JPH0160999B2 - - Google Patents
Info
- Publication number
- JPH0160999B2 JPH0160999B2 JP19669585A JP19669585A JPH0160999B2 JP H0160999 B2 JPH0160999 B2 JP H0160999B2 JP 19669585 A JP19669585 A JP 19669585A JP 19669585 A JP19669585 A JP 19669585A JP H0160999 B2 JPH0160999 B2 JP H0160999B2
- Authority
- JP
- Japan
- Prior art keywords
- radius
- piezoelectric film
- curvature
- sound pressure
- headphone
- 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
- 238000010586 diagram Methods 0.000 description 3
- 238000006073 displacement reaction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005520 electrodynamics Effects 0.000 description 1
- 229920006254 polymer film Polymers 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
Landscapes
- Piezo-Electric Transducers For Audible Bands (AREA)
- Headphones And Earphones (AREA)
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は振動板の曲率、形状について改良し
た、圧電フイルムを用いたヘツドホンに関するも
のである。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a headphone using a piezoelectric film with improved curvature and shape of a diaphragm.
(従来の技術)
ヘツドホンには振動板に圧電性高分子フイルム
を用いた圧電型ヘツドホンがある。しかして圧電
型フイルムを用いたヘツドホンは、全体的に小形
(薄形)にできること、また軽量にできることな
どの特長を有しており、注目されている。第4図
は圧電フイルムを用いたヘツドホンで、振動子と
して圧電フイルム1がケース2に支持され、ケー
ス2の一面にあけられた複数個の孔3をとおして
音圧を外に放射するが、ケース2に接してイヤパ
ツド4があり、イヤパツド4に接する耳(図示せ
ず)に音波を送るようになつている。(Prior Art) There is a piezoelectric type headphone that uses a piezoelectric polymer film as a diaphragm. Headphones using piezoelectric films are attracting attention because they have features such as being able to be made smaller overall (thinner) and lighter in weight. FIG. 4 shows a headphone using a piezoelectric film, in which a piezoelectric film 1 as a vibrator is supported by a case 2, and sound pressure is radiated to the outside through a plurality of holes 3 made on one side of the case 2. There is an ear pad 4 in contact with the case 2, and is adapted to send sound waves to an ear (not shown) in contact with the ear pad 4.
(発明が解決しようとする問題点)
圧電フイルムを用いたヘツドホンは、動電型ヘ
ツドホンと比較すると、同じ電気信号で駆動され
た場合は、出力音圧が低いという欠点がある。そ
こで第4図における圧電フイルム型ヘツドホンに
おいて、ドーム状に形成された圧電フイルム1の
曲率半径rを大きくすると、同一電気信号入力に
対する圧電フイルム1の変位が大きくなり、出力
音圧は高くなる。しかしその半面で、電気信号入
力の周波数を変えた場合の出力音圧の特性を見る
と、曲率半径rを大きくした場合の最低共振周波
数は低くなる。(Problems to be Solved by the Invention) A headphone using a piezoelectric film has a disadvantage that, compared to an electrodynamic headphone, the output sound pressure is low when driven by the same electric signal. Therefore, in the piezoelectric film type headphone shown in FIG. 4, if the radius of curvature r of the dome-shaped piezoelectric film 1 is increased, the displacement of the piezoelectric film 1 for the same electrical signal input becomes larger, and the output sound pressure becomes higher. However, on the other hand, looking at the characteristics of the output sound pressure when the frequency of the electrical signal input is changed, the lowest resonance frequency becomes lower when the radius of curvature r is increased.
