JP3668180B2 - Ultrasonic reproduction method / Ultrasonic reproduction device - Google Patents

Ultrasonic reproduction method / Ultrasonic reproduction device Download PDF

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Publication number
JP3668180B2
JP3668180B2 JP2001349998A JP2001349998A JP3668180B2 JP 3668180 B2 JP3668180 B2 JP 3668180B2 JP 2001349998 A JP2001349998 A JP 2001349998A JP 2001349998 A JP2001349998 A JP 2001349998A JP 3668180 B2 JP3668180 B2 JP 3668180B2
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Prior art keywords
ultrasonic
amplitude
frequency
ultrasonic signal
signal
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JP2001349998A
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JP2003153371A (en
Inventor
健司 清原
正人 三好
学 岡本
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Nippon Telegraph and Telephone Corp
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Nippon Telegraph and Telephone Corp
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Description

【0001】
【発明の属する技術分野】
この発明は、所望の領域にのみ再生音が聞こえるように限定させるための超音波再生方法及びその装置に係わり、特に放射される超音波エネルギーを低いレベルに抑えた超音波再生方法及びその装置に関する。
【0002】
【従来の技術】
近年、パーソナルコンピュータを用いたテレビ会議システム(以下デスクトップ会議システム;Desk Top Conference(DTC)システムと呼ぶ)が普及しつつある。これらの会議システムで相手の音声を再生する手段には従来は通常のスピーカを使用していた。
【0003】
【発明が解決しようとする課題】
しかし通常のスピーカは一般に指向性が広く、TV会議システムを使用している人だけではなく、その周辺にも相手の声(再生音)が聞こえ、周囲に不要な騒音となって聞こえてしまうという問題点があった。これを解決する一つの方法として可聴音信号で超音波信号を振幅変調し、この振幅変調された超音波信号を超音波素子から放射する構成としたパラメトリックスピーカを用いる方法が考えられる。
以下、パラメトリックスピーカの原理とその超指向性に付いて簡単に説明する。パラメトリックスピーカは強力な超音波(約100dB以上)を放射し、空気の非線形性を利用して可聴音を生成するものである。通常の音声レベル(約70dB)で伝播先における音波の強度を駆動源における強度の関数で示すと駆動源の強度の2次以上の成分は無視できる程小さい。しかし、100dB以上もの音波の伝播を考察する場合は上記2次以上の成分は無視できなくなる。この2次以上の成分の音圧は超音波の音圧が100dBのとき約60〜70dBとなり、この音圧レベルに達すると可聴音として聞こえるようになる。この空気の非線形項を利用して可聴音を生成するのがパラメトリックスピーカである。
【0004】
この可聴音生成の方法のうち、比較的効率の良い方法が超音波の振幅変調である。超音波を放射する超音波素子には共振周波数がある。この共振周波数付近の周波数を持つ超音波信号をキャリアとして可聴音信号で振幅変調する。すると超音波素子から放射された超音波は、空気の非線形性に基づく自己復調作用によって、空気を伝播するうちに自然に可聴音が生成される(鎌倉友男「非線形音響学の基礎」(愛智出版)1996 pp.107−110)。しかし図7に示す振幅変調の周波数分析からも分かる通り、振幅変調によって生成される上側波帯SU、下側波帯SDは超音波信号SU(キャリア;図では40KHz)の約50dBであり、100dB以上もの超音波を出力しても70dB程度の可聴音(音声など)しか生成できないためエネルギー効率として1/1000程度であるという問題点があった。
【0005】
この発明の目的は可聴音の放射エネルギー効率を改善することができる超音波再生方法及び装置を提供しようとするものである。
【0006】
【課題を解決するための手段】
この発明では超音波信号を可聴音信号で振幅変調し、この振幅変調された超音波信号で電気音響変換部を駆動して電気音響変換部から超音波を放射する超音波再生方法において、電気音響変換部は複数の共振周波数を有し、振幅変調される超音波の周波数は上記複数の共振周波数に挟まれ、電気音響変換部を駆動する超音波信号に対する振幅出力特性が極小となる周波数とした超音波再生方法を提案する。
