JPH0534797U - Magnetic circuit for speaker - Google Patents
Magnetic circuit for speakerInfo
- Publication number
- JPH0534797U JPH0534797U JP9145591U JP9145591U JPH0534797U JP H0534797 U JPH0534797 U JP H0534797U JP 9145591 U JP9145591 U JP 9145591U JP 9145591 U JP9145591 U JP 9145591U JP H0534797 U JPH0534797 U JP H0534797U
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- Japan
- Prior art keywords
- magnet
- magnetic
- magnetic circuit
- sub
- speaker
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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- Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)
Abstract
(57)【要約】
【目的】 副磁石を使用して、漏洩磁束を減少して、 磁
気空隙の磁束密度を向上する。
【構成】 内磁型磁気回路の、 上部プレートの上端部に
穿設した中心穴の内側面に、 上部プレートと略厚さを等
しくした直円環状の副磁石を嵌入して保持し、前記異方
性磁石の中心穴の内側面を、 磁気空隙の外側面として形
成して、 主磁石の磁路方向に直列に副磁石を挿入装着し
て、 該磁石を半径方向に着磁した構造。 (57) [Summary] [Purpose] A secondary magnet is used to reduce the leakage flux and improve the magnetic flux density in the magnetic gap. [Structure] An inner magnet type magnetic circuit is fitted with and held by a sub-circular sub-magnet having a thickness substantially equal to that of the upper plate on the inner side surface of a center hole formed at the upper end of the upper plate, and the above-mentioned difference A structure in which the inner surface of the center hole of the direction magnet is formed as the outer surface of the magnetic gap, the sub magnets are inserted and mounted in series in the magnetic path direction of the main magnet, and the magnets are magnetized in the radial direction.
Description
【0001】[0001]
本考案は、内磁型に使用した主磁石の性能を高度に引き出すとともに、 副磁石 により周囲への漏洩磁束を軽減したスピーカ用の磁気回路に関するものである。 The present invention relates to a magnetic circuit for a speaker, in which the performance of a main magnet used for an inner magnet type is brought out to a high degree and a magnetic flux leaking to the surroundings is reduced by a sub magnet.
【0002】[0002]
従来この種のスピーカ(11')の磁気回路(5")は、図7,図8に示した様に、下 部プレート(2e')の内底面に設けた凹部に、 円柱状の例えばアルニコ磁石(3')を 載置し、その上にセンタポール(1')を固着して、上部プレート(2c')の中心磁気 空隙穴(2d')内に、前記のセンタポール(1')の先端磁極部(1a')を覗出させて、円 筒ヨーク(2')側面部(2a')の下部側面部(2b')を、 前記の下部プレート(2e')の側 面縁立て部(2f')の内面部に嵌合して結合固定し、円環状磁気空隙(6')を形成し たいわゆる内磁型磁気回路構造が主であった。 As shown in FIGS. 7 and 8, the magnetic circuit (5 ″) of the speaker (11 ′) of this type conventionally has a cylindrical shape, for example, an alnico, in a recess provided in the inner bottom surface of the lower plate (2e ′). Place the magnet (3 '), fix the center pole (1') on it, and insert the center pole (1 ') into the center magnetic hole (2d') of the upper plate (2c '). Of the lower side plate (2e ') of the lower plate (2e') and the lower side part (2b ') of the side part (2a') of the cylindrical yoke (2 '). The so-called inner magnet type magnetic circuit structure in which the annular magnetic air gap (6 ′) was formed by fitting and coupling to the inner surface of the portion (2f ′) was mainly used.
【0003】 そして、 前記磁気回路(5")の磁気空隙(6')内にボイスコイル(8')をダンパ(9') で支持し、 その先端の外周をフレーム(7')に貼り付けた振動板(10')の先端部を 取り付けて、 スピーカ(11')として組み立てられていた。Then, the voice coil (8 ') is supported by the damper (9') in the magnetic gap (6 ') of the magnetic circuit (5 "), and the outer periphery of the tip is attached to the frame (7'). It was assembled as a speaker (11 ') by attaching the tip of the diaphragm (10').
