JPS607880B2 - Composite speaker - Google Patents

Composite speaker

Info

Publication number
JPS607880B2
JPS607880B2 JP15356577A JP15356577A JPS607880B2 JP S607880 B2 JPS607880 B2 JP S607880B2 JP 15356577 A JP15356577 A JP 15356577A JP 15356577 A JP15356577 A JP 15356577A JP S607880 B2 JPS607880 B2 JP S607880B2
Authority
JP
Japan
Prior art keywords
vibrating membrane
coil conductor
electrode layer
full
piezoelectric film
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.)
Expired
Application number
JP15356577A
Other languages
Japanese (ja)
Other versions
JPS5486320A (en
Inventor
欧太郎 安東
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.)
Olympus Corp
Original Assignee
Olympus Optical 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 Olympus Optical Co Ltd filed Critical Olympus Optical Co Ltd
Priority to JP15356577A priority Critical patent/JPS607880B2/en
Priority to US05/970,150 priority patent/US4242541A/en
Publication of JPS5486320A publication Critical patent/JPS5486320A/en
Publication of JPS607880B2 publication Critical patent/JPS607880B2/en
Expired 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
    • H04R23/00Transducers other than those covered by groups H04R9/00 - H04R21/00
    • H04R23/02Transducers using more than one principle simultaneously

Description

【発明の詳細な説明】 本発明は圧電フィルムを用いた平面スピーカに関するも
のである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a flat speaker using a piezoelectric film.

従来から振動板全面を駆動するようにする平面スピーが
こ関しては種々のものが提案、実施されている。
Conventionally, various types of flat speakers that drive the entire surface of the diaphragm have been proposed and implemented.

