JPS5955699A - Entirely dynamic driving speaker - Google Patents

Entirely dynamic driving speaker

Info

Publication number
JPS5955699A
JPS5955699A JP16502982A JP16502982A JPS5955699A JP S5955699 A JPS5955699 A JP S5955699A JP 16502982 A JP16502982 A JP 16502982A JP 16502982 A JP16502982 A JP 16502982A JP S5955699 A JPS5955699 A JP S5955699A
Authority
JP
Japan
Prior art keywords
diaphragm
magnetic poles
parallel
magnetic
voice coil
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.)
Pending
Application number
JP16502982A
Other languages
Japanese (ja)
Inventor
Masanori Tanaka
田中 政則
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura Electric Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP16502982A priority Critical patent/JPS5955699A/en
Publication of JPS5955699A publication Critical patent/JPS5955699A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R9/00Transducers of moving-coil, moving-strip, or moving-wire type
    • H04R9/02Details
    • H04R9/04Construction, mounting, or centering of coil
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R9/00Transducers of moving-coil, moving-strip, or moving-wire type
    • H04R9/02Details
    • H04R9/025Magnetic circuit
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R9/00Transducers of moving-coil, moving-strip, or moving-wire type
    • H04R9/02Details
    • H04R9/04Construction, mounting, or centering of coil
    • H04R9/046Construction
    • H04R9/047Construction in which the windings of the moving coil lay in the same plane
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R9/00Transducers of moving-coil, moving-strip, or moving-wire type
    • H04R9/06Loudspeakers

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Acoustics & Sound (AREA)
  • Signal Processing (AREA)
  • Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)

Abstract

PURPOSE:To attain the reproduction of a low frequency by arraying plural rod- like magnetic poles in parallel and with an alternately opposed polarity, arranging a diaphragm with a waveform section so as to cover the magnetic poles arrayed in parallel and then setting up a voice coil on the surface of the diaphragm between adjacent magnetic poles. CONSTITUTION:The end parts of plural magnetic poles 6, 6' consisting of a highly magnetic permeable material and arranged in parallel are coupled with both ends of a permanent magnet 7 through highly magnetic permeable supporting plates 12, 12', and for instance, the magnetic poles 6, 6' are magnetized with N and S poles respectively. On the other hand, the diaphragm 8 is held by a frame body 10 through an edge 9. The cross section of the diaphragm 8 is formed by affording a ruggedness to curve along the magnetic poles 6, 6' and each voice coil 11 is arranged between the adjacent magnetic poles 6, 6' on the surface of the diaphragm 8. The voice coils 11-1, 11-3 and 11-2, 11-4 are connected to conduct a reverse current and the diaphragm is driven in the same direction by the voice coils in all. Thus, the stiffness of an oscillation system is reduced to reproduce the low frequency and to improve the efficiency of conversion.

Description

【発明の詳細な説明】 〔発明の技術分野〕 カ との発明は動電型の全面駆動スピーNに関する。[Detailed description of the invention] [Technical field of invention] mosquito The invention relates to an electrodynamic type full-surface driving speed N.

〔発明の技術的背景〕[Technical background of the invention]

動電型全面駆動スピーカは、振動板の全面にわたって同
時に駆動することから振動板の分割振動が発生しにくく
、従って音響特性も一般に良く、一部高忠実ステレオ用
のスピーカとして実用されている。従来の駆動型全面駆
動スピーカの一例を第1図にその断面斜視図を示す。振
動板1の表面にはボイスコイル2が設けられ、その振動
板1は枠体3により保持されている。−力抜数個の永久
磁石4はヨーク5を介して枠体3に固定される。
Electrodynamic full-drive speakers drive the entire surface of the diaphragm at the same time, making it difficult for the diaphragm to cause split vibration, and therefore generally have good acoustic characteristics, and are used in some high-fidelity stereo speakers. FIG. 1 shows a cross-sectional perspective view of an example of a conventional fully driven speaker. A voice coil 2 is provided on the surface of the diaphragm 1, and the diaphragm 1 is held by a frame 3. - Several permanent magnets 4 are fixed to the frame 3 via a yoke 5.