この発明では更に超音波信号発振器と、超音波信号発振器で発振した超音波信号を可聴音信号により振幅変調する振幅変調器と、振幅変調された超音波信号を放射する電気音響変換部とによって構成される超音波再生装置において、電気音響変換部は複数の共振周波数を具備し、振幅変調される超音波の周波数は複数の共振周波数で挟まれ、電気音響変換部を駆動する超音波信号に対する振幅出力特性が極小となる周波数とした超音波再生装置を提案する。
【0007】
この発明では更に上記の超音波再生装置において、電気音響変換部は互に共振周波数が異なる複数の圧電素子を共通の基盤に搭載した超音波再生装置を提案する。
作用
この発明による超音波再生方法及び装置によれば、電気音響変換部の駆動周波数を電気音響変換部の共振周波数で挟まれた超音波の放射特性が極小となる周波数に選定したから、単一共振周波数特性を有する超音波素子に共振周波数の超音波信号を印加した従来の超音波再生方法の駆動エネルギーより低いエネルギーで駆動しても従来技術と同等レベルの可聴音を再生することができる。その理由は以下に説明する実施例により明らかにされよう。
【0008】
【発明の実施の形態】
図1にこの発明による可聴音生成装置の一実施例を示す。図中1は超音波信号源、2は可聴音信号源、3は振幅変調器、4は増幅器、5は電気音響変換部を示す。
超音波信号源1は例えばfc=40KHzの超音波信号を発振する。可聴音信号源2は可聴周波数帯域の周波数を持つ可聴音信号を振幅変調器3に入力し、この振幅変調器3で超音波信号源1が出力する超音波信号を振幅変調する。振幅変調された超音波信号は必要に応じて増幅器4で増幅された電気音響変換部5へ出力される。電気音響変換部5は複数の超音波素子ELが一面上にマトリックス状或いは同芯円状に配列して構成することもできる。
【0009】
ここまでの構成は従来の可聴音生成装置と同じであるが、この発明では電気音響変換部5に用いる超音波素子ELが図2に示すように複数の共振周波数f1とf2を具備していている構成とした点を特徴とするものである。
図2に示す例ではf1とf2の2つの周波数に共振周波数を具備した例を示す。複数の共振周波数f1、f2を具備した超音波素子ELは図3に示す構造により得ることができる。図3において、電極を兼ねる基盤6Aの一方の面に互いに共振周波数がf1とf2を具備した圧電素子7A、7Bを装着し、圧電素子7A、7Bの上面にリング状の電極6Bを被着し、リング状の電極6Bを共通に接続することにより共振周波数を複数具備した超音波素子ELを得ることができる。
【0010】
共振周波数f1とf2で挟まれた部分には図2に示すように電気音響変換部5を駆動する超音波信号に対する振幅出力特性が極小となる周波数が存在し、この極小となる周波数と超音波信号源1の発振周波数fcを一致させ、周波数fcを中心として電気音響変換部5を駆動する。
ここで上限周波数が20kHzの可聴音信号により超音波信号を両側波帯方式の振幅変調器で振幅変調した場合には、図4に示すようにキャリアである超音波信号の周波数fcの上側と下側に上側波帯SUと下側波帯SDを持つ両側波帯信号が発生する。
【0011】
図2に示した電気音響変換部5の共振周波数f1とf2を図4に破線で示すように上側波帯SUと下側波帯SDのほぼ中心の周波数に合致させたとすると、超音波信号USは共振特性の谷の部分で抑制され、その放射レベルは従来の超音波振動子の共振周波数と超音波信号の周波数が一致している場合より抑圧される。反面上側波帯SU及び下側波帯SDは共振周波数f1,f2により強調される。従って、キャリアの成分の放射レベルを低く抑えて従来と同等の可聴音を再生できることになる。
図5を用いてその理由を説明する。図5Aは図7に示した従来の超音波再生方法を採った場合の超音波放射特性を示す。ここでは超音波信号USと周波数f1とf2の成分の放射レベルを示す。従来の超音波再生方法によれば超音波信号USの周波数を超音波素子の共振周波数に一致させているから超音波信号USは周波数f1とf2の成分より共振特性により強調される。その放射レベルをここでは「3」と仮定し、周波数f1とf2の成分の放射レベルをここでは「1」と仮定する。
【0012】
一方、この発明による超音波再生方法による超音波放射レベルを図5Bに示す。この発明による超音波再生方法では超音波信号USの周波数を超音波放射特性が極小値となる周波数に設定したから、超音波信号USの放射レベルは抑制される。例えば放射レベルは「2」となる。これに対し、周波数f1とf2の成分はこの発明ではこれらの周波数f1とf2を共振周波数としているから、その放射レベルは共振特性で強調され、例えば放射レベルが「1.5」に強調される。
これらの仮定から超音波の放射エネルギーと音圧パワーを算出すると、
従来の場合の超音波放射エネルギーW1は
W1=12 +32 +12 =11
従来の場合の音圧パワーSW1は
SW1=3×1+3×1=6
となる。
【0013】
この発明の場合の超音波放射エネルギーW2は
W2=1.52 +22 +1.52 =8.5
この発明の場合の音圧パワーSW2は
SW2=2×1.5+2×1.5=6
となる。
これらの計算例から明らかなように、この発明によれば従来と同じ音圧パワーを得るのに超音波放射エネルギーは「11」から「8.5」に抑制され、小さいエネルギーで従来と同等の音圧パワーを得ることができる。
【0014】
尚、上述では超音波信号USに対して周波数f1とf2の成分の音圧パワーだけを計算したが、本来は超音波信号USの上側と下側に発生する上側波帯SUと下側波帯SDの成分が積分されて強調されるから、音圧パワーSW2は更に強調される。そのために同じ音圧パワーSW2を得るのであれば超音波放射エネルギーW2を更に抑制することができる。
【0015】
【発明の効果】
以上説明したように、この発明によれば従来より小さいエネルギーで従来と同等の音圧を持つ超音波を放射することができるから、超音波を効率良く生成することができる利点が得られる。
