JPH0221720B2 - - Google Patents
Info
- Publication number
- JPH0221720B2 JPH0221720B2 JP12936583A JP12936583A JPH0221720B2 JP H0221720 B2 JPH0221720 B2 JP H0221720B2 JP 12936583 A JP12936583 A JP 12936583A JP 12936583 A JP12936583 A JP 12936583A JP H0221720 B2 JPH0221720 B2 JP H0221720B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- electroacoustic transducer
- pulse code
- code modulation
- ultrasonic
- 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
Links
- 238000010586 diagram Methods 0.000 description 6
- 238000006243 chemical reaction Methods 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000010355 oscillation Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G10—MUSICAL INSTRUMENTS; ACOUSTICS
- G10K—SOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
- G10K15/00—Acoustics not otherwise provided for
- G10K15/02—Synthesis of acoustic waves
Landscapes
- Health & Medical Sciences (AREA)
- Audiology, Speech & Language Pathology (AREA)
- General Health & Medical Sciences (AREA)
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Acoustics & Sound (AREA)
- Multimedia (AREA)
- Circuit For Audible Band Transducer (AREA)
- Transducers For Ultrasonic Waves (AREA)
Description
【発明の詳細な説明】
本発明はパルス符号変調再生スピーカに関する
ものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a pulse code modulation reproduction speaker.
従来アナログ信号をデジタル信号に変換した信
号のMSBからLSBまでに対応した音響変換器で
再生するスピーカが提案されている。この場合再
生に要する音響変換器が各ビツトに対応する数だ
け必要となり装置が複雑になる欠点があり、一つ
の変換器のボビンに複数のコイルを装着する場合
には質量増加により変換効率が低下する欠点を有
する。 Conventionally, a speaker has been proposed that reproduces signals obtained by converting an analog signal into a digital signal using an acoustic converter that supports MSB to LSB. In this case, the number of acoustic transducers required for playback corresponds to each bit, which has the disadvantage of complicating the device, and when multiple coils are attached to the bobbin of one transducer, the conversion efficiency decreases due to the increased mass. It has the disadvantage of
本発明は上記欠点を解決する新規な装置を提供
するもので、空気の非線形パラメトリツク作用を
利用して成すものである。 The present invention provides a novel device which overcomes the above-mentioned drawbacks and is achieved by utilizing the non-linear parametric effects of air.
本発明を一実施例により説明する。 The present invention will be explained by way of an example.
第1図は本発明の一実施例を示す図で、入力信
号1をAD変換器2でパルス符号変調した信号を
4ビツトとし、下位ビツトから順に信号5,6,
7,8で示す。発振器4は超音波素子21,2
2,23,24のそれぞれの共振周波数に略々等
しい発振周波数を有する。発振器4の信号と信号
5,6,7,8とを乗算器9,10,11,12
で演算処理する。 FIG. 1 is a diagram showing an embodiment of the present invention. Input signal 1 is pulse code modulated by AD converter 2, and the signal is 4 bits. Signals 5, 6,
Shown as 7 and 8. The oscillator 4 includes ultrasonic elements 21 and 2
It has an oscillation frequency approximately equal to each of the resonance frequencies of 2, 23, and 24. The signal of the oscillator 4 and the signals 5, 6, 7, 8 are multiplied by the multipliers 9, 10, 11, 12.
Perform calculations with .
演算処理された信号は増幅器13,14,1
5,16で増幅し、レベルコントロール素子1
7,18,20で各々のビツトに応じた重みづけ
を行う。 The processed signals are sent to amplifiers 13, 14, 1
5, 16, level control element 1
At steps 7, 18, and 20, weighting is performed according to each bit.
超音波素子21,22,23,24に信号を加
えることにより超音波素子の共振周波数と信号に
含まれる基準周波数本実施例では発振器4の周波
数が略々等しく設定されている。次に第2図によ
り各部の信号を説明する。 By applying a signal to the ultrasonic elements 21, 22, 23, and 24, the resonance frequency of the ultrasonic element and the reference frequency included in the signal In this embodiment, the frequency of the oscillator 4 is set to be approximately equal. Next, the signals of each part will be explained with reference to FIG.
