JPS61118096A - Parametric speaker - Google Patents

Parametric speaker

Info

Publication number
JPS61118096A
JPS61118096A JP23983684A JP23983684A JPS61118096A JP S61118096 A JPS61118096 A JP S61118096A JP 23983684 A JP23983684 A JP 23983684A JP 23983684 A JP23983684 A JP 23983684A JP S61118096 A JPS61118096 A JP S61118096A
Authority
JP
Japan
Prior art keywords
level
ultrasonic
wave
audio signal
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.)
Granted
Application number
JP23983684A
Other languages
Japanese (ja)
Other versions
JPH0582799B2 (en
Inventor
Tsuneo Tanaka
恒雄 田中
Mikiro Iwasa
幹郎 岩佐
Yoichi Kimura
陽一 木村
Yasutoshi Nakama
保利 中間
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 JP23983684A priority Critical patent/JPS61118096A/en
Publication of JPS61118096A publication Critical patent/JPS61118096A/en
Publication of JPH0582799B2 publication Critical patent/JPH0582799B2/ja
Granted 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
    • H04R3/00Circuits for transducers, loudspeakers or microphones
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R2217/00Details of magnetostrictive, piezoelectric, or electrostrictive transducers covered by H04R15/00 or H04R17/00 but not provided for in any of their subgroups
    • H04R2217/03Parametric transducers where sound is generated or captured by the acoustic demodulation of amplitude modulated ultrasonic waves

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Acoustics & Sound (AREA)
  • Signal Processing (AREA)
  • Obtaining Desirable Characteristics In Audible-Bandwidth Transducers (AREA)
  • Circuit For Audible Band Transducer (AREA)

Abstract

PURPOSE:To decrease an average level of an ultrasonic wave radiated in the air and to decrease a noise by controlling a level of an ultrasonic wave in accordance with the sound signal level. CONSTITUTION:The output of a sound signal source 3 is inputted in a modulator 4 and used as a control signal of a control device 9. The signal from a carrier oscillating device 5 is controlled by a level of a signal source 3 and inputted to the modulator 4. The signal is inputted through a power amplifier 6 to a speaker 2. An acoustic filter 7 to absorb the ultrasonic wave is installed between the speaker 2 and a listener 8. Thus, the average level of the ultrasonic wave can be decreased and the noise can be decreased.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は超音波に対する空気の非線形性を用いたスピー
カ(パラメトリックスピーカ)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 (parametric speaker) that uses the nonlinearity of air with respect to ultrasonic waves.

従来の技術 従来から拡声装置において、音の指向性をスポットライ
トの様に鋭くして、周囲騒音の影響を受けずKある特定
の範囲の人々にだけ聞かせたいと言う要求は、展示会な
どで個々の出品物ごとに別々の説明を行ないたい時や、
駅ホームでの案内放送などの用途で強いものがあった。
Conventional Technology Traditionally, there has been a demand for loudspeaker equipment to sharpen the directionality of sound like a spotlight so that only a certain range of people can hear it without being affected by ambient noise, such as at exhibitions. When you want to provide separate explanations for each individual item,
It was useful for applications such as announcements on station platforms.

この様な用途には従来ホーンスピーカが主として用いら
れて来たが、ホーンスピーカの指向性はその長さと口径
に強く依存し、特に音声の様に低音域で鋭い指向性を得
るKは、長さ、口径共に極めて大きなものKなると言う
欠点があった。
Conventionally, horn speakers have been mainly used for such applications, but the directivity of a horn speaker strongly depends on its length and aperture. However, it had the disadvantage of being extremely large in both diameter.

一方近年超音波に対する空気の非線形性を利用したスピ
ーカ(以下パラメトリックスピーカという)が従来に比
べはるかに鋭い指向性を得られることから注目されてい
る。まず従来のパラメトリックスピーカについて説明す
る。(例えば特開昭58−119293号) 第5図は従来のパラメトリックスピーカの構成を示すも
のである。第5図において、1は超音波振動子であり2
はこれを蜂の巣状に並べて構成したスピーカである。3
は音声信号源であり、この出力を変調器4に入力する。
On the other hand, in recent years, speakers that utilize the nonlinearity of air with respect to ultrasonic waves (hereinafter referred to as parametric speakers) have been attracting attention because they can obtain much sharper directivity than conventional speakers. First, conventional parametric speakers will be explained. (For example, Japanese Patent Laid-Open No. 58-119293) FIG. 5 shows the configuration of a conventional parametric speaker. In Fig. 5, 1 is an ultrasonic transducer and 2
is a speaker constructed by arranging these in a honeycomb shape. 3
is an audio signal source, and its output is input to the modulator 4.

