JPS6150439B2 - - Google Patents
Info
- Publication number
- JPS6150439B2 JPS6150439B2 JP7443478A JP7443478A JPS6150439B2 JP S6150439 B2 JPS6150439 B2 JP S6150439B2 JP 7443478 A JP7443478 A JP 7443478A JP 7443478 A JP7443478 A JP 7443478A JP S6150439 B2 JPS6150439 B2 JP S6150439B2
- Authority
- JP
- Japan
- Prior art keywords
- base material
- coil
- electromagnetic
- film
- transducer
- 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
Links
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; ELECTRIC HEARING AIDS; PUBLIC ADDRESS SYSTEMS
- H04R11/00—Transducers of moving-armature or moving-core type
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Acoustics & Sound (AREA)
- Signal Processing (AREA)
- Electrostatic, Electromagnetic, Magneto- Strictive, And Variable-Resistance Transducers (AREA)
Description
産業上の利用分野
本発明は、空気や液体やレコード等の振動の機
械エネルギーと電気エネルギーとのエネルギー変
換を行うトランスデユーサの改良に係り、変換の
応答性、感度、直線性、ダイナミツクレンジ等の
優れたトランスデユーサを得ることを目的とす
る。
従来の技術
従来、振動の機械エネルギーと電気エネルギー
とのエネルギー変換を行うトランスデユーサとし
て、磁場中で電磁コイルを振動させて電磁誘導起
電力を得るムービングコイル型のピツクアツプ
や、電磁コイル近傍で永久磁石を振動させて電磁
誘導起電力を得るムービングマグネツト型のピツ
クアツプがレコード用として用いられている。ま
た、電極近傍でエレクトレツトフイルムを振動さ
せ、静電誘導起電力を得る方式がマイクロホンと
して利用され、スピーカ用には、永久磁石の近傍
で電磁コイルに音声信号電流を通電して電磁コイ
ルを振動させる方式や、電極に音声信号電圧を印
加して、近傍に設けたプラスチツクフイルムを静
電力で振動させる方式が実用化されている。
発明が解決しようとする問題点
しかしながら、いずれの場合でも応答性と出
力・効率の両方とも優れたものは得られていな
い。即ち、ムービングコイル型ピツクアツプは応
答性は比較的良いが、出力が極めて低いため専用
の高価なトランスや低ノイズアンプを必要とし、
ムービングマグネツト型ピツクアツプは出力は高
いが、重い永久磁石を振動させるので応答性が悪
く、高音の忠実再生が不得意である。また、エレ
クトレツト型マイクロホンは振動子が薄くて軽い
フイルムであるため応答性は極めて良いが、静電
誘導方式であるため電磁誘導方式に比べ出力が非
常に小さくS/N比が低い。スピーカとしても、
電磁コイルを振動させる方式は高効率で音圧レベ
ルも高いが、応答性が悪いため高音が出ないし、
プラスチツクフイルムを静電誘導力で振動させる
方式は振動体が極めて薄く軽量なため応答性が良
く、高音の音質が良いが極めて低効率であり、音
圧レベルも低いという問題がある。
本発明は、上述のような欠点を除去し、応答性
と出力・効率の両方とも優れたトランスデユーサ
を提供せんとするものであり、以下に具体例をあ
げ詳述する。
問題点を解決するための手段
本発明のトランスデユーサは垂直磁化性強磁性
体層を高分子成形物、非磁性金属、無機物等の基
材上に形成し、それを電磁コイルに近接して設け
たものである。
作 用
上記構成において、基材を機械振動させると、
磁場変化が生じ、基材近傍に配置された電磁コイ
ルの端子間に電気信号が発生する。逆に、電磁コ
イルの端子間に電気信号を供給すると、磁場変化
が生じ、基材が機械振動して音声等を発生する。
実施例
第1図に本発明のトランスデユーサーの一実施
形態を示す。第1図に於て、1は高分子成形物、
非磁性金属、無機物等の基材、2はこの基材1上
に形成された垂直磁化性強磁性体層であり、基材
1及び垂直磁化性強磁性体層2で振動体を形成し
ている。3及び4はこの振動体の表側および裏側
にそれぞれ近接設置された、リング状の電磁コイ
ルであり、AおよびBがコイル3の端子、Cおよ
びDがコイル4の端子である。
上記強磁性体層2は反磁界に抗して磁性層の面
にほぼ垂直に磁化される材料で構成され、図示の
ように面に垂直な一方向に磁化され、一面がN磁
極で他面がS磁極という磁気二重層が形成される
具体的には、Gd―Co,Tb―Fe,Co―Cr等の合
金をスパツタ法、真空蒸着法等の方法により基材
1上に形成し、磁化することによつて得られる。
第1図にトランスデユーサは音響による空気振動
等の機械振動で基材1を振動させ、垂直磁性体層
2の磁気二重層を電磁コイル3及び4の近傍で振
動させることにより、コイル3の端子A,B間及
び、コイル4の端子C,D間に電気信号を誘起
し、マイクロホンとしての機能をはたす。また、
図示を省略するがレコード針からの機械振動をカ
ンチレバーで伝達し、カンチレバーの一端と基材
1を接着しておけば、レコード用ピツクアツプと
しての機能をはたす。また、逆に、端子A,B間
およびC,D間に電気信号を供給することによ
り、磁場変化を作り、垂直磁性体層2、従つて基
材1を磁力により機械振動させ、音声等を発生さ
せる。
すなわち、一例として厚さ10ミクロンの基材1
としてのポリイミドフイルム上に厚さ0.2ミクロ
ンのCo,Cr合金の薄膜を形成して垂直磁性体層
2とし、フイルム面と垂直な一方向に磁化したも
のを考えると、これは1gで約600cm2の面積があ
り、残留磁束密度は約3000ガウスであるから単位
重量当りの表面磁束は極めて弱い。ちなみに極め
