JPH03268699A - Sound field reproducing method using compressed sound field information - Google Patents
Sound field reproducing method using compressed sound field informationInfo
- Publication number
- JPH03268699A JPH03268699A JP2068824A JP6882490A JPH03268699A JP H03268699 A JPH03268699 A JP H03268699A JP 2068824 A JP2068824 A JP 2068824A JP 6882490 A JP6882490 A JP 6882490A JP H03268699 A JPH03268699 A JP H03268699A
- Authority
- JP
- Japan
- Prior art keywords
- sound field
- time
- information
- ear
- signal
- 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
Links
- 238000000034 method Methods 0.000 title claims description 8
- 238000005314 correlation function Methods 0.000 claims abstract description 11
- 210000005069 ears Anatomy 0.000 abstract description 5
- 230000005236 sound signal Effects 0.000 abstract description 5
- 230000006835 compression Effects 0.000 description 3
- 238000007906 compression Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 1
- SKDHDLDJUMQXEN-UHFFFAOYSA-N triptofordin B Natural products CC1(C)OC23C(O)C1CC(OC(=O)c4ccccc4)C2(C)C(CCC3(C)O)OC(=O)c5ccccc5 SKDHDLDJUMQXEN-UHFFFAOYSA-N 0.000 description 1
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、任意の空間に別の音場を再現するだめの圧縮
音場情報を用いた音場再生方法に関する。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a sound field reproduction method using compressed sound field information for reproducing another sound field in an arbitrary space.
従来の技術
従来、この種の音場再生方法は、−測定された音場のイ
ンパルス応答より、エネルギーの大きいものを選択して
音場の情報量を減少させるように構成されている。これ
は物理的にインパルス応答を再現しようとする方法であ
り、情報圧縮度が小さく十分な情報量がある場合、音場
の印象を再現することかできる。BACKGROUND OF THE INVENTION Conventionally, this type of sound field reproduction method is configured to reduce the amount of information in a sound field by selecting one with larger energy than the measured impulse response of the sound field. This is a method that attempts to physically reproduce the impulse response, and if the degree of information compression is low and there is a sufficient amount of information, it is possible to reproduce the impression of a sound field.
発明が解決しようとする課題
しかしながら、上記従来の音場再生方法では、圧縮度が
高く情報量が減少すると、音場の印象の111現能力が
低下するという問題があった。本発明はこのような従来
の問題を解決するものであり、圧縮度が高く情報量が少
なくても音場の印象を再現できる音場再生方法を提供す
ることを目的とするものである。Problems to be Solved by the Invention However, the conventional sound field reproduction method described above has a problem in that when the degree of compression is high and the amount of information is reduced, the ability to create a sound field impression is reduced. The present invention is intended to solve these conventional problems, and it is an object of the present invention to provide a sound field reproduction method that can reproduce the impression of a sound field even with a high degree of compression and a small amount of information.
課題を解決するだめの手段
本発明は上記目的を達成するために、ダミーヘッドマイ
クロホンの左耳および右耳で測定された音場の情報を時
系列両耳聞相互相関関数を用いて圧縮するようにしたも
のである。Means for Solving the Problems In order to achieve the above object, the present invention compresses sound field information measured at the left and right ears of a dummy head microphone using a time-series binaural cross-correlation function. This is what I did.
作 用
したがって、本発明によれば、ダミーヘッドマイクロホ
ンで測定されたインパルス応答を時系列両耳間相互相関
をもちいて情報圧縮することにより、少ない情報量でも
音場の印象を再現できるという効果を有する。Therefore, according to the present invention, by compressing the impulse response measured with a dummy head microphone using time-series interaural cross-correlation, it is possible to reproduce the impression of a sound field even with a small amount of information. have
実施例
第1図は本発明の一実施例の構成を示すものである。第
1図においてlは再生しようとする音場である。2はイ
ンパルス発生器であり、増幅器3にt# Weされてい
る。4はインパルス応答射するスピーカーである。5に
ダミーヘッドマイクロホンであり、左耳および右耳に相
当する位置で、それぞれインパルス1答を収音する。6
は時系列内耳間相互相関関数計測器であり、ダミーヘッ
ドマイクロホン5の左および右マイクロホンでのインパ
ルス応答より、時系列置耳間相互相関関数を算出する。Embodiment FIG. 1 shows the configuration of an embodiment of the present invention. In FIG. 1, l is the sound field to be reproduced. 2 is an impulse generator, which is connected to the amplifier 3 at t#We. 4 is a speaker that emits an impulse response. 5 is a dummy head microphone, which picks up one impulse at positions corresponding to the left ear and right ear, respectively. 6
is a time-series inter-aural cross-correlation function measuring instrument, which calculates a time-series inter-aural cross-correlation function from the impulse responses at the left and right microphones of the dummy head microphone 5.