例えば特公昭47一12432、実関昭52−4592
2号公報等には高分子圧電性フィルムを用いた圧電スピ
ーカについて、特開昭47一13474、実関昭51−
100536号公報等には特殊なコイル形状を採用して
全面駆動を実現するようにした勤雷スピーカについて記
載されている。第1図は従来の全面駆動勤亀スピーカの
構造の一例を示すものであり、振動膜1をはさんで多数
の棒状の磁石2を配置したものである。振動膜1をはさ
んで対向する磁石は同極が対向するように置かれ、かつ
隣り合う磁石は異極が対向するように置かれていて、振
動膜1と平行な磁界が形成されている。振動膜1の上に
はこの磁界と直交する電流が交互に逆向きに流れるよう
にコイル導体3を蒸着等の手段により設け、このコイル
導体3に電流を流した時この電流と上記磁界との間に働
く力が振動膜1全面を同方向に駆動するようにする。こ
のコイル導体3に音声電流を流すようにすれば振動膜1
の振動によって音が再生されるわけである。次に第2図
に従来の圧電スピーカの構造の一例を示す。基板4の上
に押圧用の弾性体層5を形成し、この上に曲面状に高分
子圧電フィルム6を張架してある。この圧電フィルム6
の両面には蒸着等の手段により電極面が形成してあり、
この電極間に音声信号電圧を印加するとフィルム6は矢
印方向に伸縮し、弾性体層5の圧力によりこれと直角方
向に振動することになり、音が再生される。これ等のス
ピーカは何れも振動面がほぼ全面にわたり同位相で駆動
されるために従来一般的なコーンスピーカに比べて歪が
少ない等の利点を有している。しかし第1図に示した動
電型のスピーカにおいてはその構造上十分大きな磁束密
度を得ることが困難であり、また第2図に示した圧電型
のスピーかこおいては十分大きな圧電率を示す圧電材料
が得られていないため、いずれも効率が低かった。また
これ等のスピーカはテンションを与えて張架した振動膜
を用いているため大振幅がとれず、特に低音の再生が困
難であるという欠点があった。例えば第1図に示した勤
竜型のスピーカの場合振動膜1は常に矢印方向に張力を
受けており、そのためにこれに直角な振動方向への振動
を制限する力が働き、効率を下げると共に大振幅を不可
能にしていた。本発明の目的は動電型の全面駆動スピー
カと圧電スピーカの複合された構造を採用して、これ等
の長所を生かしながら高い効率をもち、十分な低音再生
が可能なスピーカを提供することにある。
For example, Tokuko Sho 47-12432, Jitoseki Sho 52-4592
Publications No. 2, etc. describe piezoelectric speakers using polymer piezoelectric films, JP-A No. 47-13474, Jitsugyo-Sho 51-
Publication No. 100536 and the like describe a lightning-operated speaker that employs a special coil shape to achieve full-surface drive. FIG. 1 shows an example of the structure of a conventional full-plane drive speaker, in which a large number of rod-shaped magnets 2 are arranged with a vibrating membrane 1 in between. Magnets facing each other across the vibrating membrane 1 are placed so that the same poles face each other, and adjacent magnets are placed so that different poles face each other, so that a magnetic field parallel to the vibrating membrane 1 is formed. . A coil conductor 3 is provided on the vibrating membrane 1 by means such as vapor deposition so that currents perpendicular to this magnetic field alternately flow in opposite directions, and when a current is passed through the coil conductor 3, the interaction between this current and the magnetic field is The force acting between them drives the entire surface of the vibrating membrane 1 in the same direction. If an audio current is passed through this coil conductor 3, the diaphragm 1
Sound is reproduced by the vibrations of the Next, FIG. 2 shows an example of the structure of a conventional piezoelectric speaker. A pressing elastic layer 5 is formed on the substrate 4, and a polymer piezoelectric film 6 is stretched over this in a curved shape. This piezoelectric film 6
Electrode surfaces are formed on both sides by means such as vapor deposition,
When an audio signal voltage is applied between these electrodes, the film 6 expands and contracts in the direction of the arrow, and due to the pressure of the elastic layer 5 vibrates in a direction perpendicular to this, thereby reproducing sound. All of these speakers have advantages such as less distortion than conventional cone speakers because their vibrating surfaces are driven in the same phase over almost the entire surface. However, in the electrodynamic type speaker shown in Figure 1, it is difficult to obtain a sufficiently large magnetic flux density due to its structure, and in the piezoelectric type speaker shown in Figure 2, it is difficult to obtain a sufficiently large piezoelectric constant. The efficiency of both methods was low because no piezoelectric material was available. Furthermore, since these speakers use a vibrating membrane stretched under tension, they cannot produce large amplitudes, making it particularly difficult to reproduce bass sounds. For example, in the case of the Kinryu-type speaker shown in Figure 1, the diaphragm 1 is always under tension in the direction of the arrow, and as a result, a force acts to limit vibration in the direction of vibration perpendicular to this, reducing efficiency and This made large amplitude impossible. The purpose of the present invention is to provide a speaker that employs a composite structure of an electrodynamic full-drive speaker and a piezoelectric speaker, has high efficiency while taking advantage of these advantages, and is capable of reproducing sufficient bass. be.

本発明は高分子圧電フィルムを含む振動膜の少なくとも
片面にこの振動膜と一体となり、平面コイルとして作用
するコイル導体層を設け、さらに上記振動膜を構成する
圧電フィルムを伸張および/または収縮させるようにこ
のフィルムに電界を与える手段を設け、さらに上記コイ
ル導体層に流した電流との相互作用により振動膜を振動
させるような磁界を形成する磁気装置を設けたことを特
徴とするものである。以下図面につき本発明を詳細に説
明する。
The present invention provides a coil conductor layer that is integrated with the vibrating membrane and acts as a planar coil on at least one side of the vibrating membrane including a polymeric piezoelectric film, and further extends and/or contracts the piezoelectric film constituting the vibrating membrane. The present invention is characterized in that a means for applying an electric field to the film is provided, and a magnetic device is further provided for forming a magnetic field that vibrates the diaphragm by interaction with the current flowing through the coil conductor layer. The invention will be explained in detail below with reference to the drawings.

第3図は本発明による全面駆動型スピーカの一実施例を
示す断面図である。
FIG. 3 is a sectional view showing an embodiment of a full-plane drive type speaker according to the present invention.

