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JPH0550196B2 - - Google Patents
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JPH0550196B2 - - Google Patents

Info

Publication number
JPH0550196B2
JPH0550196B2 JP59006537A JP653784A JPH0550196B2 JP H0550196 B2 JPH0550196 B2 JP H0550196B2 JP 59006537 A JP59006537 A JP 59006537A JP 653784 A JP653784 A JP 653784A JP H0550196 B2 JPH0550196 B2 JP H0550196B2
Authority
JP
Japan
Prior art keywords
region
input
frequency
mainly
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.)
Expired - Lifetime
Application number
JP59006537A
Other languages
Japanese (ja)
Other versions
JPS60150399A (en
Inventor
Tsuneo Tanaka
Mikiro Iwasa
Yoichi Kimura
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP59006537A priority Critical patent/JPS60150399A/en
Publication of JPS60150399A publication Critical patent/JPS60150399A/en
Publication of JPH0550196B2 publication Critical patent/JPH0550196B2/ja
Granted legal-status Critical Current

Links

Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B06GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
    • B06BMETHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
    • B06B1/00Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
    • B06B1/02Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy
    • B06B1/08Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with magnetostriction
    • B06B1/085Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with magnetostriction using multiple elements, e.g. arrays

Landscapes

  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Obtaining Desirable Characteristics In Audible-Bandwidth Transducers (AREA)
  • Circuit For Audible Band Transducer (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 本発明は特に展示会における出品物の説明や駅
ホームでの案内放送等に最適な指向性の鋭いスピ
ーカに関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a speaker with sharp directivity that is particularly suitable for explaining exhibits at exhibitions, broadcasting information on station platforms, and the like.

従来例の構成とその問題点 従来、拡声装置において鋭い指向性を要する場
合にはホーンスピーカが用いられてきた。しかし
ホーンスピーカの指向性はその長さと口径に強く
関係し、特に低音域で鋭い指向性を必要とする場
合にはホーン自体が極めて大きなものになると言
う欠点があつた。
Conventional configurations and their problems Conventionally, horn speakers have been used in loudspeaker systems where sharp directivity is required. However, the directivity of a horn speaker is strongly related to its length and diameter, and when sharp directivity is required, especially in the low frequency range, the horn itself has to be extremely large.

一方、近年超音波の非線型相作用であるパラメ
トリツク効果を用いたスピーカが線形領域よりも
遥かに鋭い指向性が得られると言う点で注目され
ている。まず。従来例について第1図と共に説明
する。1はバイモルフ構造のセラミツク圧電振動
子を用いた超音波トランスデユーサで、直径は
11.5cm、中心周波数40KHz、能率は軸上1mで、
10V入力時は113dBである。このトランスデユー
サの547個を図示するように並べてアレイ化しパ
ラメトリツクアレイスピーカ2を構成している。
音声信号源3からの信号は変調器4によつてAM
変調され、パワーアンプ5を経てパラメトリツク
アレイスピーカ2に入力される。搬送波(1次
波)の周波数は40KHzである。スピーカから放射
された1次波と側帯波は空気の非線形性によつて
干渉し空中で鋭どい指向性を持つた変調波(2次
波)が発生する。第2図にこのパラメトリツクア
レイスピーカ2の2次波の指向特性を示す。aは
1KHzの場合、bは5KHzの場合である。この様に
周波数が高くなる程指向性は鋭くなり、5KHzで
は音圧半減角は約4°であつた。これは実使用の状
態を考えると逆に狭すぎると考えられる。又この
様に大きく指向性が変化すると受聴位置のわずか
な変化によつて聴感が変化し極めて不自然である
と言う欠点があつた。
On the other hand, in recent years, speakers using parametric effects, which are nonlinear interaction effects of ultrasonic waves, have been attracting attention because they can provide much sharper directivity than in the linear region. first. A conventional example will be explained with reference to FIG. 1 is an ultrasonic transducer using a ceramic piezoelectric vibrator with a bimorph structure, and the diameter is
11.5cm, center frequency 40KHz, efficiency 1m on axis,
When inputting 10V, it is 113dB. A parametric array speaker 2 is constructed by arranging 547 of these transducers into an array as shown in the figure.
The signal from the audio signal source 3 is converted into AM by the modulator 4.
The signal is modulated and input to the parametric array speaker 2 via the power amplifier 5. The frequency of the carrier wave (primary wave) is 40KHz. The primary wave and sideband waves emitted from the speaker interfere with each other due to the nonlinearity of the air, and a modulated wave (secondary wave) with sharp directivity is generated in the air. FIG. 2 shows the directivity characteristics of the secondary waves of this parametric array speaker 2. a is
For 1KHz, b is for 5KHz. In this way, the higher the frequency, the sharper the directivity, and at 5KHz, the half-reduction angle of sound pressure was approximately 4°. This is considered to be too narrow considering actual usage conditions. Furthermore, such a large change in directivity has the disadvantage that even a slight change in the listening position changes the auditory sensation, resulting in an extremely unnatural sound.