【0004】[0004]
したがって、従来のこの種の内磁型磁気回路(5")にあっては、図8に示すよう に、磁気空隙(6')の部分が磁気回路(5")中の磁路全行程の内、 最も磁気抵抗が大 きく、 そのために磁力線の流れが、 磁気空隙(6')から外部へ飛び出して漏洩する 成分が殆どで、 ボイスコイルの駆動力の根源となる磁気空隙(6')内を通過する磁 束の比率が小さい(図8)ので、 能率の良いスピーカが得られないという問題が あった。 Therefore, in the conventional inner magnet type magnetic circuit (5 ") of this kind, as shown in FIG. 8, the magnetic gap (6 ') is the entire magnetic path of the magnetic circuit (5"). Of these, the magnetic reluctance is the largest, and as a result, the flow of lines of magnetic force mostly leaks out of the magnetic air gap (6 ') and leaks out. Since the ratio of magnetic flux passing through is small (Fig. 8), there is a problem that a speaker with good efficiency cannot be obtained.
【0005】 そこで、本考案は、このような従来の内磁型磁気回路(5")が有していた問題点 を解決するために、主磁石(3)には従来の例えばアルニコ磁石を使用し、同様の アルニコ磁石を副磁石(4)として磁路の一部に使用することによって、主磁石に よる磁気回路(5)の性能発揮と、 副磁石(4)の起磁力を利用して、 磁気空隙(6)の 外部に漏れる漏洩磁気を少なくして、 主、 副両磁石(3),(4)の使用効率を高めて 、磁石のスペースファクタの向上を図ることを目的とし、磁気空隙(6)の磁束密 度を飛躍的に向上させて、 小形で、 強力、 かつ高能率なスピーカに適した磁気回 路(5)を提供しようとするものである。Therefore, the present invention uses a conventional alnico magnet, for example, as the main magnet (3) in order to solve the problems of the conventional inner magnet type magnetic circuit (5 "). However, by using a similar alnico magnet as a sub-magnet (4) in a part of the magnetic path, the main magnet exerts the performance of the magnetic circuit (5) and the magnetomotive force of the sub-magnet (4) is utilized. , The magnetic flux that leaks to the outside of the magnetic air gap (6) is reduced, the use efficiency of the primary and secondary magnets (3), (4) is improved, and the space factor of the magnet is improved. It is intended to dramatically improve the magnetic flux density of the air gap (6) to provide a magnetic circuit (5) suitable for a compact, powerful, and highly efficient speaker.
【0006】[0006]
該目的を達成するための本考案の構成を、実施例に対応する図1乃至図2を用 いて説明すると、本考案は、内磁型磁気回路において、 上部プレート(2c)の上端 部(2d)に穿設した中心穴(2e)の内側面(2h)に、 上部プレート(2c)と略厚さを等し くした直円環状の磁石(4)を嵌入して保持し、 前記副磁石(4)の中心穴の内側面を 、磁気空隙(6)の外側面(6e)として形成し、 主磁石(3)の磁路方向に直列に磁石(4 )を挿入装着して、 該磁石(4)を半径方向に着磁したスピーカ用磁気回路(5)であ る。 The structure of the present invention for achieving the above object will be described with reference to FIGS. 1 and 2 corresponding to the embodiments. The present invention, in an inner magnet type magnetic circuit, shows the upper end portion (2d) of the upper plate (2c). ), The inner surface (2h) of the center hole (2e) formed in (1) is fitted with and retained by a magnet (4) in the shape of a circular ring with an approximately equal thickness to the upper plate (2c). The inner surface of the central hole of (4) is formed as the outer surface (6e) of the magnetic gap (6), and the magnet (4) is inserted and mounted in series in the magnetic path direction of the main magnet (3). This is a magnetic circuit for speakers (5) in which (4) is magnetized in the radial direction.