振動膜7はポリフッ化ビニリデン(PVDF)等の薄膜
から成る高分子圧電フィルム8と、この圧電性フィルム
の片面に蒸着「貼付等の手段により形成した全面電極層
9と、圧電性フィルムの他面に同様な方法で形成したジ
グザグ状のコイル導体層10とから成っている。この振
動膜7の斜視図を第4図に示した。振動膜7はフレーム
11によっ張架されている。この振動膜の構造以外は第
1図で説明した従来の全面駆動動電型スピーカと同様な
構造を持ち、上記振動膜7をはさんで図示するように対
向して置かれた穣磁石12と、この榛磁石12を支える
と同時に磁気回路の一部を形成する多数の関口13を有
する磁性板14とから成っている。これ等の磁気回路に
よって振動膜7に平行で、かつコイル導体10を流れる
電流に直交する磁界が形成されることも第1図の従釆例
と同様である。第4図は振動膜7の斜視図とともに、こ
の振動膜への信号電圧の供給法も示している。
The vibrating membrane 7 includes a polymer piezoelectric film 8 made of a thin film such as polyvinylidene fluoride (PVDF), a full-surface electrode layer 9 formed on one side of this piezoelectric film by means such as vapor deposition or pasting, and the other side of the piezoelectric film. and a zigzag-shaped coil conductor layer 10 formed by a similar method.A perspective view of this vibrating membrane 7 is shown in FIG. 4.The vibrating membrane 7 is stretched by a frame 11. Other than the structure of the diaphragm, it has the same structure as the conventional full-plane drive electrodynamic speaker explained in FIG. It consists of a magnetic plate 14 having a large number of gates 13 that support this magnet 12 and at the same time form part of a magnetic circuit.These magnetic circuits allow the flow to flow parallel to the diaphragm 7 and through the coil conductor 10. The formation of a magnetic field orthogonal to the current is also similar to the secondary example of Fig. 1. Fig. 4 shows a perspective view of the vibrating membrane 7, as well as a method of supplying a signal voltage to the vibrating membrane.

コイル導体1川こは低インピーダンス信号源からの信号
電圧を供給して、コイル導体1川こ比較的大きな信号電
流が流れるようにしている。この電流と上記の磁界との
間に働く力によって振動膜7が信号に応じて振動する。
さらに本発明によって、電極層9とコイル導体層10と
の間には音声信号を全波整流した電圧、すなわち音声信
号電圧の絶対値を高インピーダンス信号源から加え、電
極層9とコイル導体層10との間に信号電圧の絶対値に
比例する電圧がかかるようにする。この時電圧の極性は
電圧がかかった時圧電フィルム8が伸張する様に選択す
る。このようにすると圧電フィルム8は信号電圧がかか
ると矢印A方向、すなわちフィルム面方向に信号電圧の
大きさに応じて伸び、振動膜7、フィルム8が面と直角
方向、すなわち矢印B向に振動するのをフィルム8の張
力によって妨げることが少なくなる。なお圧電フィルム
8の伸びの量は電圧値の選択によって適当な値に選ぶこ
とができる。上述のように信号電圧をコイル導体10、
電極層9に加えるには例えばトランス15の一次側端子
16に音声信号増幅器からの出力を加え、トランスの2
次側の低インピーダンス端子17,18をコイル導体1
0の端子21,22に接続し、トランス2次側の高イン
ピーダンス端子19,20の出力をダイオード23,2
4で全波整流して電極層9に加えればよい。
The coil conductor 1 is supplied with a signal voltage from a low impedance signal source so that a relatively large signal current flows through the coil conductor 1. The force acting between this current and the magnetic field causes the vibrating membrane 7 to vibrate in accordance with the signal.
Furthermore, according to the present invention, a voltage obtained by full-wave rectification of the audio signal, that is, the absolute value of the audio signal voltage is applied from a high impedance signal source between the electrode layer 9 and the coil conductor layer 10. A voltage proportional to the absolute value of the signal voltage is applied between the two. At this time, the polarity of the voltage is selected so that the piezoelectric film 8 expands when the voltage is applied. In this way, when a signal voltage is applied, the piezoelectric film 8 expands in the direction of arrow A, that is, in the direction of the film surface, depending on the magnitude of the signal voltage, and the vibrating membrane 7 and film 8 vibrate in a direction perpendicular to the surface, that is, in the direction of arrow B. The tension of the film 8 is less likely to impede this process. Note that the amount of elongation of the piezoelectric film 8 can be selected to an appropriate value by selecting the voltage value. As mentioned above, the signal voltage is applied to the coil conductor 10,
To add to the electrode layer 9, for example, add the output from the audio signal amplifier to the primary terminal 16 of the transformer 15, and
Connect the next low impedance terminals 17 and 18 to the coil conductor 1.
0 terminals 21 and 22, and the outputs of the high impedance terminals 19 and 20 on the secondary side of the transformer are connected to the diodes 23 and 2.
It is sufficient to perform full-wave rectification in step 4 and add it to the electrode layer 9.