【図面の簡単な説明】
【図1】この発明の一実施例を説明するためのブロック図。
【図2】この発明に用いる超音波素子の周波数特性を説明するための特性曲線図。
【図3】図2に示した周波数特性を呈する超音波素子の構造の一例を説明するための断面図。
【図4】図2に示した超音波素子の周波数特性と振幅変調された超音波信号の信号成分の関係を説明するためのグラフ。
【図5】この発明の効果を説明するためのグラフ。
【図6】この発明による装置により得られる超音波放射特性を説明するための曲線図。
【図7】従来の装置における超音波放射特性を説明するための曲線図。
【符号の説明】
1 超音波信号源 EL 超音波素子
2 可聴音信号源 6A 基盤
3 振幅変調器 6B 電極
4 増幅器 7A、7B 圧電素子
5 電気音響変換部
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to an ultrasonic reproduction method and apparatus for limiting reproduction sound to be heard only in a desired region, and more particularly to an ultrasonic reproduction method and apparatus for suppressing emitted ultrasonic energy to a low level. .
[0002]
[Prior art]
In recent years, a video conference system using a personal computer (hereinafter referred to as a desktop conference system; referred to as a Desk Top Conference (DTC) system) is becoming widespread. Conventionally, a normal speaker is used as means for reproducing the voice of the other party in these conference systems.
[0003]
[Problems to be solved by the invention]
However, ordinary speakers generally have a wide directivity, and not only the person using the TV conference system but also the other party's voice (reproduced sound) can be heard in the vicinity, and it can be heard as unnecessary noise around. There was a problem. As one method for solving this, a method using a parametric loudspeaker configured to amplitude-modulate an ultrasonic signal with an audible sound signal and radiate the amplitude-modulated ultrasonic signal from the ultrasonic element is conceivable.
The principle of the parametric speaker and its superdirectivity will be briefly described below. A parametric speaker emits strong ultrasonic waves (about 100 dB or more), and generates audible sound using the nonlinearity of air. When the intensity of the sound wave at the propagation destination is expressed as a function of the intensity at the drive source at a normal sound level (about 70 dB), the second and higher order components of the intensity of the drive source are negligibly small. However, when considering the propagation of sound waves of 100 dB or more, the second and higher order components cannot be ignored. The sound pressure of the second and higher components is about 60 to 70 dB when the ultrasonic sound pressure is 100 dB. When this sound pressure level is reached, it can be heard as an audible sound. It is a parametric speaker that generates audible sound using the nonlinear term of air.