【0007】[0007]
本考案は、このような構造としたものであるから、図7に示す従来の例えばア ルニコ磁石を使用した主磁気回路の磁路の一部に直列に、 副磁石(4)を挿入する ことによって、図1,図2に示すように、副磁石(4)の起磁力を利用して、 磁気 空隙(6)の外部に漏れる漏洩磁気を少なくして、 磁気空隙(6)内に磁束を集中する ことができる。 Since the present invention has such a structure, it is necessary to insert the auxiliary magnet (4) in series with a part of the magnetic path of the main magnetic circuit using the conventional alnico magnet shown in FIG. 7, for example. As shown in Figs. 1 and 2, the magnetomotive force of the sub-magnet (4) is used to reduce the leakage magnetism leaking to the outside of the magnetic air gap (6), and the magnetic flux is generated in the magnetic air gap (6). You can concentrate.
【0008】[0008]
以下本考案の実施例について図面に基づいて説明する。 図中、図1及び図2は、本第1考案の1実施例を示す図であって、図1はその 縦断面図を、図2は図1の実施例の磁力線の流れを示す縦断面図である。 An embodiment of the present invention will be described below with reference to the drawings. 1 and 2 are views showing an embodiment of the first invention, FIG. 1 is a longitudinal sectional view thereof, and FIG. 2 is a longitudinal sectional view showing a flow of magnetic force lines of the embodiment of FIG. It is a figure.
【0009】 本第1考案は、内磁型磁気回路において、 上部プレート(2c)の上端部(2d)に穿 設した中心穴(2e)の内側面(2h)に、 上部プレート(2c)と略厚さを等しくした直円 環状の副磁石(4)を嵌入して保持し、 前記副磁石(4)の中心穴の内側面を、 磁気空 隙(6)の外側面(6e)として形成し、 主磁石(3)の磁路方向に直列に副磁石(4)を挿 入装着して、 該磁石(4)を半径方向に着磁したスピーカ用磁気回路(5)である。The first aspect of the present invention is that, in an inner magnet type magnetic circuit, an upper plate (2c) is formed on an inner side surface (2h) of a central hole (2e) formed at an upper end (2d) of the upper plate (2c). A sub-circular sub magnet (4) of approximately the same thickness is fitted and held, and the inner surface of the center hole of the sub magnet (4) is formed as the outer surface (6e) of the magnetic space (6). The secondary magnet (4) is inserted and mounted in series in the magnetic path direction of the main magnet (3), and the magnet (4) is magnetized in the radial direction to provide a speaker magnetic circuit (5).
【0010】 第2考案は、第1考案を変形した構造であって、図3に示すように、前記の副 磁石(4)を嵌入して保持した、 上部プレート(2c)の上面が、 副磁石(4)の上面を含 めて、 センタポール(1)の上面(1a)より少なくとも(D)以上高く位置せしめた第 1考案相当のスピーカ用磁気回路(5')である。ここにD>0の関係式が成立する 。A second aspect of the present invention is a modified structure of the first aspect of the present invention. As shown in FIG. 3, the upper surface of the upper plate (2c) in which the sub magnet (4) is fitted and held is A magnetic circuit (5 ') for a speaker equivalent to the first invention, which is located at least (D) higher than the upper surface (1a) of the center pole (1) including the upper surface of the magnet (4). Here, the relational expression of D> 0 holds.
【0011】 以上本考案の代表的と思われる実施例について説明したが、本考案は必ずしも これらの実施例構造のみに限定されるものではなく、本考案にいう前記の構成要 件を備え、かつ、本考案にいう目的を達成し、以下にいう効果を有する範囲内に おいて適宜改変して実施することができるものである。Although the embodiments considered to be typical of the present invention have been described above, the present invention is not necessarily limited only to the structures of these embodiments, and has the above-mentioned configuration requirements according to the present invention, and The present invention can be carried out with appropriate modifications within the scope of achieving the object of the present invention and having the following effects.