て強力なサマリウム・コバルト永久磁石と比較す
ると、サマリウム・コバルトの比重は約8.0で残
留磁束密度は約9000ガウスであり、1g当りの磁
極面積が1cm2とすると、単位重量当りの表面磁束
はサマリウム・コバルト永久磁石に比べ上記垂直
磁性体層2の方が約200倍多い。そのため、この
垂直磁性体層2を振動子として用いれば、薄くて
極めて軽量でしかも表面磁束が多いので、これに
電磁コイル3,4を近接して設ければ、わずかな
空気の振動や機械振動に対し敏感に応答し、しか
も電磁誘導作用が大きいので高効率で電気エネル
ギーに変換でき、逆に電磁コイル3,4に信号電
流を流せば垂直磁性体層2が敏感に振動し、空気
を極めて効率よく、高い応答性で振動させること
ができるため、応答性と出力・効率は従来にない
高水準で両立できる。スピーカ等として機能させ
ることも可能である。例えば基材1として厚さ10
ミクロン以下程度のポリエステル,芳香族ナイロ
ン,Ti,B,Be,マイカ,カーボン等からなる
フイルムを用い、その上に垂直磁化性強磁性体層
2を厚さ0.5ミクロン以下程度の薄膜として形成
したものは極めて軽量で、しかも表面磁束が多い
ため、機械振動と電気信号のエネルギー変換効率
が高く、しかも応答性も優れている。
次に、本実施例の具体例について説明する。
(具体例1)
厚さ10ミクロンのポリイミドフイルム上にCo
―Cr合金(Co:80重量%,Cr:20重量%)を厚
さ0.5ミクロンの薄膜としてスパツタ法で形成し
た。残留磁束密度は3000ガウスであつた。これを
100mmφの円形に切り抜き、第1図に示す構成の
スピーカを試作した。第1表に示すように、この
スピーカの音圧レベルには比較例1の市販中高音
用コーン型スピーカ(直径6〜12cm)と比べ1k
Hzの音圧レベルは同程度であり、20kHzの音圧レ
ベルは著しく高い。また比較例2は厚さ10ミクロ
ンのポリフツ化ビニリデンフイルムをエレクトレ
ツト化したものを100mmφの円形に切り抜き、両
側に電極を配置してスピーカとしたものであり、
これは応答性が良く、高周波まで再生される効率
が低く、具体例1に比べ、1kHzも20kHzも出力が
かなり小さいものしか得られなかつた。
INDUSTRIAL APPLICATION FIELD The present invention relates to the improvement of a transducer that converts the mechanical energy of vibrations of air, liquid, records, etc. into electrical energy, and improves the response, sensitivity, linearity, and dynamic range of the conversion. The purpose is to obtain an excellent transducer such as Conventional technology Conventionally, as transducers that convert mechanical energy of vibration into electrical energy, there are moving coil type pickups that generate electromagnetic induced electromotive force by vibrating an electromagnetic coil in a magnetic field, and moving coil type pickups that generate electromagnetic induced electromotive force by vibrating an electromagnetic coil in a magnetic field. Moving magnet type pickups, which generate electromagnetic induced electromotive force by vibrating a magnet, are used for records. In addition, a method to obtain electrostatically induced electromotive force by vibrating an electret film near an electrode is used for microphones, and for speakers, an audio signal current is passed through an electromagnetic coil near a permanent magnet to cause the electromagnetic coil to vibrate. A method in which an audio signal voltage is applied to an electrode to cause a nearby plastic film to vibrate using electrostatic force has been put into practical use. Problems to be Solved by the Invention However, in all cases, excellent responsiveness, output, and efficiency have not been achieved. In other words, moving coil type pickups have relatively good response, but their output is extremely low, so they require dedicated expensive transformers and low-noise amplifiers.