ダイオード23,24の樋性、トランスの巻線比等は上
述したようにフィルム8の伸びの量、方向が適正となる
ように選ぶ。なお低インピーダンス端子17,18は両
者共高インピーダンス端子19,20の中点に近い位置
から取り出して、電極層9とコイル導体層10とにかか
る電圧がほぼ信号電圧の絶対値に比例したものとなるよ
うにしている。しかし厳密にはコイル導体層10の電位
は導体の位置によって異なり、例えば電極層9とコイル
導体10の一方の端部21とにかかる電圧をe,、他の
端部22にかかる電圧をe2とすると、e,とe2との
間には若干の差がある。しかしe2〜e,《一e,,e
2であるので、このことは大した問題とはならない。又
ダイオード23,24による順方向電圧ドロップ等の影
響も電極層9とコイル導体層10との間にかかる電圧の
大きさと比べれば特に問題ではない。第5図に示すもの
は別の信号電圧供給法であり、第4図に示したものとほ
ぼ同様なものであるがコイル導体10の両端21,22
に供給する電圧をトランス1次側16′から取っている
点が異なる。
The trough properties of the diodes 23 and 24, the winding ratio of the transformer, etc. are selected so that the amount and direction of elongation of the film 8 are appropriate, as described above. Note that the low impedance terminals 17 and 18 are both taken out from a position close to the midpoint of the high impedance terminals 19 and 20, and the voltage applied to the electrode layer 9 and the coil conductor layer 10 is approximately proportional to the absolute value of the signal voltage. I'm trying to make it happen. However, strictly speaking, the potential of the coil conductor layer 10 differs depending on the position of the conductor. For example, the voltage applied to the electrode layer 9 and one end 21 of the coil conductor 10 is e, and the voltage applied to the other end 22 is e2. Then, there is a slight difference between e and e2. However, e2~e,《1e,,e
2, so this is not a big problem. Further, the influence of forward voltage drop caused by the diodes 23 and 24 is not a particular problem when compared with the magnitude of the voltage applied between the electrode layer 9 and the coil conductor layer 10. What is shown in FIG. 5 is another signal voltage supply method, which is almost the same as that shown in FIG.
The difference is that the voltage supplied to the transformer is taken from the transformer primary side 16'.

符号25はトランス2次側センタータップを示し、第4
図に対応する部分には同じ符号にダッシュをつけて示し
ている。他にもトランスを用いずに、コイル導体1川こ
電流を流すための増幅器と、コイル導体層10と電極層
9との間に電圧を印加する増幅器とを別個に設けるよう
にしてもよい。
Reference numeral 25 indicates the center tap on the secondary side of the transformer, and the fourth
Parts corresponding to the figures are indicated by the same reference numerals with a dash added. Alternatively, an amplifier for passing a current through the coil conductor and an amplifier for applying a voltage between the coil conductor layer 10 and the electrode layer 9 may be separately provided without using a transformer.

第6図aは本発明によるスピーカの他の実施例を示す断
面図である。
FIG. 6a is a sectional view showing another embodiment of the speaker according to the present invention.