入力信号1の波形aをCのようにサンプリング
してAD変換するとbに示すように信号5,6,
7,8はそれぞれLSBをb1としb2,b3および
MSBをb4として4ビツトの並列信号に変換され
る。一方発振器4より超音波周波数正弦波信号d
を出力し、乗算器9,10,11,12で演算処
理すると、それぞれの出力にはd1,d2,d3,d4の
信号を得る。 When waveform a of input signal 1 is sampled as shown in C and AD converted, signals 5, 6,
7 and 8 respectively have LSB as b 1 and b 2 , b 3 and
It is converted into a 4-bit parallel signal with the MSB as b4 . On the other hand, the ultrasonic frequency sine wave signal d from the oscillator 4
is output and processed by multipliers 9, 10, 11, and 12 to obtain signals of d 1 , d 2 , d 3 , and d 4 at the respective outputs.
それぞれのビツトに応じた重みづけをし音響変
換素子の超音波素子21,22,23,24に印
加すると各々の素子からの音波が同相で放射され
ると空気はeの波形の振動をする。 When weights are applied to the ultrasonic elements 21, 22, 23, and 24 of the acoustic transducer with weights depending on the respective bits, when the sound waves from each element are radiated in phase, the air vibrates in a waveform e.
音波の包路線をg(t)とするとこの波形
(t)は
(t)={1+g(t)}coswt
で表わされる。 If the envelope line of the sound wave is g(t), this waveform (t) is expressed as (t)={1+g(t)}coswt.
ただし は超音波素子の共振角周波数である。
この音波はパラメトリツク作用により
P(r,t)=K∂2/r∂t2g(t−r/c)
なる2次音圧を生ずる。 where is the resonant angular frequency of the ultrasonic element.
This sound wave generates a secondary sound pressure of P(r,t)=K∂ 2 /r∂t 2 g(t−r/c) due to parametric action.
ただしγは超音波素子と受音点の間隔、cは音
速、Kは空気密度,非線形定数などで決まる定数
である。 However, γ is the distance between the ultrasonic element and the sound receiving point, c is the speed of sound, and K is a constant determined by air density, nonlinear constant, etc.
g(t)がaのような正弦波であるとわかり易
いが2次音波はeの包絡線g(t)となる。g
(t)の高調波成分を無視すると我々が聞く波形
はのようになる。これは元の入力波形aに等し
い。 It is easy to understand that g(t) is a sine wave like a, but the secondary sound wave is the envelope g(t) of e. g
If we ignore the harmonic components of (t), the waveform we hear will be as follows. This is equal to the original input waveform a.
ただしこの場合に示した振幅変調指数は1と
考えられる。これを小さくするためにはどれか1
つ或いは全部の超音波振動子から超音波成分のみ
の音波を出しておけば良く、これを目的とした超
音波振動子を別に設けておけば良い。 However, the amplitude modulation index shown in this case is considered to be 1. What is the best way to make this smaller?
It is sufficient to emit sound waves of only ultrasonic components from one or all of the ultrasonic transducers, and it is sufficient to separately provide an ultrasonic transducer for this purpose.
また、レベルコントロール素子17,18,1
9,20による重みづけを用いずに超音波素子2
1,22,23,24の入力特性がそれぞれのビ
ツトに対して相当しているものを用いても良い。 In addition, level control elements 17, 18, 1
Ultrasonic element 2 without using weighting by 9, 20
It is also possible to use input characteristics 1, 22, 23, and 24 that correspond to the respective bits.
各ビツトを並列に成し音響変換するので共振周
波数の高い振動素子を得ることができる。また各
音響変換素子の共振周波数に合わせた演算処理に
よる超音波振動周波数を作成し変調することも可
能である。 Since each bit is arranged in parallel for acoustic conversion, a vibrating element with a high resonance frequency can be obtained. It is also possible to create and modulate an ultrasonic vibration frequency through arithmetic processing that matches the resonance frequency of each acoustic transducer element.
第3図は本考案の他の一実施例を示す図で、乗
算器9,10,11,12の出力を重みづけした
後加算器34で合成し増幅器33で増幅し、超音
波振動子35で音響変換する。この場合増幅器は
一個で構成できる。 FIG. 3 is a diagram showing another embodiment of the present invention, in which the outputs of multipliers 9, 10, 11, and 12 are weighted, combined in an adder 34, amplified in an amplifier 33, and to convert the sound. In this case, only one amplifier can be used.
第4図は本考案の他の一実施例を示す図で、第
3図の構成に発振器4よりの信号をレベルコント
ロール素子36でレベル調整して加算器34へ加
えバイアス分とする構成を示す。 FIG. 4 is a diagram showing another embodiment of the present invention, and shows a configuration in which the signal from the oscillator 4 is level-adjusted by a level control element 36 and added to the adder 34 as a bias component in the configuration shown in FIG. 3. .