ここで音声信号(変調波)は搬送波発振器6から出力さ
れる搬送波を40KHzとして振幅変調され、パワーア
ンプ6を経てスピーカ2に入力される。7は超音波を吸
収するための音響フィルタであり、スピーカ2と受聴者
8の間に設置されている。
Here, the audio signal (modulated wave) is amplitude-modulated using a carrier wave output from the carrier wave oscillator 6 at 40 KHz, and is input to the speaker 2 via the power amplifier 6. 7 is an acoustic filter for absorbing ultrasonic waves, and is installed between the speaker 2 and the listener 8.

上述したパラメトリックスピーカにおいて、スピーカ2
から放射された振幅変調超音波の搬送波と上下の側帯波
とは空中で非線形相互作用を起こし、鋭い指向性を有す
る変調波が発生する。ここでスピーカ2から出た振幅変
調超音波のことを1次波、1次波の非線形相互作用の結
果として生じた元の音声信号(変調波)のことを2次波
と称するO ところでパラメトリックスピーカでは1次波から2次波
への変換効率が極めて低い(1%以下)ために実用レベ
ルの2次波を発生させるためには強力な超音波が必要と
なる。例えば5odBの2次波音圧を得るためには14
0dB或いはそれ以上の1次波音圧が必要である。この
様な強い超音波を直接受聴者が浴びると聴力障害等の悪
影響が起こることが考えられる。そのためパラメトリッ
クスピーカの実用化に際しては第6図に示す音響フィル
タ7の設置が不可欠である。
In the parametric speakers described above, speaker 2
The carrier wave and the upper and lower sideband waves of the amplitude modulated ultrasonic wave emitted from the oscilloscope cause nonlinear interaction in the air, and a modulated wave with sharp directivity is generated. Here, the amplitude modulated ultrasonic wave emitted from the speaker 2 is called a primary wave, and the original audio signal (modulated wave) generated as a result of the nonlinear interaction of the primary waves is called a secondary wave.By the way, parametric speakers Since the conversion efficiency from primary waves to secondary waves is extremely low (1% or less), powerful ultrasonic waves are required to generate a practical level of secondary waves. For example, to obtain a secondary wave sound pressure of 5 odB, 14
A primary wave sound pressure of 0 dB or more is required. If a listener is directly exposed to such strong ultrasonic waves, it is conceivable that adverse effects such as hearing loss may occur. Therefore, when putting parametric speakers into practical use, it is essential to install an acoustic filter 7 shown in FIG. 6.

発明が解決しようとする問題点 しかしながら、上記の様な構成では以下の様な問題点が
残されていた。
Problems to be Solved by the Invention However, with the above configuration, the following problems remain.

(1)音響フィルタ7の下では超音波のレベルを十分に
下げたとしても、音響フィルタ7からはずれたところで
は、スピーカ2からの超音波を直接受けることになCる
。超音波は指向性が鋭いとは言えこのレベルは必ずしも
安全とは言い難い0 (2)  屋内でパラメトリックスピーカを使用する時
は周囲の壁などに超音波が反射し、音響フィルタ7の下
にも強い超音波レベルに達する領域が現れることがある
0 (鴻 超音波のレベルを下げるために音響フィルタ7の
超音波吸収係数を上げると、可聴音のレベルも低下して
しまう。
(1) Even if the level of the ultrasonic waves is sufficiently lowered below the acoustic filter 7, the ultrasonic waves from the speaker 2 will be directly received outside the acoustic filter 7. Although ultrasonic waves have sharp directivity, this level is not necessarily safe. (2) When using parametric speakers indoors, ultrasonic waves are reflected by surrounding walls and can also be transmitted under the acoustic filter 7. A region reaching a strong ultrasonic level may appear (Ko) If the ultrasonic absorption coefficient of the acoustic filter 7 is increased in order to lower the ultrasonic level, the audible sound level will also decrease.