この実施例は第3図〜第5図で説明したものと同じ考え
方に基〈ものである。ただし振動膜の形状は上述した実
施例では方形状であったのに対し、この実施例では円形
状となっている。振動膜26はやはり圧電性フィルム2
7、全面電極層28、コイル導体層29とから成ってい
る。振動膜26は円環状のフレーム30によって張架さ
れ、振動膜26をはさんで第6図bに示すように円環状
磁石31,32が同D円状に並べられ、同極が振動膜2
6をはさんで対向するように、かつ隣り合う磁石は逆極
性となるようにしてある。なおこれ等の磁石は多数の関
口33をもつ磁性体の円板34によって保持され、磁気
回路を形成している。第7図aには第6図と同じ円板状
の振動膜を使用した例の断面図を示し、第7図bにはこ
の実施例に使用する磁石の上面図を示している。第7図
の実施例は第6図のものと概ね同じものであるが、磁石
として同心円状のものを複数個用いる代わりに同○円状
に着磁した2枚の円盤状磁石37,38を用いている点
が異なっている。なお、磁石37,38には音響放射用
の関口39が多数設けるようにする。第8図、第9図は
何れも第6図又は第7図の実施例に使用するコイル導体
層29のパターンの上面図である。
This embodiment is based on the same concept as that explained in FIGS. 3 to 5. However, while the shape of the vibrating membrane was square in the above embodiment, it is circular in this embodiment. The vibrating membrane 26 is also the piezoelectric film 2
7, a full-surface electrode layer 28 and a coil conductor layer 29. The vibrating membrane 26 is stretched by an annular frame 30, and as shown in FIG.
6, and adjacent magnets have opposite polarities. Note that these magnets are held by a magnetic disc 34 having a large number of gates 33, forming a magnetic circuit. FIG. 7a shows a sectional view of an example using the same disc-shaped vibrating membrane as in FIG. 6, and FIG. 7b shows a top view of a magnet used in this embodiment. The embodiment shown in FIG. 7 is almost the same as that shown in FIG. 6, but instead of using a plurality of concentric magnets, two disc-shaped magnets 37 and 38 magnetized in the same circle are used. They differ in the way they are used. Note that the magnets 37 and 38 are provided with a large number of exits 39 for acoustic radiation. 8 and 9 are top views of the pattern of the coil conductor layer 29 used in the embodiment of FIG. 6 or 7. FIG.

何れのパターンにおいても同心円状に電粒が流れ、隣り
合う同○円状の電流は逆向きとなるようにしてあること
がわかる。上述の第6図、第7図何れに示した構成にお
いても磁石31,32,37,38によって形成される
磁界は振動板26に平行でかつコイル導体層29を流れ
る電流に直交するようになり、コイル導体層29に信号
電流が流れた時振動膜26を信号に応じて振動させるこ
とは第3図に示す実施例と同様である。したがって第4
及び第5図に示した方法で、あるいは別に説明した方法
でこれ等の実施例によるスピーカを駆動することができ
る。第10図に示すものはコイル導体層を振動膜の両面
に設けたものであり、振動膜の形状は方形状でもよいし
円形状でもよい。
It can be seen that in both patterns, the electric particles flow concentrically, and the currents in adjacent circles are in opposite directions. In both the configurations shown in FIGS. 6 and 7 above, the magnetic field formed by the magnets 31, 32, 37, and 38 is parallel to the diaphragm 26 and perpendicular to the current flowing through the coil conductor layer 29. Similarly to the embodiment shown in FIG. 3, when a signal current flows through the coil conductor layer 29, the vibrating membrane 26 is vibrated in accordance with the signal. Therefore, the fourth
The loudspeaker according to these embodiments can be driven in the manner shown in FIG. 5, or in the manner described elsewhere. The device shown in FIG. 10 has coil conductor layers provided on both sides of a vibrating membrane, and the vibrating membrane may have a rectangular shape or a circular shape.