ここで永久磁石4の極性及び永久磁石とボイスコイル2
の位置関係を見れば、第2図に示すようになる。すなわ
ち振動板1をはさんで対向する一対の磁石は同極性の磁
極を内側に向けて配置され、かつ隣シ合った磁石は互い
に反対方向の極性となるように配置される。こうするこ
とによシ図中矢印で示したように振動板1と略平行な磁
界を生成することが出来る。ここで振動板1の表面のボ
イスコイル2は前記した略平行な磁界中にその磁界と直
交するように配置される。このような構造にしてボイス
コイルに信号電流を流せば、電流信号に応じた音響信号
を発生することが出来る。
Here, the polarity of the permanent magnet 4, the permanent magnet and the voice coil 2
If you look at the positional relationship, it will be as shown in Figure 2. That is, a pair of magnets facing each other with the diaphragm 1 in between are arranged with their magnetic poles of the same polarity facing inward, and adjacent magnets are arranged so that their polarities are opposite to each other. By doing so, it is possible to generate a magnetic field substantially parallel to the diaphragm 1, as shown by the arrow in the figure. Here, the voice coil 2 on the surface of the diaphragm 1 is placed in the above-described substantially parallel magnetic field so as to be perpendicular to the magnetic field. If a signal current is caused to flow through the voice coil with such a structure, it is possible to generate an acoustic signal corresponding to the current signal.

〔背景技術の問題点〕[Problems with background technology]

ところがこの様なスピーカは以下に述べるような欠点を
有していた。すなわち、1としてボイスコイル付近の磁
界を平行かつ均一にするのが困難なため、とくに低音の
大振巾動作時に歪が発生しやすい。2として磁力線を空
中で曲げる構造になるため、もれ磁束が多くなシ磁束を
有効に使えないのでスピーカとしての能率を高くするこ
とが非常に困難であり、一定の能率を確保するためには
磁性材料を沢山使う必要がありコスト高になる傾向があ
る。3として各磁石の磁化方向が交互に逆向きになるの
で、組立て後に磁石を磁化するのが困難である。従って
既に磁化された磁石を用いてスピーカを組立てる必要が
あるが、磁石の吸引力や反発力のため組立ては容易で々
く量産性に乏しかった。
However, such speakers have the following drawbacks. That is, since it is difficult to make the magnetic field near the voice coil parallel and uniform, distortion is likely to occur particularly during large amplitude operation of bass sounds. 2. Since the structure bends the lines of magnetic force in the air, it is very difficult to increase the efficiency of the speaker because there is a lot of leakage magnetic flux and the magnetic flux cannot be used effectively.In order to ensure a certain level of efficiency, It is necessary to use a large amount of magnetic material, and the cost tends to be high. Third, since the magnetization direction of each magnet is alternately reversed, it is difficult to magnetize the magnets after assembly. Therefore, it is necessary to assemble a speaker using magnets that have already been magnetized, but because of the attractive and repulsive forces of the magnets, assembly is difficult and mass production is difficult.

〔発明の目的〕[Purpose of the invention]

この発明の目的とするところは、電気音響変換効率が高
く大振中動作において歪を発生しにくい動電型全面駆動
スピーカを提供するにある。
An object of the present invention is to provide an electrodynamic full-plane drive speaker that has high electroacoustic conversion efficiency and is less likely to generate distortion during operation during large vibrations.

〔発明の概要〕[Summary of the invention]

この発明に詠へ″%は、複数個の極性の異なる磁極を交
互に並べ隣り合う磁極の間に略平行磁界が発生するよう
にするとともに、振動板はこれらの磁極を縫うように断
面波形に形成配置し、前記略し 来又、隣合う磁極の間隔はボイスコイルを含めた振動板
の厚さよりも大きくする必要があるが、通常この厚さは
非常に小さく出来るので、ギャップでの磁界を強くする
ことが出来る。以上により変換効率を高くし大振巾動作
時の歪を小さくすることが出来た。
In this invention, a plurality of magnetic poles with different polarities are alternately arranged so that a substantially parallel magnetic field is generated between adjacent magnetic poles, and the diaphragm has a cross-sectional waveform that threads through these magnetic poles. In addition, the distance between adjacent magnetic poles must be greater than the thickness of the diaphragm including the voice coil, but this thickness can usually be made very small, so the magnetic field at the gap can be made stronger. As a result of the above, it was possible to increase the conversion efficiency and reduce distortion during large amplitude operation.

〔発明の実施例〕[Embodiments of the invention]

以下、図面を用いてとの発明の一実施例につき詳細に説
明する。第3図はこの発明に係る一実施例の断面斜視図
である。高透磁率材料からなる複数の並設された磁極6
及び6′は端部がそれぞれ高透磁率材料の支持板12 
、12’を介して永久磁石7の両端に結合され、それぞ
れ例えば磁極6はN極に、又磁極6′はS極に磁化され
ている。なお図示されていないが磁極6.6′の他の端
部にも永久磁石7と支持板12 、12’を設けること
も可能である。
Hereinafter, one embodiment of the invention will be described in detail with reference to the drawings. FIG. 3 is a cross-sectional perspective view of one embodiment of the present invention. Multiple parallel magnetic poles 6 made of high magnetic permeability material
and 6' are support plates 12 whose ends are each made of a high magnetic permeability material.
, 12' are connected to both ends of the permanent magnet 7, and the magnetic pole 6 is magnetized to the north pole, and the magnetic pole 6' is magnetized to the south pole, respectively. Although not shown, it is also possible to provide the permanent magnet 7 and the support plates 12, 12' at the other ends of the magnetic poles 6, 6'.