レベルコントロール素子36でレベル調整する
ので空気の非直線特性に合わせる場合単一の素子
による調整が可能になる。 Since the level is adjusted by the level control element 36, adjustment using a single element is possible when adjusting to the non-linear characteristics of air.
超音波素子35は素子単体であつても良く、ア
レー状に合成したものでも良い。 The ultrasonic element 35 may be a single element or may be composed of an array.
以上の説明は4ビツトで行なつたがビツト数を
増減することも可能である。 Although the above explanation has been made using 4 bits, it is also possible to increase or decrease the number of bits.
上記のように本発明によるとパルス符号変調信
号を超音波素子で再生することにより空気の非線
形パラメトリツク作用を利用する音響再生を可能
と成す。 As described above, according to the present invention, by reproducing a pulse code modulated signal with an ultrasonic element, it is possible to reproduce sound using the nonlinear parametric effect of air.
第1図は本発明の一実施例を示す図、第2図は
各部の波形を説明するための図、第3図、第4図
は本発明の他の一実施例をそれぞれ示す図であ
る。
1……入力信号、2……AD変換器、4……発
振器、5,6,7,8……信号、9,10,1
1,12……乗算器、13,14,15,16,
33……増幅器、17,18,19,20,36
……レベルコントロール素子、21,22,2
3,24,35……超音波素子。
FIG. 1 is a diagram showing one embodiment of the present invention, FIG. 2 is a diagram for explaining waveforms of each part, and FIGS. 3 and 4 are diagrams showing other embodiments of the present invention. . 1... Input signal, 2... AD converter, 4... Oscillator, 5, 6, 7, 8... Signal, 9, 10, 1
1, 12...multiplier, 13, 14, 15, 16,
33...Amplifier, 17, 18, 19, 20, 36
...Level control element, 21, 22, 2
3, 24, 35... Ultrasonic element.
Claims (1)
換された並列信号に電気音響変換器の共振周波数
に略等しい周波数と乗算する乗算器と、乗算され
た並列信号をそれぞれ重み付けする手段と、重み
付けされた並列信号を加算する加算手段と、加算
された信号を電気音響変換器に入力し音響信号に
変換する電気音響変換器を具備し空気の非線形パ
ラメトリツク作用を利用して再生音を得ることを
特徴とするパルス符号変調信号再生装置。 2 重み付けされた並列信号をそれぞれの電気音
響変換器に入力し加算手段を再生音場とした特許
請求の範囲第1項記載のパルス符号変調信号再生
装置。[Claims] 1. An AD converter that AD converts an input signal, a multiplier that multiplies the AD converted parallel signal by a frequency approximately equal to the resonant frequency of the electroacoustic transducer, and the multiplied parallel signal, respectively. It is equipped with a weighting means, an adding means for adding weighted parallel signals, and an electroacoustic transducer that inputs the added signal to an electroacoustic transducer and converts it into an acoustic signal, and utilizes the nonlinear parametric action of air. What is claimed is: 1. A pulse code modulation signal reproducing device which obtains reproduced sound using a pulse code modulation signal. 2. The pulse code modulation signal reproducing device according to claim 1, wherein the weighted parallel signals are input to each electroacoustic transducer and the adding means is a reproduction sound field.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12936583A JPS6021695A (en) | 1983-07-18 | 1983-07-18 | Reproducing device of pulse code modulating signal |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12936583A JPS6021695A (en) | 1983-07-18 | 1983-07-18 | Reproducing device of pulse code modulating signal |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6021695A JPS6021695A (en) | 1985-02-04 |
| JPH0221720B2 true JPH0221720B2 (en) | 1990-05-15 |
Family
ID=15007780
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12936583A Granted JPS6021695A (en) | 1983-07-18 | 1983-07-18 | Reproducing device of pulse code modulating signal |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6021695A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH11164384A (en) | 1997-11-25 | 1999-06-18 | Nec Corp | Super directional speaker and speaker drive method |
| US6850623B1 (en) * | 1999-10-29 | 2005-02-01 | American Technology Corporation | Parametric loudspeaker with improved phase characteristics |
| EP3101907A1 (en) * | 2015-06-01 | 2016-12-07 | Université du Maine | Digital loudspeaker |
-
1983
- 1983-07-18 JP JP12936583A patent/JPS6021695A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6021695A (en) | 1985-02-04 |
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