Moving magnet pickups have high output, but because they vibrate a heavy permanent magnet, they have poor response and are not good at faithfully reproducing high-pitched sounds. Further, since the electret type microphone has a thin and light film vibrator, the response is extremely good, but since it uses an electrostatic induction method, the output is very small and the S/N ratio is low compared to the electromagnetic induction method. As a speaker,
The method of vibrating an electromagnetic coil has high efficiency and a high sound pressure level, but the response is poor and high-pitched sounds cannot be produced.
The method of vibrating a plastic film using electrostatic induction force has a good response because the vibrating body is extremely thin and lightweight, and the sound quality of high-pitched sounds is good, but the problem is that the efficiency is extremely low and the sound pressure level is low. The present invention aims to eliminate the above-mentioned drawbacks and provide a transducer that is excellent in both responsiveness and output/efficiency, and will be described in detail below with specific examples. Means for Solving the Problems The transducer of the present invention forms a perpendicularly magnetized ferromagnetic layer on a base material such as a molded polymer, a non-magnetic metal, or an inorganic material, and places it in close proximity to an electromagnetic coil. It was established. Effect In the above configuration, when the base material is mechanically vibrated,
A magnetic field change occurs and an electrical signal is generated between the terminals of an electromagnetic coil placed near the substrate. Conversely, when an electric signal is supplied between the terminals of the electromagnetic coil, a change in the magnetic field occurs, causing the base material to mechanically vibrate and generate sounds and the like. Example FIG. 1 shows an embodiment of the transducer of the present invention. In Fig. 1, 1 is a polymer molded product;
A base material such as a non-magnetic metal or an inorganic material, 2 is a perpendicularly magnetized ferromagnetic layer formed on this base material 1, and the base material 1 and the perpendicularly magnetized ferromagnetic layer 2 form a vibrating body. There is. 3 and 4 are ring-shaped electromagnetic coils installed close to the front and back sides of the vibrating body, respectively, A and B are terminals of the coil 3, and C and D are terminals of the coil 4. The ferromagnetic layer 2 is made of a material that is magnetized almost perpendicularly to the plane of the magnetic layer against a demagnetizing field, and is magnetized in one direction perpendicular to the plane as shown in the figure, with one side having an N magnetic pole and the other side. Specifically, an alloy such as Gd-Co, Tb-Fe, Co-Cr, etc. is formed on the base material 1 by a method such as a sputtering method or a vacuum evaporation method, and then magnetized. obtained by doing.