一方振動板8は一部ウレタン等やわらかい材料からなる
エツジ9を介して枠体10により保持されている。振動
板8の横断面は図示したように、磁極6及び6′を縫う
ように凹凸に形成されており、ボイスコイル11は振動
板8の面上で隣り合った磁極6と6′の間に配置される
。第4図を用いて動作を説明する。図に示したように例
えば磁極6がN極に6′が8極に磁化されているとする
と、ボイスコイル付近の磁界は11−1と11−3では
図面左向きで、11−2と11−4では図面右向きにな
る。
On the other hand, the diaphragm 8 is partially held by a frame 10 via an edge 9 made of a soft material such as urethane. As shown in the figure, the cross section of the diaphragm 8 is formed in a concave and convex manner so as to weave through the magnetic poles 6 and 6', and the voice coil 11 is arranged between the adjacent magnetic poles 6 and 6' on the surface of the diaphragm 8. Placed. The operation will be explained using FIG. As shown in the figure, for example, if the magnetic pole 6 is magnetized to the N pole and the magnetic pole 6' is magnetized to the 8 pole, the magnetic field near the voice coil will be directed to the left in the drawing at 11-1 and 11-3, and 11-2 and 11- In 4, the drawing will face right.

従ってボイスコイル11−1°、 11−3と11−2
.11−4には反対向きの電流が淀れる様に接続すれば
、振動板は全てのボイスコイルによシ同一方向の駆動力
を受けることになる。ボイスコイルの結線方法の一例を
第5図に示す第5図は振動板の一例の展開図で、一点破
線の部分を折シたたむことによって第3図に示した振動
板8になる。ボイスコイル11は表裏二面からな!51
1−a及び11−bにおいてスルーホール処理又はリベ
ント等適宜な方法によシ表裏のボイスコイルの導通が取
られる。電気信号は11−0点と11−d点の間に加え
られる。この振動板は例えば金属箔をプラスチック板に
張シ付けた後、エツチングによって導通部分を形成する
という通常のプリント基板の製法と同様の方法によって
容易に作ることが出来る。
Therefore, voice coils 11-1°, 11-3 and 11-2
.. If the diaphragm 11-4 is connected so that the current in the opposite direction stagnates, the diaphragm will receive driving force from all the voice coils in the same direction. An example of a voice coil connection method is shown in FIG. 5. FIG. 5 is a developed view of an example of a diaphragm, and the diaphragm 8 shown in FIG. 3 is obtained by folding the portion indicated by a dotted line. Voice coil 11 has two sides, front and back! 51
At 1-a and 11-b, conduction between the front and back voice coils is established by an appropriate method such as through-hole processing or reventing. An electrical signal is applied between points 11-0 and 11-d. This diaphragm can be easily manufactured by a method similar to that used for manufacturing ordinary printed circuit boards, in which, for example, metal foil is pasted onto a plastic plate and then conductive parts are formed by etching.

〔発明の効果〕〔Effect of the invention〕

この実施例のような構造にすることによυ第1に振動板
が折シたたまれた構造なので、振動系のスチフネスを小
さくすることが出来るので低い周波数の再生が可能にな
る。第2に磁極の間隔を小さく出来るのでもれ磁束の少
ない磁気回路とすることが出来、変換効率を高くするこ
とが出来る。
By adopting the structure of this embodiment, firstly, since the diaphragm is folded, the stiffness of the vibration system can be reduced, making it possible to reproduce low frequencies. Second, since the spacing between the magnetic poles can be reduced, a magnetic circuit with less leakage magnetic flux can be achieved, and the conversion efficiency can be increased.