【0012】[0012]
以上の説明から既に明らかなように、本考案は、このような構造としたもので あるから、主磁石には従来の例えばアルニコ磁石を使用して、副磁石(4)として 磁路の一部に使用することによって、主磁石による磁気回路の性能発揮と、 異方 性磁石(4)の起磁力を利用して、 磁気空隙(6)の外部に漏れる漏洩磁気を少なくし て、 主、 副両磁石(3),(4)の使用効率を高めて、 磁石のスペースファクタの向上 を図ることを目的とし、磁気空隙の磁束密度を飛躍的に向上させて、 小形で、 強 力、 かつ高能率なスピーカに適した磁気回路(5)となる。 従来例と本願考案との磁気回路の漏洩磁束の比較を、 磁気空隙のレラクタンス の比較から計算すると、次ぎの表1のようになる。 As is apparent from the above description, since the present invention has such a structure, a conventional alnico magnet, for example, is used as the main magnet, and a part of the magnetic path is used as the sub magnet (4). By using the magnetic field performance of the main magnet and the magnetomotive force of the anisotropic magnet (4), the leakage magnetism that leaks to the outside of the magnetic air gap (6) can be reduced, and The magnetic flux density of the magnetic air gap is dramatically improved by increasing the use efficiency of both magnets (3) and (4) to improve the space factor of the magnet, resulting in a small size, high strength, and high strength. The magnetic circuit (5) is suitable for an efficient speaker. The comparison of the leakage flux of the magnetic circuit between the conventional example and the present invention is calculated from the comparison of the reluctance of the magnetic gap.
【0013】[0013]
【表1】 [Table 1]
【0014】 従来例と本願考案との磁気回路側面の近傍を、 磁気回路の軸と平行な方向に沿 って測定した漏洩磁束の実数比較は、図4,図5に示すとおりであって、横軸に 磁気回路(原点0)からの距離を取り、縦軸にその点からの磁束密度の絶対値を示 す。 測定位置は、図5に示すとおりである。これらから見られるように、本考 案実施例は従来例に対し、 15〜23%漏洩磁束が少なく、有効に作用して効果 が現出している。即ち、図4の従来例と本願考案の実施例のカーブの上下の開き の大きな箇所が漏洩磁束の差が大きなところである。これから、磁気回路外側の 原点O点から2cmの測定点が、 最も差が大きくなっている。A comparison of the real numbers of the leakage magnetic flux measured along the direction parallel to the axis of the magnetic circuit in the vicinity of the side surface of the magnetic circuit between the conventional example and the present invention is as shown in FIGS. The horizontal axis shows the distance from the magnetic circuit (origin 0), and the vertical axis shows the absolute value of the magnetic flux density from that point. The measurement position is as shown in FIG. As can be seen from the above, the proposed embodiment has 15 to 23% less magnetic flux leakage than the conventional example, and the effect is exhibited by effectively acting. That is, there is a large difference in the leakage magnetic flux between the conventional example shown in FIG. From this, the difference is the largest at the measurement point 2 cm from the origin O point outside the magnetic circuit.
【0015】 図6に示す図は、従来例と本考案実施例の磁気空隙に発生する磁束密度の比較 であり、横軸に磁気空隙上端部(0)からの距離を、 縦軸に磁束密度の絶対値を表 す。これから見られるように、磁気空隙の中央付近で本考案で10,200ガウス、 従 来例で8,000ガウスとなり、 実施例は従来例に対して24%程度向上している。 第2考案は、図3に示すように、請求項1に記載のスピーカ用磁気回路の変形 であって、前記の副磁石(4)を嵌入して保持した、 上部プレート(2c)の上面が、 磁石(4)の上面を含めて、 センタポール(1)の上面(1a)より少なくとも高く位置せ しめた構造によって、センタポール(1)の上面(1a)の角部の、 最も磁束の集中す る箇所が、 副磁石(4)の磁気空隙(6)の中腹部に対向するので、 磁束が下方へ引き 込まれて、 その漏洩率が減少し、磁気空隙の磁束密度の増加効果は更に向上する 。FIG. 6 is a comparison of the magnetic flux densities generated in the magnetic gap of the conventional example and the embodiment of the present invention. The horizontal axis represents the distance from the upper end (0) of the magnetic gap, and the vertical axis represents the magnetic flux density. Represents the absolute value of. As can be seen, in the vicinity of the center of the magnetic gap, the present invention has 10,200 gauss and the conventional example has 8,000 gauss, which is about 24% higher than that of the conventional example. The second invention is a modification of the speaker magnetic circuit according to claim 1, as shown in FIG. 3, in which the upper surface of the upper plate (2c) in which the sub magnet (4) is fitted and held is , The top of the center pole (1) including the top surface of the magnet (4) is positioned at least higher than the top surface (1a) of the center pole (1). Since the magnetic field faces the middle part of the magnetic air gap (6) of the sub-magnet (4), the magnetic flux is drawn downward, the leakage rate is reduced, and the effect of increasing the magnetic flux density of the magnetic air gap is further reduced. improves .