この例では全面電極層40をはさんで2枚の圧電フィル
ム41,42を設け、さらにコイル導体層43,44を
設けたものである。駆動方法としてはコイル導体層43
,44を流れる電流の向きが同じとなるように、すなわ
ちコイル導体43,44を流れる電流と磁石による磁界
との相互作用が同方向となるようにコイル導体43,4
4を直列あるいは並列に接続してやればよい。又コイル
導体層43,44と全面電極層40との間には信号電圧
の絶対値に比例する電圧を圧軍フィルム41,42が伸
びる向きに印加することは上述の各実施例と同機である
。なお本発明は上述した実施例に限られるものではなく
、例えばコイル導体層、電極層のパターン、磁石の配列
等はコイル導体に信号電流を流した時に、それに応じて
圧電フィルムを振動させる力と圧電フィルムを伸張させ
る力とが働けばよいのであり、別の適当な構成とするこ
とができる。
In this example, two piezoelectric films 41 and 42 are provided with a full-surface electrode layer 40 in between, and coil conductor layers 43 and 44 are further provided. As a driving method, the coil conductor layer 43
, 44 so that the direction of the current flowing through the coil conductors 43, 44 is the same, that is, the interaction between the current flowing through the coil conductors 43, 44 and the magnetic field generated by the magnet is in the same direction.
4 can be connected in series or in parallel. Also, in the same manner as in the above embodiments, a voltage proportional to the absolute value of the signal voltage is applied between the coil conductor layers 43, 44 and the entire surface electrode layer 40 in the direction in which the compression films 41, 42 extend. Note that the present invention is not limited to the above-mentioned embodiments; for example, the coil conductor layer, the pattern of the electrode layer, the arrangement of the magnets, etc. can be used to create a force that vibrates the piezoelectric film in response to a signal current flowing through the coil conductor. It is sufficient that a force that stretches the piezoelectric film is applied, and other suitable configurations can be used.

例えばコイル導体を流れる電流と適当な相互作用をもつ
ような磁界が形成されるなら磁石は振動面の片側に置く
ようにしてもよいし、振動膜の構造もさらに多層のもの
とすることもできる。又コイルとして作用する導体層を
圧電フィルムに電圧を印加する電極と兼用させずに、各
々専用のコイル導体層と電極層を設けてもよい。さらに
上述した実施例では全て振動膜を張架した状態で用いて
無信号時に比べて信号のある時の方が振動膜が伸張する
ようにしたが、信号によって振動膜が収縮するようにし
てこれによって振動が促進されるような構造とすること
もできる。さらに振動膜の形としては円形、方形とは限
らず例えば楕円形とすることもできる。本発明によれば
動電型及び圧電型という全く異なる原理を組み合わせて
用いることにより、勤電型の平面駆動スピーカの低歪、
平坦な周波数特性等の長所はそのままで、従来の膜張架
方式のものに比べて効率が高く、振動振幅が大きくとれ
、比較的小型で低域再生が可能なスピーカが得られる。
For example, if a magnetic field is formed that has an appropriate interaction with the current flowing through the coil conductor, the magnet may be placed on one side of the vibrating surface, or the structure of the vibrating membrane may be made of more layers. . Further, the conductor layer acting as a coil may not also be used as an electrode for applying a voltage to the piezoelectric film, but a dedicated coil conductor layer and electrode layer may be provided respectively. Furthermore, in all of the above-mentioned embodiments, the diaphragm was used in a stretched state so that the diaphragm expanded more when there was a signal than when there was no signal. It is also possible to have a structure in which vibration is promoted by. Furthermore, the shape of the vibrating membrane is not limited to circular or rectangular shapes, and may be, for example, elliptical. According to the present invention, by combining the completely different principles of electrodynamic type and piezoelectric type, the distortion of the electrodynamic type planar drive speaker can be reduced.
While maintaining its advantages such as flat frequency characteristics, it is possible to obtain a speaker that is more efficient than conventional membrane-mounted systems, has a large vibration amplitude, is relatively compact, and is capable of reproducing low frequencies.