第3に、磁極の間隔を小さくしても振動板の許容される
振巾は磁極の間隔と無関係に大きくすることが出来、大
振巾に耐えるスピーカとすることが出来る。第4に従来
例のように、空気中で磁力線をねじ曲げる必要が無いの
で平行磁界の範囲を広く出来るのでこの点でも大振巾時
の歪を小さく出来る。第5にこの実施例では第3図に示
したように磁石7と図示しない反対側に置かれたもう一
個の磁石は同じ方向に磁化すれば良いので、スピーカを
組立てた後に磁化するのが容易である。従って前記実施
例にくらべて組立てが容易になる。第6に前記実施例に
くらべて振動板は厚いものを使うことが出来るので部品
としての取扱いが容易になる。さらに最低共振周波数を
下げることが出来るので低音再生帯域を拡げることがで
きる。
Thirdly, even if the spacing between the magnetic poles is reduced, the allowable amplitude of the diaphragm can be increased regardless of the spacing between the magnetic poles, making it possible to create a speaker that can withstand large amplitudes. Fourthly, unlike the conventional example, there is no need to twist the lines of magnetic force in the air, so the range of the parallel magnetic field can be widened, and in this respect too, distortion at large amplitudes can be reduced. Fifth, in this embodiment, as shown in FIG. 3, magnet 7 and another magnet placed on the opposite side (not shown) need only be magnetized in the same direction, making it easy to magnetize them after assembling the speaker. It is. Therefore, assembly is easier than in the previous embodiment. Sixth, since the diaphragm can be thicker than in the previous embodiment, it is easier to handle it as a component. Furthermore, since the lowest resonance frequency can be lowered, the bass reproduction band can be expanded.

〔発明の他の実施例、変形例、応用例〕振動板の断面形
状は第3図の様に折ジたたんだ形である必要はなく、第
6図のように波形であっても良い。この場合、ボイスコ
イル付近では振動板面は振動方向と平行であることが望
ましいが、(7) 第 変換効率が若干低下することを′設計的に許容すれば必
ずしも平行である必要はない。
[Other embodiments, modifications, and applications of the invention] The cross-sectional shape of the diaphragm does not need to be folded as shown in Figure 3, but may be wave-shaped as shown in Figure 6. . In this case, it is desirable that the diaphragm surface be parallel to the vibration direction in the vicinity of the voice coil, but it does not necessarily have to be parallel if (7) the design allows for a slight decrease in the conversion efficiency.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来例の断面斜視図、第2図は従来例の断面図
、第3図は本発明の断面斜視図、第4図は本発明の断面
図、第5図は本発明の振動板の展開図、第6図は本発明
のその他の実施例の断面図。 1・・・・・・[動板  2・・・ボイスコイル4・・
・・・・磁石     6,6′・・・磁極7・・・・
・・磁石     8・・・・・・振動板11・・・・
・・ホイスコイル 代理人弁理士  則 近 憲 佑(ほか1名)(8) 1図
Fig. 1 is a cross-sectional perspective view of the conventional example, Fig. 2 is a cross-sectional view of the conventional example, Fig. 3 is a cross-sectional perspective view of the present invention, Fig. 4 is a cross-sectional view of the present invention, and Fig. 5 is a vibration of the present invention. FIG. 6 is a developed view of the plate, and FIG. 6 is a sectional view of another embodiment of the present invention. 1...[Moving plate 2...Voice coil 4...
...Magnet 6,6'...Magnetic pole 7...
... Magnet 8 ... Vibration plate 11 ...
・・Patent attorney Noriyuki Chika (and 1 other person) representing Heuscoil (8) Figure 1

Claims (4)

【特許請求の範囲】[Claims] (1)振動板の全面にわたってボイスコイルを配置した
全面駆動型のスピーカにおいて、複数個の棒状の磁極を
その極性が交互に反対になるよう並設して磁気回路を構
成し、これら並設された磁極を縫うように断面波形の振
動板を配置し、ボイスコイルを前記相隣シ合う磁極の間
の振動板面に配したことを特徴とする動電型全面駆動ス
ピーカ。
(1) In a full-plane drive type speaker in which a voice coil is arranged over the entire surface of the diaphragm, a magnetic circuit is constructed by arranging a plurality of bar-shaped magnetic poles in parallel so that their polarities are alternately opposite, and these are arranged in parallel. 1. An electrodynamic full-drive speaker characterized in that a diaphragm having a corrugated cross section is arranged so as to weave through the magnetic poles, and a voice coil is arranged on the surface of the diaphragm between the adjacent magnetic poles.
(2)棒状の磁極の長手方向の一方の終端に永久磁石を
配したことを特徴とする特許請求の範囲第1項記載の動
電型全面駆動スピーカ。
(2) The electrodynamic full-plane drive speaker according to claim 1, characterized in that a permanent magnet is disposed at one longitudinal end of the rod-shaped magnetic pole.
(3)棒状の磁極の長手方向の両端に永久磁石を配した
ことを特徴とする特許請求の範囲第1項記載の動電型全
面駆動スピーカ。
(3) The electrodynamic full-plane drive speaker according to claim 1, characterized in that permanent magnets are arranged at both longitudinal ends of the rod-shaped magnetic pole.
(4)  振動板の磁極と磁極に狭まれた部分は振動板
の振動方向に平行であるこ・とを特徴とする特許請求の
範囲第1項記載の動電型全面駆動スピーカ。
(4) The electrodynamic full-plane drive speaker according to claim 1, wherein the magnetic poles of the diaphragm and the portion between the magnetic poles are parallel to the vibration direction of the diaphragm.
JP16502982A 1982-09-24 1982-09-24 Entirely dynamic driving speaker Pending JPS5955699A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16502982A JPS5955699A (en) 1982-09-24 1982-09-24 Entirely dynamic driving speaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16502982A JPS5955699A (en) 1982-09-24 1982-09-24 Entirely dynamic driving speaker