[0004]
Among these audible sound generation methods, a relatively efficient method is ultrasonic amplitude modulation. An ultrasonic element that emits ultrasonic waves has a resonance frequency. The ultrasonic signal having a frequency near the resonance frequency is used as a carrier to modulate the amplitude with an audible sound signal. Then, the ultrasonic wave emitted from the ultrasonic element naturally generates audible sound while propagating through the air due to the self-demodulation action based on the nonlinearity of the air (Tomoo Kamakura “Basics of Nonlinear Acoustics” (Ai Satoshi Publishing) 1996 pp. 107-110). However, as can be seen from the frequency analysis of the amplitude modulation shown in FIG. 7, the upper sideband SU and the lower sideband SD generated by the amplitude modulation are about 50 dB of the ultrasonic signal SU (carrier; 40 KHz in the figure), and 100 dB Even if the above ultrasonic waves are output, only an audible sound (sound, etc.) of about 70 dB can be generated, so that there is a problem that the energy efficiency is about 1/1000.
[0005]
An object of the present invention is to provide an ultrasonic reproduction method and apparatus capable of improving the radiant energy efficiency of audible sound.
[0006]
[Means for Solving the Problems]
According to the present invention, in an ultrasonic reproduction method in which an ultrasonic signal is amplitude-modulated with an audible sound signal, an electroacoustic transducer is driven by the amplitude-modulated ultrasonic signal, and an ultrasonic wave is emitted from the electroacoustic transducer, The conversion unit has a plurality of resonance frequencies, and the frequency of the ultrasonic wave to be amplitude-modulated is sandwiched between the plurality of resonance frequencies, so that the amplitude output characteristic for the ultrasonic signal driving the electroacoustic conversion unit is minimized. We propose an ultrasonic reproduction method.
The present invention further includes an ultrasonic signal oscillator, an amplitude modulator that amplitude-modulates an ultrasonic signal oscillated by the ultrasonic signal oscillator with an audible sound signal, and an electroacoustic converter that radiates the amplitude-modulated ultrasonic signal. In the ultrasonic reproducing apparatus, the electroacoustic conversion unit has a plurality of resonance frequencies, and the frequency of the ultrasonic wave to be amplitude-modulated is sandwiched between the plurality of resonance frequencies, and the amplitude with respect to the ultrasonic signal that drives the electroacoustic conversion unit We propose an ultrasonic reproducing device with a frequency that minimizes the output characteristics.
[0007]
The present invention further proposes an ultrasonic reproducing apparatus in which, in the ultrasonic reproducing apparatus described above, a plurality of piezoelectric elements having resonance frequencies different from each other are mounted on a common substrate.
Action According to the ultrasonic reproduction method and apparatus according to the present invention, the drive frequency of the electroacoustic transducer is selected as a frequency at which the radiation characteristic of the ultrasonic wave sandwiched between the resonance frequencies of the electroacoustic transducer is minimized. Therefore, even if it is driven with an energy lower than the driving energy of the conventional ultrasonic reproduction method in which an ultrasonic signal having a resonance frequency is applied to an ultrasonic element having a single resonance frequency characteristic, an audible sound of the same level as that of the conventional technique is reproduced. be able to. The reason will be clarified by the examples described below.
[0008]
DETAILED DESCRIPTION OF THE INVENTION
FIG. 1 shows an embodiment of an audible sound generating apparatus according to the present invention. In the figure, 1 is an ultrasonic signal source, 2 is an audible sound signal source, 3 is an amplitude modulator, 4 is an amplifier, and 5 is an electroacoustic converter.
The ultrasonic signal source 1 oscillates an ultrasonic signal of fc = 40 KHz, for example. The audible sound signal source 2 inputs an audible sound signal having a frequency in the audible frequency band to the amplitude modulator 3, and the amplitude modulator 3 amplitude-modulates the ultrasonic signal output from the ultrasonic signal source 1. The amplitude-modulated ultrasonic signal is output to the electroacoustic conversion unit 5 amplified by the amplifier 4 as necessary. The electroacoustic transducer 5 can also be configured by arranging a plurality of ultrasonic elements EL in a matrix or concentric circles on one surface.
[0009]
The configuration so far is the same as that of the conventional audible sound generating apparatus. However, in the present invention, the ultrasonic element EL used for the electroacoustic transducer 5 has a plurality of resonance frequencies f1 and f2 as shown in FIG. It is characterized by the point of having a configuration.