In FIG. 1, the transducer vibrates the base material 1 with mechanical vibrations such as acoustic air vibrations, and vibrates the magnetic double layer of the vertical magnetic layer 2 in the vicinity of the electromagnetic coils 3 and 4. Electric signals are induced between terminals A and B and between terminals C and D of the coil 4, thereby functioning as a microphone. Also,
Although not shown, if the mechanical vibration from the record stylus is transmitted by a cantilever and one end of the cantilever and the base material 1 are bonded, it will function as a record pickup. Conversely, by supplying electrical signals between terminals A and B and between terminals C and D, magnetic field changes are created, and the vertical magnetic layer 2, and thus the base material 1, are mechanically vibrated by magnetic force, and audio, etc. generate. That is, as an example, a base material 1 with a thickness of 10 microns
If we consider that a thin film of Co, Cr alloy with a thickness of 0.2 microns is formed on a polyimide film to form the perpendicular magnetic layer 2, and magnetized in one direction perpendicular to the film surface, this is approximately 600 cm 2 at 1 g. , and the residual magnetic flux density is about 3000 Gauss, so the surface magnetic flux per unit weight is extremely weak. By the way, when compared to extremely strong samarium-cobalt permanent magnets, the specific gravity of samarium-cobalt is about 8.0 and the residual magnetic flux density is about 9000 Gauss.If the magnetic pole area per gram is 1 cm 2 , the surface magnetic flux per unit weight is There are about 200 times more perpendicular magnetic layers 2 than samarium-cobalt permanent magnets. Therefore, if this perpendicular magnetic layer 2 is used as a vibrator, it is thin and extremely lightweight, and has a large surface magnetic flux, so if the electromagnetic coils 3 and 4 are placed close to it, it can be used to suppress slight air vibrations and mechanical vibrations. It responds sensitively to energy and has a large electromagnetic induction effect, so it can be converted into electrical energy with high efficiency. Conversely, when a signal current is passed through the electromagnetic coils 3 and 4, the vertical magnetic layer 2 vibrates sensitively, causing the air to become extremely Since it can vibrate efficiently and with high responsiveness, it is possible to achieve both responsiveness, output, and efficiency at an unprecedentedly high level. It is also possible to function as a speaker or the like. For example, base material 1 has a thickness of 10
A film made of polyester, aromatic nylon, Ti, B, Be, mica, carbon, etc. with a thickness of about 0.5 microns or less is used, and a perpendicularly magnetizable ferromagnetic layer 2 is formed thereon as a thin film with a thickness of about 0.5 microns or less. Because it is extremely lightweight and has a large amount of surface magnetic flux, it has high energy conversion efficiency between mechanical vibration and electrical signals, and has excellent responsiveness. Next, a specific example of this embodiment will be explained. (Example 1) Co on a polyimide film with a thickness of 10 microns
- Cr alloy (Co: 80% by weight, Cr: 20% by weight) was formed as a thin film with a thickness of 0.5 microns using the sputtering method. The residual magnetic flux density was 3000 Gauss. this
A 100mmφ circular cutout was used to fabricate a prototype speaker with the configuration shown in Figure 1. As shown in Table 1, the sound pressure level of this speaker is 1k compared to Comparative Example 1, a commercially available cone-type speaker for medium and high frequencies (6 to 12 cm in diameter).
The sound pressure level at Hz is similar, and the sound pressure level at 20kHz is significantly higher. In Comparative Example 2, a 10 micron thick polyvinylidene fluoride film was made into an electret, cut out into a 100 mm diameter circle, and electrodes were placed on both sides to make a speaker.
This had good response, but had low efficiency in reproducing high frequencies, and compared to Example 1, only considerably smaller outputs at 1 kHz and 20 kHz could be obtained.
