JPS6021695A - Reproducing device of pulse code modulating signal - Google Patents

Reproducing device of pulse code modulating signal

Info

Publication number
JPS6021695A
JPS6021695A JP12936583A JP12936583A JPS6021695A JP S6021695 A JPS6021695 A JP S6021695A JP 12936583 A JP12936583 A JP 12936583A JP 12936583 A JP12936583 A JP 12936583A JP S6021695 A JPS6021695 A JP S6021695A
Authority
JP
Japan
Prior art keywords
signal
pulse code
signals
frequency
ultrasonic wave
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
JP12936583A
Other languages
Japanese (ja)
Other versions
JPH0221720B2 (en
Inventor
Shiyouichi Sasabe
佐々部 昭一
Junichiro Fujimoto
潤一郎 藤本
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.)
Nippon Columbia Co Ltd
Original Assignee
Nippon Columbia 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 Nippon Columbia Co Ltd filed Critical Nippon Columbia Co Ltd
Priority to JP12936583A priority Critical patent/JPS6021695A/en
Publication of JPS6021695A publication Critical patent/JPS6021695A/en
Publication of JPH0221720B2 publication Critical patent/JPH0221720B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K15/00Acoustics not otherwise provided for
    • G10K15/02Synthesis of acoustic waves

Abstract

PURPOSE:To attain the acoustic reproduction utilizing the nonlinear parametric operation of air by reproducing a pulse code modulating signal by an ultrasonic wave element. CONSTITUTION:A signal subject to pulse code modulation from an input signal 1 at an A/D converter 2 is formed as 4 bits; signals 5-8 in order from the lower bit. An oscillator 4 has an oscillating frequency nearly equal to the resonance frequency of ultrasonic wave elements 21-24. The signal of the oscillator 4 and the signals 5-8 are processed for operation by multipliers 9-12. The signals subject to processing operation are amplified by amplifiers 13-16 and the weighting depending on each bit is conducted by level control elements 17-20. The resonance frequency of the ultrasonic wave elements 21-24 and the reference frequency (the frequency of the oscillator 4 in this case) included in the signal 5-8 are set nearly equal by applying the signals to the ultrasonic wave elements 21-24.

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MS
B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」ガ案されている。この場合再生に要する音響変
換器が各ビッ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。
MS of signals converted from conventional analog signals to digital signals
A speaker that uses an acoustic transducer that supports signals from B to LSB is being proposed. In this case, the number of acoustic transducers required for playback corresponds to each bit, which has the disadvantage of complicating the equipment.If multiple coils are attached to the bobbin of one transducer, the conversion efficiency will decrease due to the increased mass. It has the disadvantage of decreasing.

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ック作用を利用して成すも
のである。
The present invention provides a novel device which solves the above-mentioned drawbacks and is achieved by utilizing the non-linear parametric action 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A
D変換器2でパルス符号変調した信号を4ビツトとし、
下位ビットから順に信号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9.10.1
1.12で演算処理する。
FIG. 1 is a diagram showing an embodiment of the present invention, in which input signal 1 is
The signal pulse code modulated by the D converter 2 is 4 bits,
Signals 5, 6°, 7.8. Indicated by The oscillator 4 has an oscillation frequency approximately equal to the resonant frequency of each of the ultrasonic elements 21.2.2.23.24. The signal of the oscillator 4 and the signal 5.6.7.8 are multiplied by the multiplier 9.10.1.
1. Perform calculation processing in 12.

演算処理された信号は増幅器1.3.14.15.16
で増幅シ、レベルコントロール素子17.18.20で
各々のビットに応じた重みづけを行う。
The processed signal is sent to amplifier 1.3.14.15.16
The level control elements 17, 18, and 20 perform weighting 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40周波数が略々等しく設定さ
れている。次に第2図によりように信号5.6.7.8
はそれぞれLSBをb’l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。一方弁
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’di、 d2. d3. d4の信号を得る
By applying a signal to the ultrasonic elements 21, 22, 23, 24, the resonant frequency of the ultrasonic element and the reference frequency included in the signal In this embodiment, the frequency of the oscillator 40 is set to be approximately equal. Then signal 5.6.7.8 as per figure 2
b'l is the LSB, b2゜b3 and the MSB, respectively.
is converted into a 4-bit parallel signal as b4. On the other hand, the valve vibrator 4 outputs an ultrasonic frequency sine wave signal d, and the multiplier 9.10. When the calculation is performed in '11.12, each output has 'di, d2. d3. Obtain the d4 signal.

それぞれのピッI−一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 each pitch is weighted accordingly and applied to the ultrasonic elements 21', 22, 23, and 24 of the acoustic transducer, the sound waves from each element are radiated in phase, and the air vibrates with a waveform of e. do.