(→ 信号波のレベルが小さい時(例えば無音時)でも
超音波のレベルは一定であるためエネルギー利用率が悪
く、更に無音時には超音波振動子から発生する低調波が
ノイズとなって聞こえる。
(→ Even when the level of the signal wave is low (for example, when there is no sound), the level of the ultrasonic wave is constant, so the energy utilization rate is poor, and when there is no sound, the low harmonics generated from the ultrasonic transducer can be heard as noise.

本発明は上記問題点に鑑み、超音波のレベルを変調波の
レベルによって制御することKより、超音波の平均レベ
ルを大幅に低下させたパラメトリックスピーカを提供す
るものである。
In view of the above problems, the present invention provides a parametric speaker in which the average level of ultrasonic waves is significantly reduced by controlling the level of ultrasonic waves by the level of modulated waves.

問題点を解決するための手段 上記問題点を解決するために本発明のパラメトリックス
ピーカは、超音波振動子と前記超音波振動子を音声信号
て変調された超音波で駆動するための変調器と音声信号
のレベルに応じて超音波のレベルを制御するための制御
器とから構成されている。
Means for Solving the Problems In order to solve the above problems, the parametric speaker of the present invention includes an ultrasonic vibrator and a modulator for driving the ultrasonic vibrator with an ultrasonic wave modulated by an audio signal. and a controller for controlling the level of ultrasonic waves according to the level of the audio signal.

作   用 本発明は上記の構成により変調器に入力される超音波領
域の搬送波のレベルを可聴周波である変調波のレベルに
よって制御し、変調波のレベルが小さい時には搬送波の
レベルを下げ逆に変調波のレベルが大きい時には搬送波
のレベルも上げる作用を行なわせる。その結果変調度は
ほぼ一定に保たれる。変調器によって変調された超音波
領域の信号は超音波振動子に入力された超音波として空
中に放射される。そして空気の非線形性によって搬送波
と側帯波とが干渉し、元の音声信号(変調波)が空中に
発生する。従来のパラメトリックスピーカでは、超音波
のレベルは変調波のレベルが最大の時を基準として設定
されていたので、変調波のレベルがゼロ即ち無音状態の
時でも超音波のレベルは強いままであった。しかるに本
発明によれば、超音波のレベルは、変調波のレベルに応
じて変化するため、空中に放射される超音波の平均レベ
ルを大幅に減少させることができる。
Effect of the Invention The present invention uses the above-described configuration to control the level of the carrier wave in the ultrasonic range input to the modulator by the level of the modulated wave which is an audio frequency, and when the level of the modulated wave is small, the level of the carrier wave is lowered and the level of the carrier wave is reversely modulated. When the wave level is high, the carrier wave level is also raised. As a result, the modulation degree is kept almost constant. The signal in the ultrasonic range modulated by the modulator is radiated into the air as an ultrasonic wave input to an ultrasonic transducer. Then, due to the nonlinearity of the air, the carrier wave and sideband waves interfere, and the original audio signal (modulated wave) is generated in the air. In conventional parametric speakers, the ultrasonic level was set based on the maximum modulated wave level, so the ultrasonic level remained strong even when the modulated wave level was zero, that is, there was no sound. . However, according to the present invention, since the level of the ultrasonic wave changes depending on the level of the modulated wave, the average level of the ultrasonic wave radiated into the air can be significantly reduced.

実施例 以下本発明の一実施例について図面を参照しながら説明
する。第1図において、9は搬送波の信号レベルを制御
するための制御器であり、他の構成は従来例と同じであ
るので説明を省略する。
EXAMPLE An example of the present invention will be described below with reference to the drawings. In FIG. 1, reference numeral 9 denotes a controller for controlling the signal level of a carrier wave, and since the other configurations are the same as those of the conventional example, a description thereof will be omitted.

制御器9は第2図に示す構成で実現できる。中心となる
のは電圧制御型増幅器1oである。制御信号には変調波
を整流回路11で整流し、増幅器12で増幅したものを
加える。必要により、適当な直流バイアスを重畳して加
えても差支えない。
The controller 9 can be realized with the configuration shown in FIG. The centerpiece is a voltage-controlled amplifier 1o. A modulated wave rectified by a rectifier circuit 11 and amplified by an amplifier 12 is added to the control signal. If necessary, an appropriate DC bias may be added in a superimposed manner.