【図1】本考案の1実施例を示した縦断面図。FIG. 1 is a vertical sectional view showing an embodiment of the present invention.
【図2】図1の本考案の実施例の磁力線の流れを示す縦
断面図。FIG. 2 is a vertical cross-sectional view showing the flow of magnetic force lines according to the embodiment of the present invention in FIG.
【図3】本考案の他の実施例の縦断面図。FIG. 3 is a vertical sectional view of another embodiment of the present invention.
【図4】磁気回路の側面漏洩磁束の比較図。FIG. 4 is a comparison diagram of side leakage magnetic flux of a magnetic circuit.
【図5】図4の測定点の位置を示す図。FIG. 5 is a diagram showing the positions of measurement points in FIG.
【図6】磁気空隙内の磁束密度の比較図。FIG. 6 is a comparison diagram of magnetic flux densities in a magnetic gap.
【図7】従来例の縦断面図。FIG. 7 is a vertical sectional view of a conventional example.
【図8】従来例の磁力線の流れを示す縦断面図。FIG. 8 is a vertical cross-sectional view showing the flow of magnetic force lines in a conventional example.
(1) センタポール (1a) センタポール先端部 (2) 円筒形ヨーク (2a) 円筒形ヨーク側面部 (2b) 円筒形ヨーク下部内側面 (2c) 上部プレート (2d) 上端部 (2e) 中心穴 (2h) 内側面 (3) 主磁石 (4) 副磁石 (5) 磁気回路 (5') 磁気回路 (6) 磁気空隙 (6e) 磁気空隙外側面 (D) 差 (1) Center pole (1a) Center pole tip (2) Cylindrical yoke (2a) Cylindrical yoke side surface (2b) Cylindrical yoke lower inner surface (2c) Upper plate (2d) Upper end (2e) Center hole (2h) Inner surface (3) Main magnet (4) Secondary magnet (5) Magnetic circuit (5 ') Magnetic circuit (6) Magnetic air gap (6e) Magnetic air gap outer surface (D) Difference
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【手続補正書】[Procedure amendment]
【提出日】平成3年12月6日[Submission date] December 6, 1991
【手続補正1】[Procedure Amendment 1]
【補正対象書類名】図面[Document name to be corrected] Drawing
【補正対象項目名】図4[Name of item to be corrected] Fig. 4
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【図4】 [Figure 4]
【手続補正2】[Procedure Amendment 2]
【補正対象書類名】図面[Document name to be corrected] Drawing
【補正対象項目名】図6[Name of item to be corrected] Figure 6
【補正方法】変更[Correction method] Change
【補正内容】[Correction content]
【図6】 [Figure 6]
Claims (2)
(2c)の上端部(2d)に穿設した中心穴(2e)の内側面(2h)
に、 上部プレート(2c)と略厚さを等しくした直円環状の
副磁石(4)を嵌入して保持し、 前記副磁石(4)の中心穴の
内側面を、 磁気空隙(6)の外側面(6e)として形成し、 主
磁石(3)の磁路方向に直列に副磁石(4)を挿入装着して、
該磁石(4)を半径方向に着磁したスピーカ用磁気回路。1. In an inner magnet type magnetic circuit, an upper plate
Inner surface (2h) of the center hole (2e) formed in the upper end (2d) of (2c)
A sub-magnet (4) in the shape of a circular ring of approximately the same thickness as the upper plate (2c) is inserted and held, and the inner surface of the center hole of the sub-magnet (4) is fixed to the magnetic gap (6). It is formed as an outer surface (6e), and the auxiliary magnet (4) is inserted and installed in series in the magnetic path direction of the main magnet (3).