第5図は、第4図のヘツドホンの圧電フイルム
1について、種々の入力周波数に対する出力音圧
の大きさを表す特性図であるが、2種類の圧電フ
イルムの曲率半径が、それぞれr1とr2である場
合、その特性曲線は図に示すとおりである。こゝ
でr1>r2とすれば、曲率半径r1のものはr2のもの
より、出力音圧の絶対値は大きいが、最低共振周
波数f1は、曲率半径がr2のものの最低共振周波数
f2よりも低い。最低共振周波数が低いということ
は、再生周波数帯域が狭くなることと同義である
が、ヘツドホンのように広い周波数帯域で音声周
波数を再生することが必要なものでは大きな欠点
となる。本発明は圧電フイルムの曲率半径を大き
くして、同一電気信号入力に対する出力音圧を大
きくしながら、しかも周波数特性のすぐれたヘツ
ドホンを得るために成されたものである。 FIG. 5 is a characteristic diagram showing the magnitude of the output sound pressure with respect to various input frequencies for the piezoelectric film 1 of the headphone shown in FIG. 2 , its characteristic curve is as shown in the figure. Here, if r 1 > r 2 , the absolute value of the output sound pressure is larger for the one with the radius of curvature r 2 than that of the one with the radius of curvature r 2 , but the lowest resonance frequency f 1 is the lowest of the one with the radius of curvature r 2 . resonant frequency
lower than f2 . A low minimum resonant frequency is synonymous with a narrow reproduction frequency band, but this is a major drawback in devices such as headphones that need to reproduce audio frequencies over a wide frequency band. The present invention has been accomplished in order to increase the radius of curvature of the piezoelectric film, thereby increasing the output sound pressure for the same electrical signal input, and to obtain a headphone with excellent frequency characteristics.
(問題点を解決するための手段)
本発明は上記の問題点を解決するための手段と
して曲率半径の大きいドーム状の圧電フイルムを
主振動板とし、この圧電フイルムの曲率半径より
小さい半径をもつ円筒状圧電フイルムを高音用振
動板として、ケースに取付けたものである。(Means for Solving the Problems) As a means for solving the above problems, the present invention uses a dome-shaped piezoelectric film with a large radius of curvature as the main diaphragm, and has a radius smaller than the radius of curvature of the piezoelectric film. A cylindrical piezoelectric film is attached to the case as a diaphragm for high-pitched sounds.
(作用)
以上のような構成とすることにより、曲率の大
きいドーム状の圧電フイルムの、低周波で大きい
出力音圧を得ることができる特性と、円筒状圧電
フイルムの、高い周波数でも十分な出力音圧を得
ることができる特性とが合成されて、出力音圧げ
大きく、しかも再生周波数帯域の広いヘツドホン
を得ることができる。(Function) With the above configuration, the dome-shaped piezoelectric film with a large curvature has the characteristic of being able to obtain a large output sound pressure at low frequencies, and the cylindrical piezoelectric film has the characteristic of being able to obtain a large output sound pressure even at high frequencies. By combining the characteristics with which the sound pressure can be obtained, a headphone with a large output sound pressure and a wide playback frequency band can be obtained.
(実施例)
以下本発明の実施例を図について説明する。第
1図は本発明のヘツドホンの片耳分の断面図で、
ヘツドホン10には大きい曲率半径R1のドーム
状の圧電フイルム11が、ケース12に取付けら
れており、圧電フイルム11の曲率半径R1より
小さい半径R2をもち、ドーム状の圧電フイルム
の外周13にそうような円筒状圧電フイルム14
が、ケース12にフイルム11と同様に取付けら
れる。なおケース12の一面(第1図で左側)に
は、音圧を放射するために複数個の孔15があけ
られており、またケース12に接してイヤパツド
16が取付けられている。またケース12の音圧
放射側と反対側にはダンパ17が設けられてい
る。ケース12からドーム状フイルム11と円筒
状フイルム14を取り出してその形状を斜視図で
表したものが第2図である。図からもわかるとお
り、円筒状フイルム14の円筒の半径R2は、ド
ーム状フイルム11のドームの曲率半径R1より
も、かなり小さくなつている。(Example) Examples of the present invention will be described below with reference to the drawings. FIG. 1 is a cross-sectional view of one ear of the headphone of the present invention.
In the headphone 10, a dome-shaped piezoelectric film 11 with a large radius of curvature R1 is attached to a case 12, and an outer periphery 13 of the dome-shaped piezoelectric film has a radius R2 smaller than the radius of curvature R1 of the piezoelectric film 11. A cylindrical piezoelectric film 14 similar to
is attached to the case 12 in the same way as the film 11. A plurality of holes 15 are drilled on one side of the case 12 (the left side in FIG. 1) for radiating sound pressure, and an ear pad 16 is attached in contact with the case 12. Further, a damper 17 is provided on the side of the case 12 opposite to the sound pressure radiation side. FIG. 2 is a perspective view showing the shapes of the dome-shaped film 11 and the cylindrical film 14 taken out from the case 12. As can be seen from the figure, the radius R 2 of the cylinder of the cylindrical film 14 is considerably smaller than the radius of curvature R 1 of the dome of the dome-shaped film 11 .