【表】
(具体例2)
厚さ5ミクロンのポリイミドフイルムGd―Co
(50:50)薄膜を0.5ミクロン厚さずつ両面にスパ
ツタ法で形成し、カンチレバーを接続するととも
に電磁コイルを近接設置し、レコード用ピツクア
ツプを試作した。これは第2表に示すように、比
較例3の市販ムービングマグネツト型ピツクアツ
プに比べ、コンプライアンス(機械的応答性)が
著しく高く、55kHz程度までレコード再生ができ
るようになつた。また、比較例4の市販ムービン
グコイル型ピツクアツプと比べると出力は著しく
高い。したがつて、この場合も応答性と出力が高
次元で両立されている。尚、第2表の測定は、試
験レコード(CBS STR―150)の1kHz基準信号
を用いた。[Table] (Specific example 2) Polyimide film Gd-Co with a thickness of 5 microns
(50:50) A thin film of 0.5 micron thickness was formed on both sides using the sputtering method, a cantilever was connected, and an electromagnetic coil was placed nearby to create a prototype record pickup. As shown in Table 2, the compliance (mechanical response) was significantly higher than that of the commercially available moving magnet type pickup of Comparative Example 3, and records could be played up to about 55 kHz. Furthermore, the output is significantly higher than that of the commercially available moving coil type pickup of Comparative Example 4. Therefore, in this case as well, both responsiveness and output are achieved at a high level. For the measurements in Table 2, a 1kHz reference signal of the test record (CBS STR-150) was used.
【表】
次に本発明のトランスデユーサの他の実施形態
について第2図を参照して説明する。5はエレク
トレツトからなる基材で、表面と裏面とで異なる
極性に帯電して、電気二重層を形成しており、6
は基材5の上に形成した垂直磁化性強磁性体層で
ある。この基材5と強磁性体層6により振動体が
形成されている。エレクトレツトとしては、ポリ
プロピレン,ポリカーボネート,ポリフツ化ビニ
リデン等の材料を強制的に帯電(ポーリング)す
ることによつて半永久的に500〜900V程度に帯電
したものが用いられる。7および8はこの振動体
の表側及び裏側にそれぞれ近接設置されたリング
状の電磁コイルであり、AおよびBがコイル7の
端子、CおよびDがコイル8の端子である。第2
図の構成のものを用いると、電磁エネルギーと機
械エネルギーとの変換がさらに効率良く行なわれ
る。即ち、強磁性体層6の磁気二重層の振動によ
り端子A,B間及びC,D間に電磁誘導による起
電力が発生すると同時に、基材5のエレクトレツ
トの振動により、コイル7全体とコイル8全体の
間に静電誘導起電力が発生する。そこでコイル7
と8を直列接続或いはコンデンサ等で位相調整し
た接続をすれば、電磁誘導と静電誘導の両方のエ
ネルギーを受けることが可能になり、より高い変
換効率が得られる。また、この場合、電磁コイル
7,8としては、第3図に示すように、高分子フ
イルム等の基材9の上に薄膜状の導体10を形成
したものや、これらを多層に重ねたもの等を用い
れば、第2図に示す基材5との静電的結合性が良
いため、高感度、高効率のトランスデユーサが得
られる。尚、振動体としては、基材両面に垂直磁
化性強磁性体層を設けたものや、逆に垂直磁化性
強磁性体層の両面に基材5を設けたものでもよい
し、互いに多層に重ねたものでも良いことは勿論
である。
次に、第2図に示す実施例の具体例について説
明する。
(具体例3)
厚さ5ミクロンのポリフツ化ビニリデンフイル
ム上にCo―Cr(Cr:20重量%)を真空蒸着し、
0.2ミクロン厚さの垂直磁化薄膜を形成し、フイ
ルムをポーリングし、帯電電圧850Vのエレクト
レツト化をした。垂直磁化性強性体層6の残留磁
化は2800ガウスであつた。次にこれを10mmφの振
動体として第2図の構造のマイクロホンを試作し
た。但し、電磁コイル7,8としては、第3図の
構造のものを5層積層して用いた。
(具体例4)
具体例3と同じものでフイルムをポーリングし
ていないもの、即ち、垂直磁化膜による電磁誘導
だけのものを用いて構成した。
(比較例5)
具体例3と同じものでCo―Cr薄膜のないも
の、即ち、エレクトレツトによる静電誘導だけの
ものを用いて構成した。[Table] Next, another embodiment of the transducer of the present invention will be described with reference to FIG. 2. 5 is a base material made of electret, which is charged with different polarities on the front and back sides to form an electric double layer;
is a perpendicularly magnetized ferromagnetic layer formed on the base material 5. The base material 5 and the ferromagnetic layer 6 form a vibrating body. The electret used is one semipermanently charged to about 500 to 900 V by forcibly charging (poling) a material such as polypropylene, polycarbonate, polyvinylidene fluoride, or the like. 7 and 8 are ring-shaped electromagnetic coils installed close to each other on the front and back sides of the vibrating body, A and B are terminals of the coil 7, and C and D are terminals of the coil 8. Second
When the configuration shown in the figure is used, the conversion between electromagnetic energy and mechanical energy is performed more efficiently. That is, the vibration of the magnetic double layer of the ferromagnetic layer 6 generates an electromotive force due to electromagnetic induction between terminals A and B and between terminals C and D, and at the same time, the vibration of the electret of the base material 5 causes the entire coil 7 and the coil to 8, an electrostatically induced electromotive force is generated. So coil 7