A magnetic circuit for a speaker, wherein the magnet (4) is magnetized in the radial direction.
上部プレート(2c)の上面が、 副磁石(4)の上面を含めて、
センタポール(1)の上面(1a)より少なくとも(D)以上高
く位置せしめた請求項1に記載のスピーカ用磁気回路。2. The auxiliary magnet (4) is inserted and held,
The upper surface of the upper plate (2c), including the upper surface of the sub magnet (4),
2. The speaker magnetic circuit according to claim 1, wherein the center pole (1) is positioned at least (D) higher than the upper surface (1a) of the center pole (1).
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9145591U JP2568241Y2 (en) | 1991-10-11 | 1991-10-11 | Magnetic circuit for speaker |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9145591U JP2568241Y2 (en) | 1991-10-11 | 1991-10-11 | Magnetic circuit for speaker |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0534797U true JPH0534797U (en) | 1993-05-07 |
JP2568241Y2 JP2568241Y2 (en) | 1998-04-08 |
Family
ID=14026846
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9145591U Expired - Lifetime JP2568241Y2 (en) | 1991-10-11 | 1991-10-11 | Magnetic circuit for speaker |
Country Status (1)
Country | Link |
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JP (1) | JP2568241Y2 (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2006080405A1 (en) * | 2005-01-28 | 2006-08-03 | Matsushita Electric Industrial Co., Ltd. | Electrokinetic electro-acoustic converter and electronic device |
JP2007281869A (en) * | 2006-04-06 | 2007-10-25 | Fujitsu Ten Ltd | Speaker magnetic circuit |
JP2007281910A (en) * | 2006-04-07 | 2007-10-25 | Matsushita Electric Ind Co Ltd | Speaker and electronic apparatus using the same |
WO2008038762A1 (en) * | 2006-09-29 | 2008-04-03 | Panasonic Corporation | Process for manufacturing speaker |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US11184712B2 (en) | 2015-05-19 | 2021-11-23 | Bose Corporation | Dual-field single-voice-coil transducer |
US11245986B2 (en) | 2019-10-24 | 2022-02-08 | Bose Corporation | Electro-magnetic motor geometry with radial ring and axial pole magnet |
-
1991
- 1991-10-11 JP JP9145591U patent/JP2568241Y2/en not_active Expired - Lifetime
Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2006080405A1 (en) * | 2005-01-28 | 2006-08-03 | Matsushita Electric Industrial Co., Ltd. | Electrokinetic electro-acoustic converter and electronic device |
EP1843630A1 (en) * | 2005-01-28 | 2007-10-10 | Matsushita Electric Industrial Co., Ltd. | Electrodynamic electroacoustic transducer and electronic device |
EP1843630A4 (en) * | 2005-01-28 | 2010-10-27 | Panasonic Corp | Electrodynamic electroacoustic transducer and electronic device |
EP2437518A1 (en) | 2005-01-28 | 2012-04-04 | Panasonic Corporation | Electrodynamic electroacoustic transducer and electronic device |
JP2007281869A (en) * | 2006-04-06 | 2007-10-25 | Fujitsu Ten Ltd | Speaker magnetic circuit |
JP2007281910A (en) * | 2006-04-07 | 2007-10-25 | Matsushita Electric Ind Co Ltd | Speaker and electronic apparatus using the same |
JP4661666B2 (en) * | 2006-04-07 | 2011-03-30 | パナソニック株式会社 | Speaker and electronic device using it |
WO2008038762A1 (en) * | 2006-09-29 | 2008-04-03 | Panasonic Corporation | Process for manufacturing speaker |
WO2008038760A1 (en) * | 2006-09-29 | 2008-04-03 | Panasonic Corporation | Speaker and electronic equipment utilizing the same |
WO2008038761A1 (en) * | 2006-09-29 | 2008-04-03 | Panasonic Corporation | Process for manufacturing speaker |
Also Published As
Publication number | Publication date |
---|---|
JP2568241Y2 (en) | 1998-04-08 |
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