【図面の簡単な説明】 第1図は従釆の全面駆動勤電スピーカの構造を示す断面
図、第2図は従来の圧電スピーカの一例の構造を示す断
面図、第3図は本発明の全面駆動型スピーカの一実施例
の構造を示す断面図、第4図は本発明による全面駆動型
スピーカの駆動法を示す線図、第5図は同じく駆動法の
別の実施例を示す線図、第6図aは本発明による全面駆
動スピーカの別の実施例を直径方向に切って示す斜示図
、bはこの実施例に使用される磁石の配列を示す上面図
、第7図aは本発明のさらに別の実施例の構成を直径方
向に切って示す斜視図、bはこの実施例に使用される磁
石の上面図、第8図、第9図は第6図、第7図の実施例
に用いる振動膜のコイル導電層パターンを示す上面図、
第10図は本発明のさらに別の実施例に用いる振動膜の
構成を示す断面図である。 1,7,26・・・・・・振動膜、2,12,31,3
2・・・・・・磁石、3,10,29,43,44..
・..・コイル導電層、8,27・・・・・・圧電フィ
ルム、9,28,40・・・・・・全面電極層、11,
30..・..・フレーム、13,33,39…・・・
開□、14,34......磁性板、15,i5′…
…トランス、23,23′,24,24′……ダイオー
ド。 第1図 第2図 第3.図 第14図 第5図 第10図 第6図 第7図 第8図 第9図
[Brief Description of the Drawings] Fig. 1 is a cross-sectional view showing the structure of a slave full-plane drive power speaker, Fig. 2 is a cross-sectional view showing the structure of an example of a conventional piezoelectric speaker, and Fig. 3 is a cross-sectional view showing the structure of an example of a conventional piezoelectric speaker. 4 is a cross-sectional view showing the structure of an embodiment of a full-surface drive type speaker, FIG. 4 is a diagram showing a driving method of the full surface drive type speaker according to the present invention, and FIG. 5 is a diagram showing another embodiment of the driving method. , FIG. 6a is a diametrically cut perspective view of another embodiment of a full-plane drive speaker according to the present invention, FIG. 6b is a top view showing the arrangement of magnets used in this embodiment, and FIG. A perspective view showing the configuration of yet another embodiment of the present invention cut in the diametrical direction, b is a top view of the magnet used in this embodiment, and FIGS. 8 and 9 are the same as those in FIGS. 6 and 7. A top view showing a coil conductive layer pattern of a vibrating membrane used in an example,
FIG. 10 is a sectional view showing the structure of a vibrating membrane used in yet another embodiment of the present invention. 1, 7, 26... Vibration membrane, 2, 12, 31, 3
2... Magnet, 3, 10, 29, 43, 44. ..
・.. ..・Coil conductive layer, 8, 27...Piezoelectric film, 9, 28, 40...Full surface electrode layer, 11,
30. ..・.. ..・Frame, 13, 33, 39...
Open □, 14, 34. .. .. .. .. .. Magnetic plate, 15, i5'...
...Transformer, 23, 23', 24, 24'...Diode. Figure 1 Figure 2 Figure 3. Figure 14 Figure 5 Figure 10 Figure 6 Figure 7 Figure 8 Figure 9

Claims (1)