In the example shown in FIG. 2, an example is shown in which resonance frequencies are provided at two frequencies f1 and f2. An ultrasonic element EL having a plurality of resonance frequencies f1 and f2 can be obtained by the structure shown in FIG. In FIG. 3, piezoelectric elements 7A and 7B having resonance frequencies f1 and f2 are mounted on one surface of a base 6A that also serves as an electrode, and a ring-shaped electrode 6B is attached to the upper surfaces of the piezoelectric elements 7A and 7B. By connecting the ring-shaped electrode 6B in common, an ultrasonic element EL having a plurality of resonance frequencies can be obtained.
[0010]
As shown in FIG. 2, there is a frequency at which the amplitude output characteristic with respect to the ultrasonic signal for driving the electroacoustic transducer 5 is minimized in the portion sandwiched between the resonance frequencies f1 and f2. The oscillation frequency fc of the signal source 1 is matched, and the electroacoustic transducer 5 is driven around the frequency fc.
Here, when the ultrasonic signal is amplitude-modulated with an audible sound signal having an upper limit frequency of 20 kHz by a double-sideband type amplitude modulator, as shown in FIG. 4, the upper side and the lower side of the frequency fc of the ultrasonic signal as a carrier are shown. A double sideband signal having an upper sideband SU and a lower sideband SD on the side is generated.
[0011]
Assuming that the resonance frequencies f1 and f2 of the electroacoustic transducer 5 shown in FIG. 2 coincide with the frequencies of the substantially center of the upper side band SU and the lower side band SD as shown by broken lines in FIG. Is suppressed in the valley portion of the resonance characteristics, and the radiation level is suppressed compared to the case where the resonance frequency of the conventional ultrasonic transducer and the frequency of the ultrasonic signal coincide with each other. On the other hand, the upper sideband SU and the lower sideband SD are emphasized by the resonance frequencies f1 and f2. Therefore, it is possible to reproduce the audible sound equivalent to the conventional one while keeping the radiation level of the carrier component low.
The reason will be described with reference to FIG. FIG. 5A shows ultrasonic radiation characteristics when the conventional ultrasonic reproducing method shown in FIG. 7 is adopted. Here, the radiation levels of the components of the ultrasonic signal US and the frequencies f1 and f2 are shown. According to the conventional ultrasonic reproducing method, since the frequency of the ultrasonic signal US is matched with the resonance frequency of the ultrasonic element, the ultrasonic signal US is emphasized by the resonance characteristics from the components of the frequencies f1 and f2. The radiation level is assumed to be “3” here, and the radiation levels of the components of the frequencies f1 and f2 are assumed to be “1” here.
[0012]
On the other hand, the ultrasonic radiation level by the ultrasonic reproducing method according to the present invention is shown in FIG. 5B. In the ultrasonic reproducing method according to the present invention, since the frequency of the ultrasonic signal US is set to a frequency at which the ultrasonic radiation characteristic becomes a minimum value, the radiation level of the ultrasonic signal US is suppressed. For example, the radiation level is “2”. On the other hand, since the components of the frequencies f1 and f2 use the frequencies f1 and f2 as resonance frequencies in the present invention, the radiation level is emphasized by the resonance characteristics, for example, the radiation level is emphasized to “1.5”. .
When calculating the radiation energy and sound pressure power of ultrasonic waves from these assumptions,
The ultrasonic radiation energy W1 in the conventional case is W1 = 1 2 +3 2 +1 2 = 11.
The sound pressure power SW1 in the conventional case is SW1 = 3 × 1 + 3 × 1 = 6.
It becomes.
[0013]
The ultrasonic radiation energy W2 in the case of this invention is W2 = 1.5 2 +2 2 +1.5 2 = 8.5.
In the present invention, the sound pressure power SW2 is SW2 = 2 × 1.5 + 2 × 1.5 = 6.
It becomes.
As is clear from these calculation examples, according to the present invention, the ultrasonic radiation energy is suppressed from “11” to “8.5” in order to obtain the same sound pressure power as in the prior art, and is equivalent to the conventional one with a small energy. Sound pressure power can be obtained.
[0014]
In the above description, only the sound pressure power of the components of the frequencies f1 and f2 is calculated for the ultrasonic signal US, but the upper side band SU and the lower side band that are originally generated above and below the ultrasonic signal US. Since the SD component is integrated and emphasized, the sound pressure power SW2 is further emphasized. Therefore, if the same sound pressure power SW2 is obtained, the ultrasonic radiation energy W2 can be further suppressed.