一方、従来のパラメトリツクアレイスピーカの
アレイの直径と2次波の指向性の関係を第3図に
示す。aは直径150mm、bは450mmの場合で、周波
数は1KHzである。この様に直径が大きくなると
指向性は鋭くなる。
On the other hand, FIG. 3 shows the relationship between the array diameter and the directivity of secondary waves in a conventional parametric array speaker. A is for a diameter of 150 mm, b is for a diameter of 450 mm, and the frequency is 1 KHz. In this way, as the diameter increases, the directivity becomes sharper.

次に同じく従来のパラメトリツクアレイスピー
カの音圧周波数特性を第4図に示す。パラメトリ
ツクアレイスピーカでは1次波の音圧周波数特性
が平坦であれば、2次波の音圧周波数特性は
12dB/octで周波数と共に上昇する。現在用いて
いるトランスデユーサは帯域が40±2KHzと狭い
ために、2KHzまではほぼ理論通りに音圧が上昇
しているが、それ以上では1次波の音圧周波数特
性を反映して凹凸のある特性となつている。
Next, FIG. 4 shows the sound pressure frequency characteristics of a conventional parametric array speaker. In a parametric array speaker, if the sound pressure frequency characteristics of the primary wave are flat, the sound pressure frequency characteristics of the secondary wave are
It increases with frequency at 12dB/octave. Since the transducer currently in use has a narrow band of 40±2KHz, the sound pressure rises almost as expected up to 2KHz, but beyond that it becomes uneven due to the sound pressure frequency characteristics of the primary wave. It has become a certain characteristic.

発明の目的 本発明は、上記従来の欠点を解消し、周波数に
よる指向特性や音圧周波数特性の変化の少ないパ
ラメトリツクアレイスピーカを提供することを目
的とする。
OBJECTS OF THE INVENTION It is an object of the present invention to eliminate the above-mentioned conventional drawbacks and to provide a parametric array speaker with little change in directivity characteristics and sound pressure frequency characteristics depending on frequency.

発明の構成 本発明は、略同心円状に分離された複数の領域
からなるパラメトリツクアレイスピーカと各領域
にそれぞれ異なつた周波数特性や変調度の入力を
供給するための複数台の変調器、フイルタ、パワ
ーアンプ等から構成される。
Structure of the Invention The present invention provides a parametric array speaker consisting of a plurality of regions separated approximately concentrically, and a plurality of modulators and filters for supplying inputs with different frequency characteristics and modulation degrees to each region. Consists of power amplifiers, etc.

実施例の説明 パラメトリツクアレイスピーカでは2次波の周
波数が高くなる程一定の2次波の音圧を出すのに
要する1次波の音圧は小さくてすむ。即ちトラン
スデユーサの個数は少なく、アレイの直径は小さ
くてすむことがわかる。又直径を小さくする程指
向特性は広くなる。よつてアレイを同心円状に複
数の領域に分離し、中心部には全周波数帯域を、
又周辺には低音域のみを入力することによつて、
平坦な音圧周波数特性と均一な指向特性が実現で
きる。
Description of Embodiments In a parametric array speaker, the higher the frequency of the secondary wave, the smaller the sound pressure of the primary wave required to produce a constant sound pressure of the secondary wave. That is, it can be seen that the number of transducers is small and the diameter of the array is small. Also, the smaller the diameter, the broader the directional characteristics. Therefore, the array is divided into multiple concentric areas, with the entire frequency band in the center.
Also, by inputting only the low range to the surrounding area,
A flat sound pressure frequency characteristic and uniform directional characteristics can be achieved.