搬送波発振器6の出力は電圧制御型増幅器1oに入力さ
れ、制御信号レベル〈応じて増幅されたあと対数/線形
変換増幅器13を経て変調器4に出力される。
The output of the carrier wave oscillator 6 is input to the voltage-controlled amplifier 1o, amplified according to the control signal level, and then output to the modulator 4 via the logarithmic/linear conversion amplifier 13.

次にこの制御器9の動作について説明する。音声信号源
3の出力は変調器4に入力されると共に制御器9の制御
信号として用いられる。搬送波発振器6からの信号は上
記制御信号のレベルによって制御され変調器4に入力さ
れる。制御信号電圧vcと制御器9の出力電圧/入力電
圧(V0/V、)の特性図を第3図に示す。この特性の
時には変調度を常に一定(0,3)とすることができる
。その結果、超音波の平均レベルは従来に比べて約20
dBも減少した。
Next, the operation of this controller 9 will be explained. The output of the audio signal source 3 is input to a modulator 4 and is used as a control signal for a controller 9. The signal from the carrier wave oscillator 6 is controlled by the level of the control signal and input to the modulator 4. A characteristic diagram of the control signal voltage vc and the output voltage/input voltage (V0/V,) of the controller 9 is shown in FIG. With this characteristic, the modulation degree can always be constant (0, 3). As a result, the average level of ultrasonic waves is approximately 20
dB also decreased.

第4図〜第6図の各図において、点線Aは従来、実線B
は本実施例の音声信号レベル、変調度、超音波レベルの
それぞれの時間変化を示したものである。従来は音声信
号のピーク時に変調度が0.3となる様に超音波の出力
を設定していたため、超音波のレベルは常に140dB
と一定であった。
In each figure from FIG. 4 to FIG. 6, dotted line A is conventionally replaced by solid line B.
1 shows the temporal changes in the audio signal level, modulation degree, and ultrasonic level in this example. Conventionally, the ultrasonic output was set so that the modulation depth was 0.3 at the peak of the audio signal, so the ultrasonic level was always 140 dB.
was constant.

しかるに本実施例では変調度が常1/C0,3となる様
に超音波の出力を制御しているために、超音波のレベル
は平均で約20dB低下させることができる0 発明の効果 本発明は、変調波(可聴周波)のレベルに応じて搬送波
(超音波)のレベルを制御する制御器を設けたことによ
り以下の効果を有する。
However, in this embodiment, since the ultrasonic output is controlled so that the modulation degree is always 1/C0.3, the ultrasonic level can be lowered by about 20 dB on average. has the following effects by providing a controller that controls the level of the carrier wave (ultrasonic wave) according to the level of the modulated wave (audio frequency).

(1)空中に放射される超音波の平均レベルを大幅に下
げることができるので、従来近距離での受聴には不可欠
であった音響フィルタを小型化或いはなくすことができ
る。
(1) Since the average level of ultrasonic waves radiated into the air can be significantly lowered, it is possible to miniaturize or eliminate acoustic filters, which have conventionally been indispensable for listening at short distances.

(に)音響フィルタを設ける場合もフィルタによる超音
波の減衰量は従来に比べて少なくてすむために、構造が
簡単になると共に音響フィルタによる可聴音レベルの低
下が防げる。
(2) Even when an acoustic filter is provided, the amount of attenuation of ultrasonic waves by the filter is smaller than that of the conventional method, so the structure is simplified and a decrease in the audible sound level due to the acoustic filter can be prevented.

(′4 変調波のレベルが小さい又は零の時は超音波の
出力も小さくなるため、従来の様に超音波振動子から発
生する低調波がノイズとなって聞こえると言った欠点が
解消される。
('4) When the level of the modulated wave is small or zero, the output of the ultrasonic wave is also small, which eliminates the drawback of conventional methods in which low harmonics generated from the ultrasonic transducer can be heard as noise. .

(萄 パワーアンプに対する平均負荷が低下するので省
エネルギー及びアンプの寿命が延びる。
(萄) The average load on the power amplifier is reduced, saving energy and extending the life of the amplifier.