By connecting 8 and 8 in series or by connecting them with phase adjustment using a capacitor or the like, it becomes possible to receive energy from both electromagnetic induction and electrostatic induction, and higher conversion efficiency can be obtained. In this case, as shown in FIG. 3, the electromagnetic coils 7 and 8 may be those in which a thin film-like conductor 10 is formed on a base material 9 such as a polymer film, or those in which these are stacked in multiple layers. If such a material is used, a highly sensitive and highly efficient transducer can be obtained because of good electrostatic coupling with the base material 5 shown in FIG. The vibrating body may be one in which perpendicularly magnetized ferromagnetic layers are provided on both sides of the base material, or conversely, the base material 5 is provided on both sides of a perpendicularly magnetized ferromagnetic material layer, or a vibrating body may be one in which a perpendicularly magnetized ferromagnetic material layer is provided on both sides of the base material. Of course, it is also possible to use a layered one. Next, a specific example of the embodiment shown in FIG. 2 will be described. (Specific Example 3) Co-Cr (Cr: 20% by weight) was vacuum-deposited on a polyvinylidene fluoride film with a thickness of 5 microns,
A perpendicularly magnetized thin film with a thickness of 0.2 microns was formed, the film was polled, and it was made into an electret with a charging voltage of 850V. The residual magnetization of the perpendicular magnetic ferromagnetic layer 6 was 2800 Gauss. Next, we used this as a 10mmφ vibrator to fabricate a prototype microphone with the structure shown in Figure 2. However, as the electromagnetic coils 7 and 8, five layers of the structure shown in FIG. 3 were used. (Concrete Example 4) The same structure as in Concrete Example 3 was used, but the film was not polled, that is, only electromagnetic induction by a perpendicularly magnetized film was used. (Comparative Example 5) The same material as in Example 3 was used, but without the Co--Cr thin film, that is, using only electrostatic induction by electrets.
【表】
これらの実験結果を第3表に示す。比較例5の
静電誘導方式に比べ具体例4の垂直磁性体層によ
る電磁誘導方式は著しくマイクロホン感度が高
く、具体例3の複合方式ではさらに高感度になつ
た。尚、高周波に於てもこの傾向は変化しなかつ
た。
発明の効果
以上のように本発明のトランスデユーサは、高
分子成形物、非磁性金層、無機物等の基材上に垂
直磁化性強磁性体層を形成し、これに近設して電
磁コイルを設けたものであるため、薄く、軽量か
つ表面磁束の多い(単位重量あたりの表面磁束の
著しく多い)振動体が得られ、そのため、応答性
と効率・感度が従来にない高水準で両立され、ス
ピーカ,マイクロホン,レコード用ピツクアツプ
等に適用した場合、実用性の極めて高いものであ
る。[Table] Table 3 shows the results of these experiments. Compared to the electrostatic induction method of Comparative Example 5, the electromagnetic induction method using the perpendicular magnetic layer of Example 4 had significantly higher microphone sensitivity, and the combined method of Example 3 had even higher sensitivity. This tendency did not change even at high frequencies. Effects of the Invention As described above, the transducer of the present invention includes a perpendicularly magnetized ferromagnetic layer formed on a base material such as a polymer molded product, a nonmagnetic gold layer, an inorganic material, etc., and an electromagnetic Because it is equipped with a coil, it is possible to obtain a vibrating body that is thin, lightweight, and has a high surface magnetic flux (significantly high surface magnetic flux per unit weight), which achieves unprecedented levels of responsiveness, efficiency, and sensitivity. It is highly practical when applied to speakers, microphones, record pickups, etc.