Publications (1)

Publication Number Publication Date
JPS5955699A true JPS5955699A (en) 1984-03-30

Family

ID=15804484

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16502982A Pending JPS5955699A (en) 1982-09-24 1982-09-24 Entirely dynamic driving speaker

Country Status (1)

Country Link
JP (1) JPS5955699A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2008135221A1 (en) * 2007-05-02 2008-11-13 Mundorf Eb Gmbh Membrane or membrane arrangement for an electrodynamic sound transducer, and loudspeaker comprising such a membrane or membrane arrangement
WO2010119488A1 (en) * 2009-04-15 2010-10-21 三菱電機エンジニアリング株式会社 Electromagnetic converter
WO2014134851A1 (en) * 2013-03-08 2014-09-12 Shandong Gettop Acoustic Co.,Ltd Motor for dynamic loudspeaker
WO2024033635A1 (en) * 2022-08-08 2024-02-15 Arya Audio Labs Ltd Electroacoustic transducer

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2008135221A1 (en) * 2007-05-02 2008-11-13 Mundorf Eb Gmbh Membrane or membrane arrangement for an electrodynamic sound transducer, and loudspeaker comprising such a membrane or membrane arrangement
US8208678B2 (en) 2007-05-02 2012-06-26 Mundorf Eb Gmbh Membrane or membrane configuration for an electrodynamic sound transducer, and loudspeaker comprising such a membrane or membrane configuration
WO2010119488A1 (en) * 2009-04-15 2010-10-21 三菱電機エンジニアリング株式会社 Electromagnetic converter
JP2010252028A (en) * 2009-04-15 2010-11-04 Mitsubishi Electric Engineering Co Ltd Electromagnetic converter
WO2014134851A1 (en) * 2013-03-08 2014-09-12 Shandong Gettop Acoustic Co.,Ltd Motor for dynamic loudspeaker
WO2024033635A1 (en) * 2022-08-08 2024-02-15 Arya Audio Labs Ltd Electroacoustic transducer

Similar Documents

Publication Publication Date Title
US3997739A (en) Electrodynamic type electroacoustic transducer
US4550228A (en) Ribbon speaker system
US5901235A (en) Enhanced efficiency planar transducers
US3141071A (en) Full range electroacoustic transducers
US3164686A (en) Electrodynamic transducer
US5003610A (en) Whole surface driven speaker
US4276449A (en) Speaker or microphone having corrugated diaphragm with conductors thereon
CN114286266B (en) Speaker and electronic device
US6810126B2 (en) Planar magnetic transducer
US9641938B2 (en) Electro-acoustic transducer with radiating acoustic seal and stacked magnetic circuit assembly
CN210157382U (en) Speaker assembly and magnetic assembly
JP5112159B2 (en) Electromagnetic electroacoustic transducer
CN109413553B (en) Equal magnetic loudspeaker
US3922504A (en) Electroacoustic transducer
EP0077228A2 (en) Electroacoustic transducer
JPS5955699A (en) Entirely dynamic driving speaker
US7088837B2 (en) High efficiency planar magnetic transducer with angled magnet structure
JP2003032787A (en) Electric acoustic transducer
US10499158B2 (en) Electro-acoustic transducer with radiating acoustic seal and stacked magnetic circuit assembly
JPS6247398B2 (en)
CN209949430U (en) Moving coil flat plate composite electroacoustic transducer
JP2003102088A (en) Planar acoustic transducer
US6868166B1 (en) Chord-like vibration loudspeaker
CN209949405U (en) Moving coil flat plate composite electroacoustic transducer
CN209748803U (en) Equal magnetic loudspeaker