【特許請求の範囲】 1 高分子圧電フイルムを含む振動膜の少なくとも片面
にこの振動膜と一体となり、平面コイルとして作用する
コイル導体層を設け、さらに上記振動膜を構成する圧電
フイルムを伸張および/または収縮させるようにこのフ
イルムに電界を与える手段を設け、さらに上記コイル導
体層に流した電流との相互作用により振動膜を振動させ
るような磁界を形成する磁気装置を設けたことを特徴と
する圧電方式と動電方式の複合方式スピーカ。 2 高分子圧電フイルムの片面に平面コイルとして作用
すると共に電極層としても作用するコイル導体層、他面
に全面電極層を設けて形成した振動膜を具え、この振動
膜をはさんで同極同士を対向させ、交互に逆極性が並ぶ
ように配置した棒状磁石の磁気装置によって振動膜にほ
ぼ平行な磁界を形成するようにし、上記コイル導体層を
交互に反対向きの電流が流れる平行部分を持つものとし
たことを特徴とする特許請求の範囲1記載の複合方式ス
ピーカ。 3 高分子圧電フイルムの片面に平面コイルとして作用
すると共に電極層としても作用するコイル導体層、他面
に全面電極層を設けて形成した振動膜を具え、この振動
膜をはさんで同極同士を対向させ、かつ交互に逆極性と
なるように同心円状に配置した複数の円環状磁石、又は
振動膜をはさんで同極同士が対向し、かつ同心円状に交
互に逆極性に着磁された2枚の円盤状磁石から成る磁気
装置によって振動膜にほぼ平行な磁界を形成するように
し、上記コイル導体層が交互に反対向きの電流が流れる
ように構成した同心円状のコイル導体層であることを特
徴とする特許請求の範囲1記載の複合方式スピーカ。 4 高分子圧電フイルムの片面に平面コイルとして作用
すると共に電極層としても作用するコイル導体層、他面
に全面電極層を設けて形成した振動膜と、この振動膜に
ほぼ平行な磁界を形成する磁気装置とを具え、上記コイ
ル導体に低インピーダンス信号源からの音声電流を流し
て全面駆動方式の動電型スピーカとして動作させると共
に、上記コイル導体と全面電極層との間に音声信号の絶
対値に応じて上記振動膜が伸縮するように全波整流され
た音声信号を加えるように構成したことを特徴とする複
合方式スピーカ。
[Scope of Claims] 1. A coil conductor layer is provided on at least one side of a vibrating membrane including a polymeric piezoelectric film and is integrated with the vibrating membrane and acts as a planar coil, and furthermore, the piezoelectric film constituting the vibrating membrane is stretched and/or Alternatively, a means for applying an electric field to the film so as to cause it to contract is provided, and a magnetic device is further provided for forming a magnetic field that causes the vibrating membrane to vibrate through interaction with the current passed through the coil conductor layer. A composite piezoelectric and electrodynamic speaker. 2 A vibrating membrane formed by providing a coil conductor layer that acts as a planar coil and also an electrode layer on one side of a polymeric piezoelectric film, and a full-scale electrode layer on the other side, and connecting the same polarity with each other with this vibrating membrane in between. A magnetic device of bar-shaped magnets arranged so that opposite polarities are arranged to form a nearly parallel magnetic field to the vibrating membrane, and the coil conductor layer has parallel portions through which currents in opposite directions alternately flow. 2. A composite speaker according to claim 1, characterized in that: 3 A vibrating membrane formed by providing a coil conductor layer that acts as a planar coil and also an electrode layer on one side of a polymer piezoelectric film, and a full-scale electrode layer on the other side, and connecting the same polarity with each other with this vibrating membrane in between. A plurality of annular magnets arranged concentrically so that they face each other and alternately have opposite polarities, or magnets with the same polarity facing each other across a vibrating membrane and magnetized concentrically and alternately with opposite polarities. A magnetic device consisting of two disk-shaped magnets forms a magnetic field substantially parallel to the diaphragm, and the coil conductor layers are concentric coil conductor layers configured so that currents in opposite directions alternately flow through the coil conductor layers. A composite speaker according to claim 1, characterized in that: 4 A vibrating membrane formed by providing a coil conductor layer that acts as a planar coil and also an electrode layer on one side of a polymer piezoelectric film, and a full-scale electrode layer on the other side, and a magnetic field that is almost parallel to this vibrating membrane. A magnetic device is provided, in which an audio current from a low-impedance signal source is passed through the coil conductor to operate as a full-surface drive type electrodynamic speaker, and an absolute value of the audio signal is provided between the coil conductor and the full-surface electrode layer. 1. A composite system speaker characterized in that a full-wave rectified audio signal is added so that the diaphragm expands and contracts in response to the vibration.
JP15356577A 1977-12-22 1977-12-22 Composite speaker Expired JPS607880B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP15356577A JPS607880B2 (en) 1977-12-22 1977-12-22 Composite speaker
US05/970,150 US4242541A (en) 1977-12-22 1978-12-18 Composite type acoustic transducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15356577A JPS607880B2 (en) 1977-12-22 1977-12-22 Composite speaker

Publications (2)

Publication Number Publication Date
JPS5486320A JPS5486320A (en) 1979-07-09
JPS607880B2 true JPS607880B2 (en) 1985-02-27

Family

ID=15565266

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15356577A Expired JPS607880B2 (en) 1977-12-22 1977-12-22 Composite speaker

Country Status (1)

Country Link
JP (1) JPS607880B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20040029872A (en) * 2002-10-02 2004-04-08 (주) 모토조이 Thin Film Speaker

Also Published As

Publication number Publication date
JPS5486320A (en) 1979-07-09

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