第1図は本発明の第1の実施例を示すトランス
デユーサの要部断面図、第2図は本発明の第2の
実施例を示すトランスデユーサの要部断面図、第
3図は同トランスデユーサの電磁コイルの斜視図
である。
1,5……基材、2,6……垂直磁化性強磁性
体層、3,4,7,8……コイル。
FIG. 1 is a cross-sectional view of a main part of a transducer showing a first embodiment of the present invention, FIG. 2 is a cross-sectional view of a main part of a transducer showing a second embodiment of the present invention, and FIG. It is a perspective view of the electromagnetic coil of the same transducer. 1, 5... Base material, 2, 6... Perpendicular magnetization ferromagnetic layer, 3, 4, 7, 8... Coil.
Claims (1)
性金属、無機物等の基材上に形成し、電磁コイル
に近接して設けたことを特徴とするトランスデユ
ーサ。 2 基材がエレクトレツトであることを特徴とす
る特許請求の範囲第1項に記載のトランスデユー
サ。[Claims] 1. A transducer characterized in that a perpendicularly magnetizable ferromagnetic layer is formed on a base material such as a molded polymer, a nonmagnetic metal, an inorganic material, etc., and is provided in close proximity to an electromagnetic coil. . 2. The transducer according to claim 1, wherein the base material is an electret.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7443478A JPS551737A (en) | 1978-06-19 | 1978-06-19 | Transducer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7443478A JPS551737A (en) | 1978-06-19 | 1978-06-19 | Transducer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS551737A JPS551737A (en) | 1980-01-08 |
| JPS6150439B2 true JPS6150439B2 (en) | 1986-11-04 |
Family
ID=13547101
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7443478A Granted JPS551737A (en) | 1978-06-19 | 1978-06-19 | Transducer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS551737A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6847090B2 (en) * | 2001-01-24 | 2005-01-25 | Knowles Electronics, Llc | Silicon capacitive microphone |
| ATE392117T1 (en) | 2005-01-26 | 2008-04-15 | Harman Becker Automotive Sys | ELECTROACOUSTIC TRANSDUCER |
| EP1881732A1 (en) | 2006-06-21 | 2008-01-23 | Harman/Becker Automotive Systems GmbH | Magnetic membrane suspension |
-
1978
- 1978-06-19 JP JP7443478A patent/JPS551737A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS551737A (en) | 1980-01-08 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| KR101596894B1 (en) | Balanced plate type electromagnetic speaker | |
| US4901357A (en) | Electromagnetic transducer | |
| EP1209945A2 (en) | Multifunction acoustic device | |
| WO2000027166A2 (en) | Transducer concepts for hearing aids and other devices | |
| US7016515B2 (en) | Speaker apparatus | |
| US3046361A (en) | Electroacoustic transducer | |
| JP2001346291A (en) | Speaker device | |
| JPS6150439B2 (en) | ||
| JPH1141685A (en) | Speaker device | |
| JP2004056771A (en) | Vibrating membrane for electro-acoustic transducer and electro-acoustic transducer | |
| JPS6033800A (en) | Electromechanical transducer | |
| JPH0134476Y2 (en) | ||
| JP3835649B2 (en) | Speaker device | |
| JP2785206B2 (en) | Electroacoustic transducer | |
| JPH0323758Y2 (en) | ||
| JP3106338B2 (en) | Speaker and its magnetic circuit | |
| JP2003274487A (en) | Electroacoustic transducer | |
| CN209250878U (en) | The compound electroacoustic transducer of moving-coil electrostatic | |
| JP3021756B2 (en) | Horn type screwdriver | |
| JP2003163991A (en) | Speaker | |
| JPH037199B2 (en) | ||
| JPH10276497A (en) | Speaker | |
| JPS5892199A (en) | Electrostatic acoustic transducer | |
| JPS5810040B2 (en) | Musikosei speaker | |
| JP2890472B2 (en) | Electroacoustic transducer |