same time, speaker distortion due to improvement of the amplitude linearity of the speaker, that is, power linearity can be reduced.
- the edge 4 is lighter, it is possible to provide a speaker with high driving efficiency even for medium and high sounds.
- the present invention can reduce speaker distortion and drive efficiency in a speaker, and is particularly useful for a speaker for a full range, medium sound, and high range.
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- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Acoustics & Sound (AREA)
- Signal Processing (AREA)
- Multimedia (AREA)
- Diaphragms For Electromechanical Transducers (AREA)
- Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)
Abstract
Description
Claims
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP07708026A EP1892996A4 (en) | 2006-02-06 | 2007-02-05 | SPEAKER |
CN2007800006186A CN101326854B (zh) | 2006-02-06 | 2007-02-05 | 扬声器 |
US11/915,466 US7974434B2 (en) | 2006-02-06 | 2007-02-05 | Loudspeaker |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2006028073A JP4735299B2 (ja) | 2006-02-06 | 2006-02-06 | スピーカ |
JP2006-028073 | 2006-02-06 |
Publications (1)
Publication Number | Publication Date |
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WO2007091513A1 true WO2007091513A1 (ja) | 2007-08-16 |
Family
ID=38345111
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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PCT/JP2007/051908 WO2007091513A1 (ja) | 2006-02-06 | 2007-02-05 | スピーカ |
Country Status (6)
Country | Link |
---|---|
US (1) | US7974434B2 (ja) |
EP (1) | EP1892996A4 (ja) |
JP (1) | JP4735299B2 (ja) |
KR (1) | KR20080015121A (ja) |
CN (1) | CN101326854B (ja) |
WO (1) | WO2007091513A1 (ja) |
Cited By (1)
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CN102666094A (zh) * | 2009-12-30 | 2012-09-12 | 乐金华奥斯株式会社 | 离型膜及其制备方法 |
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CN1992996B (zh) * | 2005-12-30 | 2012-02-29 | 丁轶 | 扬声器振膜的分体式支承结构 |
JP4735376B2 (ja) * | 2006-04-04 | 2011-07-27 | パナソニック株式会社 | スピーカ用ダンパーおよびこれを用いたスピーカ |
US20100158305A1 (en) * | 2008-06-05 | 2010-06-24 | Osamu Funahashi | Loudspeaker |
KR101046786B1 (ko) * | 2009-05-25 | 2011-07-05 | 에스텍 주식회사 | 스피커 |
WO2011001498A1 (ja) * | 2009-06-29 | 2011-01-06 | パイオニア株式会社 | スピーカ用ダンパ、スピーカ装置 |
FR2947689A1 (fr) * | 2009-07-03 | 2011-01-07 | Focal Jmlab | Combinaison de "spider" a rupture de linearite controlee et de suspension a amortissement dans un haut parleur pour enceinte acoustique |
JP2011166335A (ja) * | 2010-02-08 | 2011-08-25 | Panasonic Corp | スピーカ |
US8442259B2 (en) * | 2010-06-04 | 2013-05-14 | Beats Electronics, Llc | System for vibration confinement |
CN202949560U (zh) * | 2012-11-16 | 2013-05-22 | 瑞声声学科技(常州)有限公司 | 发声器 |
US9485586B2 (en) | 2013-03-15 | 2016-11-01 | Jeffery K Permanian | Speaker driver |
KR101413965B1 (ko) * | 2013-04-15 | 2014-07-04 | 에스텍 주식회사 | 시스템 스피커 |
KR101503820B1 (ko) * | 2013-09-23 | 2015-03-25 | 아이모스시스템 주식회사 | 고출력 스피커 |
US9466280B2 (en) * | 2014-10-24 | 2016-10-11 | Bose Corporation | Acoustic device suspension |
US9854365B2 (en) * | 2016-04-15 | 2017-12-26 | Harman International Industries, Inc. | Loudspeaker motor and suspension system |
CN107580284B (zh) * | 2017-08-31 | 2019-08-23 | 东莞顺合丰电业有限公司 | 扬声器 |
WO2020227956A1 (zh) * | 2019-05-10 | 2020-11-19 | 瑞声声学科技(深圳)有限公司 | 一种磁路系统及应用其的扬声器 |
US11044562B1 (en) * | 2020-01-21 | 2021-06-22 | Resonado, Inc. | Multi-diaphragm speaker driven by multiple voice coil plates and a shared permanent magnet pair |
CN111641902B (zh) * | 2020-05-20 | 2021-09-28 | 瑞声科技(新加坡)有限公司 | 一种发声器件 |
CN112969132B (zh) * | 2021-01-29 | 2023-01-24 | 歌尔股份有限公司 | 弹性支片、电子装置及终端 |
CN113965860B (zh) * | 2021-12-23 | 2022-04-12 | 深圳市中天迅通信技术股份有限公司 | 发声单元 |
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JP2004007332A (ja) | 2002-04-15 | 2004-01-08 | Matsushita Electric Ind Co Ltd | スピーカ |
JP2004364270A (ja) * | 2003-06-04 | 2004-12-24 | Harman Becker Automotive Systems Gmbh | ラウドスピーカ |
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2006
- 2006-02-06 JP JP2006028073A patent/JP4735299B2/ja not_active Expired - Fee Related
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2007
- 2007-02-05 CN CN2007800006186A patent/CN101326854B/zh not_active Expired - Fee Related
- 2007-02-05 EP EP07708026A patent/EP1892996A4/en not_active Withdrawn
- 2007-02-05 WO PCT/JP2007/051908 patent/WO2007091513A1/ja active Application Filing
- 2007-02-05 KR KR1020077029954A patent/KR20080015121A/ko not_active Application Discontinuation
- 2007-02-05 US US11/915,466 patent/US7974434B2/en not_active Expired - Fee Related
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CN102666094A (zh) * | 2009-12-30 | 2012-09-12 | 乐金华奥斯株式会社 | 离型膜及其制备方法 |
Also Published As
Publication number | Publication date |
---|---|
CN101326854A (zh) | 2008-12-17 |
EP1892996A1 (en) | 2008-02-27 |
JP4735299B2 (ja) | 2011-07-27 |
EP1892996A4 (en) | 2011-10-19 |
US20090080686A1 (en) | 2009-03-26 |
US7974434B2 (en) | 2011-07-05 |
KR20080015121A (ko) | 2008-02-18 |
JP2007208877A (ja) | 2007-08-16 |
CN101326854B (zh) | 2011-08-03 |
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