[0015]
【The invention's effect】
As described above, according to the present invention, it is possible to radiate an ultrasonic wave having a sound pressure equivalent to that of the prior art with energy smaller than that of the prior art. Therefore, there is an advantage that the ultrasonic waves can be generated efficiently.
[Brief description of the drawings]
FIG. 1 is a block diagram for explaining an embodiment of the present invention.
FIG. 2 is a characteristic curve diagram for explaining frequency characteristics of an ultrasonic element used in the present invention.
3 is a cross-sectional view for explaining an example of a structure of an ultrasonic element exhibiting frequency characteristics shown in FIG. 2;
4 is a graph for explaining the relationship between the frequency characteristics of the ultrasonic element shown in FIG. 2 and the signal components of an amplitude-modulated ultrasonic signal. FIG.
FIG. 5 is a graph for explaining the effect of the present invention.
FIG. 6 is a curve diagram for explaining the ultrasonic radiation characteristics obtained by the apparatus according to the present invention.
FIG. 7 is a curve diagram for explaining ultrasonic radiation characteristics in a conventional apparatus.
[Explanation of symbols]
1 Ultrasonic Signal Source EL Ultrasonic Element 2 Audible Sound Signal Source 6A Base 3 Amplitude Modulator 6B Electrode 4 Amplifier 7A, 7B Piezoelectric Element 5 Electroacoustic Converter

Claims (3)

超音波信号を可聴音信号で振幅変調し、この振幅変調された超音波信号で電気音響変換部を駆動して電気音響変換部から超音波を放射する超音波再生方法において、
上記電気音響変換部は複数の共振周波数を有し、上記振幅変調される超音波の周波数は上記複数の共振周波数に挟まれ、上記電気音響変換部を駆動する超音波信号に対する振幅出力特性が極小となる周波数であることを特徴とする超音波再生方法。
In the ultrasonic reproduction method of amplitude-modulating an ultrasonic signal with an audible sound signal, driving the electroacoustic conversion unit with the amplitude-modulated ultrasonic signal and emitting ultrasonic waves from the electroacoustic conversion unit,
The electroacoustic transducer has a plurality of resonance frequencies, and the amplitude-modulated ultrasonic frequency is sandwiched between the plurality of resonance frequencies, and the amplitude output characteristic for the ultrasonic signal that drives the electroacoustic transducer is minimal. An ultrasonic reproduction method characterized in that the frequency is
超音波信号発振器と、超音波信号発振器で発振した超音波信号を可聴音信号により振幅変調する振幅変調器と、振幅変調された超音波信号を放射する電気音響変換部とによって構成される超音波再生装置において、
上記電気音響変換部は複数の共振周波数を具備し、上記振幅変調される超音波の周波数は上記複数の共振周波数で挟まれ、上記電気音響変換部を駆動する超音波信号に対する振幅出力特性が極小となる周波数であることを特徴とする超音波再生装置。
Ultrasound composed of an ultrasonic signal oscillator, an amplitude modulator that modulates the ultrasonic signal generated by the ultrasonic signal oscillator with an audible sound signal, and an electroacoustic transducer that emits the amplitude-modulated ultrasonic signal In the playback device,
The electroacoustic transducer has a plurality of resonance frequencies, and the amplitude-modulated ultrasonic frequency is sandwiched between the plurality of resonance frequencies, and the amplitude output characteristic for the ultrasonic signal that drives the electroacoustic transducer is minimal. An ultrasonic reproducing apparatus having a frequency of
請求項2記載の超音波再生装置において、上記電気音響変換部は互に共振周波数が異なる複数の圧電素子を共通の基盤に搭載したことを特徴とする超音波再生装置。  3. The ultrasonic reproduction apparatus according to claim 2, wherein the electroacoustic conversion unit has a plurality of piezoelectric elements having different resonance frequencies mounted on a common substrate.
JP2001349998A 2001-11-15 2001-11-15 Ultrasonic reproduction method / Ultrasonic reproduction device Expired - Fee Related JP3668180B2 (en)

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JP2009141451A (en) * 2007-12-04 2009-06-25 Nippon Ceramic Co Ltd Ultrasonic wave transceiver
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