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

第1図は本発明の一実施例におけるパラメトリックスピ
ーカの構成図、第2図は同制御器のブロック図、第3図
は制御器の電圧減衰特性を示す図、第4図乃至第6図は
従来と本実施例の音声信号レベル、変調度、超音波レベ
ルの時間変化を示す特性図、第7図は従来例の構成を示
す図である。 1・・・・・・超音波振動子、2・・・・・スピーカ、
3・・・・・・音声信号源、4・・・・・・変調器、5
・・・・・・搬送波発振器、6・・・・・・パワーアン
プ、7・・・・・・音響フィルタ、8・・・・・・受聴
者、9・・・・・・制御器。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 [2図 Q 第3図 $4 FP(f !  (’ n   Vc  (v)
第4図 時7%1− 第 6 図 特開 −
Fig. 1 is a block diagram of a parametric speaker according to an embodiment of the present invention, Fig. 2 is a block diagram of the controller, Fig. 3 is a diagram showing voltage attenuation characteristics of the controller, and Figs. 4 to 6 are FIG. 7 is a characteristic diagram showing temporal changes in the audio signal level, modulation degree, and ultrasonic level of the conventional example and this embodiment. FIG. 7 is a diagram showing the configuration of the conventional example. 1... Ultrasonic vibrator, 2... Speaker,
3...Audio signal source, 4...Modulator, 5
... Carrier wave oscillator, 6 ... Power amplifier, 7 ... Acoustic filter, 8 ... Listener, 9 ... Controller. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure [Figure 2 Q Figure 3 $4 FP (f ! (' n Vc (v)
Fig. 4: 7% 1 - Fig. 6 Unexamined patent application -

Claims (1)

【特許請求の範囲】[Claims] 音声信号源と、超音波帯の搬送波発振器と、前記搬送波
発振器からの出力が入力され、搬送波のレベルを前記音
声信号の出力レベルに応じて制御するための制御器と、
前記制御器の出力と前記音声信号源の出力とが入力され
前記制御器の搬送波を音声信号源の変調波で変調するた
めの変調器と、前記変調器の出力が入力され、変調され
た超音波を空中に放射し、空気の非線形性によって元の
音声信号を空中で発生させるための1個又は複数個の超
音波振動子からなるスピーカとを具備してなるパラメト
リックスピーカ。
an audio signal source, an ultrasonic band carrier wave oscillator, and a controller into which the output from the carrier wave oscillator is input and controls the level of the carrier wave according to the output level of the audio signal;
a modulator to which the output of the controller and the output of the audio signal source are input and for modulating the carrier wave of the controller with the modulated wave of the audio signal source; A parametric speaker comprising one or more ultrasonic transducers for radiating sound waves into the air and generating an original audio signal in the air due to the nonlinearity of the air.
JP23983684A 1984-11-14 1984-11-14 Parametric speaker Granted JPS61118096A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23983684A JPS61118096A (en) 1984-11-14 1984-11-14 Parametric speaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23983684A JPS61118096A (en) 1984-11-14 1984-11-14 Parametric speaker

Publications (2)

Publication Number Publication Date
JPS61118096A true JPS61118096A (en) 1986-06-05
JPH0582799B2 JPH0582799B2 (en) 1993-11-22

Family

ID=17050579

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23983684A Granted JPS61118096A (en) 1984-11-14 1984-11-14 Parametric speaker

Country Status (1)

Country Link
JP (1) JPS61118096A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000050387A (en) * 1998-07-16 2000-02-18 Massachusetts Inst Of Technol <Mit> Parameteric audio system
JP2003047096A (en) * 2001-07-30 2003-02-14 Mitsubishi Electric Engineering Co Ltd Super-directive speaker for railroad crossing

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000050387A (en) * 1998-07-16 2000-02-18 Massachusetts Inst Of Technol <Mit> Parameteric audio system
JP2010051039A (en) * 1998-07-16 2010-03-04 Massachusetts Inst Of Technology Parametric audio system
US8027488B2 (en) 1998-07-16 2011-09-27 Massachusetts Institute Of Technology Parametric audio system
US9036827B2 (en) 1998-07-16 2015-05-19 Massachusetts Institute Of Technology Parametric audio system
JP2003047096A (en) * 2001-07-30 2003-02-14 Mitsubishi Electric Engineering Co Ltd Super-directive speaker for railroad crossing

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