第3図のC1は曲率半径R1のドーム状圧電フイ
ルム11の出力音圧の周波数特性を表したもの
で、最低共振周波数fR1はかなり低い周波数とな
る。第3図のC2は半径R2の円筒状圧電フイルム
14の周波数特性を表したもので、フイルム11
の最低共振周波数fR1よりもかなり高い共振周波
数fR2を持つている。よつてこの両者を第1図の
ようにケース12に取付け、ドーム状フイルム1
1のドームの曲率半径R1、円筒状フイルム14
の円筒の半径R2を適当に選び、イコライザ等の
音響素子定数を適当に選択することにより、第3
図において曲線C1および曲線C2が合成された曲
線C3のような周波数特性を得ることができる。 C1 in FIG. 3 represents the frequency characteristic of the output sound pressure of the dome-shaped piezoelectric film 11 with a radius of curvature R1, and the lowest resonance frequency fR1 is a considerably low frequency. C 2 in FIG. 3 represents the frequency characteristics of the cylindrical piezoelectric film 14 with a radius of R 2 .
has a resonant frequency fR 2 that is significantly higher than the lowest resonant frequency fR 1 . Then, attach both of them to the case 12 as shown in FIG.
Radius of curvature R 1 of dome 1, cylindrical film 14
By appropriately selecting the radius R 2 of the cylinder and appropriately selecting the constants of the acoustic elements such as the equalizer, the third
In the figure, a frequency characteristic such as curve C 3 , which is a combination of curve C 1 and curve C 2 , can be obtained.
(発明の効果)
本発明は上記のような構成と作用を有するもの
であるから、同一の電気信号入力に対し、従来の
ものよりも大きい出力音圧をもち、しかも広い再
生周波数帯域を持つた圧電型ヘツドホンの実現が
可能となる。(Effects of the Invention) Since the present invention has the above-described configuration and operation, it has a higher output sound pressure than the conventional one for the same electrical signal input, and also has a wider reproduction frequency band. It becomes possible to realize piezoelectric headphones.
第1図は本発明のヘツドホンの片側のみの断面
図、第2図は第1図のものの振動子であるフイル
ムだけを取出した斜視図、第3図は出力音圧の周
波数特性図、第4図は従来技術のヘツドホンの断
面図、第5図はその出力音圧の周波数特性図であ
る。
11……ドーム状圧電フイルム、14……円筒
状圧電フイルム、12……ケース。
Fig. 1 is a sectional view of only one side of the headphone of the present invention, Fig. 2 is a perspective view of the one in Fig. 1 with only the film that is the vibrator taken out, Fig. 3 is a frequency characteristic diagram of output sound pressure, and Fig. 4 The figure is a sectional view of a conventional headphone, and FIG. 5 is a frequency characteristic diagram of its output sound pressure. 11... Dome-shaped piezoelectric film, 14... Cylindrical piezoelectric film, 12... Case.
Claims (1)
板の曲率半径より小さい半径をもつ円筒状振動板
とをケースに取付けたことを特徴とする圧電型ヘ
ツドホン。1. A piezoelectric headphone characterized in that a dome-shaped diaphragm with a large radius of curvature and a cylindrical diaphragm with a radius smaller than the radius of curvature of the diaphragm are attached to a case.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19669585A JPS6257400A (en) | 1985-09-05 | 1985-09-05 | Piezoelectric type headphone |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19669585A JPS6257400A (en) | 1985-09-05 | 1985-09-05 | Piezoelectric type headphone |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6257400A JPS6257400A (en) | 1987-03-13 |
| JPH0160999B2 true JPH0160999B2 (en) | 1989-12-26 |
Family
ID=16362049
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19669585A Granted JPS6257400A (en) | 1985-09-05 | 1985-09-05 | Piezoelectric type headphone |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6257400A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06206086A (en) * | 1993-01-08 | 1994-07-26 | Nippon Steel Corp | Biological treatment of waste liquid and acclimation of microorganism |
| JP2693099B2 (en) * | 1993-01-20 | 1997-12-17 | 新日本製鐵株式会社 | Biological treatment method and acclimation method of microorganisms |
| JP2014212552A (en) * | 2014-06-24 | 2014-11-13 | 国立大学法人九州工業大学 | Speaker |
-
1985
- 1985-09-05 JP JP19669585A patent/JPS6257400A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6257400A (en) | 1987-03-13 |
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