第5図に本発明の実施例の構成を示す。アレイ
の中心部のトランスデユーサの127個(直径180
mm)を領域A、その外側を領域Bとする。音声信
号を領域A,Bに分離し、領域Aには従来通り、
変調器4、パワーアンプ5を通して信号を入力す
る。領域Bにはローパスフイルタ6によつて2K
Hz以上の成分をカツトし、変調器4′、パワーア
ンプ5′を通して信号を入力する。各領域への入
力電圧又は変調度はできるだけ音圧周波数特性が
平坦になる様に選ぶ。具体的には低域の音圧を向
上させるために主として低域の入力される領域B
の方の入力レベル、変調度を領域Aよりも上げ
る。入力レベルや変調度を上げることは歪の増加
を招くが、低域の歪は高域に比べわかりにくいの
で聴感上は問題はほとんどない。本実施例の音圧
周波数特性を第6図に示し、指向特性を第7図に
示す。第7図aは1KHzの場合、bは5KHzの場合
である。従来の第4図、第2図と比較すれば明ら
かに改善されているのがわかる。本実施例ではア
レイを2つの領域に分離したが更に多くの領域に
分離することにより一層音圧、指向特性共に改善
されることは言うまでもない。
FIG. 5 shows the configuration of an embodiment of the present invention. 127 transducers in the center of the array (diameter 180
mm) is region A, and the outside thereof is region B. The audio signal is separated into areas A and B, and area A has the conventional
A signal is input through a modulator 4 and a power amplifier 5. 2K in area B by low pass filter 6
Components higher than Hz are cut off, and the signal is input through a modulator 4' and a power amplifier 5'. The input voltage or modulation degree to each region is selected so that the sound pressure frequency characteristics are as flat as possible. Specifically, in order to improve the sound pressure in the low range, area B is mainly used for low frequency input.
Raise the input level and modulation depth for region A than for region A. Increasing the input level or modulation degree causes an increase in distortion, but since low-frequency distortion is less noticeable than high-frequency distortion, there is almost no problem in terms of hearing. The sound pressure frequency characteristics of this embodiment are shown in FIG. 6, and the directivity characteristics are shown in FIG. 7. Figure 7a shows the case of 1KHz, and b shows the case of 5KHz. When compared with the conventional figures 4 and 2, it can be seen that there is a clear improvement. In this embodiment, the array is divided into two regions, but it goes without saying that by dividing the array into more regions, both the sound pressure and the directivity characteristics can be further improved.

発明の効果 以上のように、本発明は超音波トランスデユー
サアレイを略同心円状の複数の領域に分離し、独
立に駆動することにより以下の効果が得られる。
Effects of the Invention As described above, the present invention provides the following effects by dividing the ultrasonic transducer array into a plurality of substantially concentric regions and driving them independently.

(1) 中心部には主として高音域を、そして周辺部
程主として低音域を入力することによつて指向
特性の平坦化が図れる。
(1) The directional characteristics can be flattened by inputting mainly the high range to the center and mainly the low range to the periphery.

(2) 各領域によつて変調度や入力レベル、変調波
の周波数特性を変化させる(例えば低音域程変
調度をあげる)ことによつて音圧周波数特性の
平坦化が図れる。
(2) The sound pressure frequency characteristics can be flattened by changing the modulation degree, input level, and frequency characteristics of the modulated wave depending on each region (for example, increasing the modulation degree in the lower range).

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

第1図は従来例の構成を示す図、第2図は同2
次波の指向特性を示す図、第3図は従来のパラメ
トリツクアレイスピーカの直径と指向特性の関係
を示す図、第4図は従来例の音圧周波数特性を示
す図、第5図は本発明のパラメトリツクアレイス
ピーカの一実施例を示す構成図、第6図は同音圧
周波数特性を示す図、第7図は同指向特性を示す
図である。 1……超音波トランスデユーサ、2……トラン
スデユーサアレイ、3……音声信号源、4,4′
……変調器、5,5′……パワーアンプ、6……
ローパスフイルタ、A,B……領域。
Figure 1 is a diagram showing the configuration of a conventional example, and Figure 2 is a diagram showing the configuration of a conventional example.
Figure 3 is a diagram showing the relationship between the diameter and directional characteristics of a conventional parametric array speaker. Figure 4 is a diagram showing the sound pressure frequency characteristics of the conventional example. FIG. 6 is a diagram showing the same sound pressure frequency characteristic, and FIG. 7 is a diagram showing the same directional characteristic. 1... Ultrasonic transducer, 2... Transducer array, 3... Audio signal source, 4, 4'
...Modulator, 5,5'...Power amplifier, 6...
Low-pass filter, A, B... area.