音波の包絡線を7(71とするとこの波形子(わけで表
わされる。
If the envelope of a sound wave is 7 (71), it is expressed by this waveform element.

ただし は超音波素子の共振角周波数である。However, is the resonance angular frequency of the ultrasonic element.

なる2次音圧を生ずる。This produces a secondary sound pressure of

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.

7(hがaのような正弦波であるとわかり易いが2次音
波は・0の包絡嬬(t)となる。グ■の高調波成分を無
視すると極々か聞く波形は÷のようになる。これは元の
入力波形aに等しい。
7 (It is easy to understand that h is a sine wave like a, but the secondary sound wave has an envelope (t) of 0. If the harmonic component of 3 is ignored, the waveform that can be heard at the extreme becomes ÷. This is equal to the original input waveform a.

ただしこの場合士に示し7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1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, in this case, the amplitude modulation index shown in Figure 7 is considered to be 1. In order to reduce this, it is possible to emit a sound wave containing only ultrasonic components from one or all of the ultrasonic transducers, and it is necessary to provide a separate ultrasonic transducer for this purpose. good.

また、レベルコントロール素子17.18.19.20
による重みづけを用いずに超音波素子2.1.22゜2
3、24の入力特性がそれぞれのピッ) I/(対して
相当しているものを用いても良い。
Also, level control element 17.18.19.20
Ultrasonic element 2.1.22゜2 without weighting by
It is also possible to use input characteristics corresponding to the input characteristics of 3 and 24 for each pitch.

各ビッ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1ffit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 and acoustically converted, a vibrating element with a high resonant frequency can be obtained. It is also possible to create and modulate an ultrasonic vibration frequency by 1ffit calculation 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 a multiplier 9.
After weighting the outputs of 10, 11, and 12, they are combined by an adder 34, amplified by an amplifier 33, and acoustically converted by an ultrasonic transducer 35. 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, in which the signal from the oscillator 4 is transferred to the level control element 36 in the configuration shown in FIG.
A configuration is shown in which the level is adjusted and added to the adder 34 as a bias amount.

レベルコントロール素子36でレベル調整スルので空気
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は素子単体であっても良く、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 a combination of elements in an array.

以上の説明は4ビツトで行なったがビット数を増減する
ことも可能で入る。
Although the above explanation has been made using 4 bits, it is 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1. 
IIラック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, nonlinear parameters of air can be determined.
This makes it possible to reproduce sound using II racks.

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

第1図は本発明の一実施例を示す図、第2図は各部の波
形を説明するだめの図、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、9.10.11.、12・・・・・・乗算器、13
.14.15.16.33・・・・・・増幅器、17.
18.19.2(1゜36・・・・・・レベルコントロ
ール素子、21.22.23.24゜35・・・・・・
超音波素子 出願人 日本コロムビア株式会社 代理人 弁理士 山 口 和 美 ゛・・几惺゛: 、5)5戸・ 修l目 112図
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, 9.10.11. , 12... Multiplier, 13
.. 14.15.16.33...Amplifier, 17.
18.19.2 (1゜36... Level control element, 21.22.23.24゜35...
Ultrasonic device applicant: Nippon Columbia Co., Ltd. Agent: Kazumi Yamaguchi, patent attorney: 5) 5 houses/School 112

Claims (1)

【特許請求の範囲】[Claims] 入力信号をパルス符号変調し演算処理した信号を空気の
非線形パラメトリック作用を利用したスピーカに加え該
信号に含まれる基準周波数を該スピーカの共振周波数に
略々等しく成すことを特徴とするどくルス符号変調信号
再生装置。
A pulse code modulated signal, which is characterized in that a signal obtained by pulse code modulating an input signal and processing it is applied to a speaker that utilizes the nonlinear parametric effect of air, and the reference frequency included in the signal is made approximately equal to the resonant frequency of the speaker. playback device.
JP12936583A 1983-07-18 1983-07-18 Reproducing device of pulse code modulating signal Granted JPS6021695A (en)

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 true JPS6021695A (en) 1985-02-04
JPH0221720B2 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)

Cited By (3)

* Cited by examiner, † Cited by third party
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
JP2018518110A (en) * 2015-06-01 2018-07-05 ユニベルシテ ドゥ メーヌ Digital speaker

Cited By (4)

* Cited by examiner, † Cited by third party
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
US6678381B1 (en) 1997-11-25 2004-01-13 Nec Corporation Ultra-directional speaker
US6850623B1 (en) * 1999-10-29 2005-02-01 American Technology Corporation Parametric loudspeaker with improved phase characteristics
JP2018518110A (en) * 2015-06-01 2018-07-05 ユニベルシテ ドゥ メーヌ Digital speaker

Also Published As

Publication number Publication date
JPH0221720B2 (en) 1990-05-15

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