Claims (1)

【特許請求の範囲】 1 略同心円状の複数の領域からなる超音波トラ
ンスデユーサアレイと、それぞれの領域を可聴周
波で変調された超音波で駆動するための複数個の
変調器とからなり、トランスデユーサアレイから
有限振幅超音波を空気中に放射し空気の非線形性
によつて可聴周波を再生することを特徴とするパ
ラメトリツクアレイスピーカ。 2 入力信号のレベル、変調度、変調波の周波数
特性の少なくとも1つを各領域によつて独立に制
御することを特徴とする特許請求の範囲第1項記
載のパラメトリツクアレイスピーカ。 3 複数の領域の内側の領域には可聴周波の主と
して高音域を、外側の領域には主として低音域を
入力することを特徴とする特許請求の範囲第1項
又は第2項記載のパラメトリツクアレイスピー
カ。 4 複数の領域の中で主として高音域が入力され
る領域は入力レベル又は変調度の少なく共1つを
小さく、主として低音域の入力される領域は大き
くしたことを特徴とする特許請求の範囲第1項、
第2項又は第3項記載のパラメトリツクアレイス
ピーカ。
[Claims] 1. An ultrasonic transducer array consisting of a plurality of substantially concentric regions, and a plurality of modulators for driving each region with ultrasound modulated with audio frequency, A parametric array speaker characterized in that finite amplitude ultrasonic waves are emitted into the air from a transducer array and audio frequencies are reproduced by the nonlinearity of the air. 2. The parametric array speaker according to claim 1, wherein at least one of the level of the input signal, the degree of modulation, and the frequency characteristic of the modulated wave is independently controlled in each region. 3. The parametric array according to claim 1 or 2, characterized in that the inner region of the plurality of regions is input with mainly the high range of audio frequencies, and the outer region is mainly input with the low range of audio frequencies. speaker. 4. Among the plurality of regions, at least one of the input level and the modulation degree is made smaller in the region where the high frequency range is mainly input, and the region where the low frequency range is mainly input is made larger. Section 1,
Parametric array speaker according to item 2 or 3.
JP59006537A 1984-01-18 1984-01-18 Parametric array speaker Granted JPS60150399A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59006537A JPS60150399A (en) 1984-01-18 1984-01-18 Parametric array speaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59006537A JPS60150399A (en) 1984-01-18 1984-01-18 Parametric array speaker

Publications (2)

Publication Number Publication Date
JPS60150399A JPS60150399A (en) 1985-08-08
JPH0550196B2 true JPH0550196B2 (en) 1993-07-28

Family

ID=11641093

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59006537A Granted JPS60150399A (en) 1984-01-18 1984-01-18 Parametric array speaker

Country Status (1)

Country Link
JP (1) JPS60150399A (en)

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6128293A (en) * 1984-07-18 1986-02-07 Matsushita Electric Ind Co Ltd Parametric array speaker
JPS62296698A (en) * 1986-06-17 1987-12-23 Matsushita Electric Ind Co Ltd Parametric speaker
US6359990B1 (en) 1997-04-30 2002-03-19 American Technology Corporation Parametric ring emitter
US7088830B2 (en) 1997-04-30 2006-08-08 American Technology Corporation Parametric ring emitter
JP4221792B2 (en) * 1998-01-09 2009-02-12 ソニー株式会社 Speaker device and audio signal transmitting device
JP2000050387A (en) 1998-07-16 2000-02-18 Massachusetts Inst Of Technol <Mit> Parametric audio system
FR2799873B1 (en) * 1999-10-18 2002-02-08 Comptoir De La Technologie ACTIVE SOUND INTENSITY MITIGATION DEVICE
JP4087199B2 (en) * 2002-09-17 2008-05-21 三菱電機エンジニアリング株式会社 Super directional speaker

Also Published As

Publication number Publication date
JPS60150399A (en) 1985-08-08

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