7は任意の空間であり、ここで音場を再生する。8は音
声信号源であり、畳み込み演算器9に接続されている。7 is an arbitrary space in which a sound field is reproduced. 8 is an audio signal source, which is connected to a convolution calculator 9;
10Fi増幅器であり、スピーカー11に接続されてい
る。12は聴取者である。It is a 10Fi amplifier and is connected to the speaker 11. 12 is a listener.
動 作
次に、上記実施例の動作について説明する。まず、再生
しようとする音場1において、インパルス発生器2で発
生したインパルス全増幅器3で増幅した後、音源位置に
設(iされたスピーカー4により放射し、聴取位置に設
置されたダミーヘッドマイクロホン5で左および右耳に
相当する位置でのインパルス応答を測定して時系列内耳
間相互相関関数計測器6に出力する。左耳および右耳に
相当する位置でのインパルス応答をそれぞれhNtlお
よびhr(tlとする。時系列両耳間相互相関関数計測
器6においては、i番目の時間窓の時系列置耳間相互相
関関数RCC(i、 τ)を次式を用いて計算する。Operation Next, the operation of the above embodiment will be explained. First, in the sound field 1 to be reproduced, the impulse generated by the impulse generator 2 is amplified by the total amplifier 3, and then radiated by the speaker 4 installed at the sound source position, and then radiated by the dummy head microphone installed at the listening position. 5, the impulse responses at positions corresponding to the left and right ears are measured and output to the time-series inter-cochlear cross-correlation function measuring instrument 6.The impulse responses at positions corresponding to the left and right ears are measured as hNtl and hr, respectively. (tl) The time-series interaural cross-correlation function measuring device 6 calculates the time-series interaural cross-correlation function RCC(i, τ) of the i-th time window using the following equation.
RCC(i、T )=fTwhl(i−1)4”W+t
) ・hr((i−1) ・TW+ t+r ) dt
/[7Twhl”((i−1) ・TW−1−t)d
t ・/”Twhr2((i−1)・TW+t)dtl
”′(1)(t)ここで、時間窓TWは5〜10m5で
あり、両耳間時間差τは一1〜+1msである。RCC(i,T)=fTwhl(i-1)4”W+t
) ・hr((i-1) ・TW+t+r) dt
/[7Twhl”((i-1) ・TW-1-t)d
t ・/”Twhr2((i-1)・TW+t)dtl
``'(1)(t) Here, the time window TW is 5 to 10 m5, and the interaural time difference τ is -1 to +1 ms.
また、各区間のRCCが最大となる時間τ(ifおよび
τ(ifと両耳間時間差が等しくなる方位角ψ(ilを
求める。次に、ダミーヘッドマイクロホン5の左耳およ
び右耳に相当する位置でのインパルス応答より、RC’
Cを計算した各区間内で音圧が最大となる時間△t(i
tを求める。さらに、各区間内のエネルギーE(il′
ff:式2を用いて求める。Also, find the time τ(if) at which the RCC of each section is maximum and the azimuth angle ψ(il) at which the interaural time difference is equal to τ(if). From the impulse response at the position, RC'
The time △t(i
Find t. Furthermore, the energy E(il'
ff: Calculated using Equation 2.
E(il=6−1og2(2””+2Lr/6)
(21ことで、LlおよびLrは、それぞれ各区間内で
のダミーへヴドマイクロホン5の左耳および右耳に相当
する位置での音圧レベルである。E(il=6-1og2(2""+2Lr/6)
(21) Ll and Lr are the sound pressure levels at positions corresponding to the left ear and right ear of the dummy heated microphone 5 in each section, respectively.
このようにして算出した、それぞれの時間遅れ△t (
il、エネルギーE (it、方位角ψ(itの情報は
畳み込み演算器9に入力される。Each time delay Δt (
The information of il, energy E(it, azimuth ψ(it) is input to the convolution calculator 9.
音声信号源8から出力された音声信号は畳み込み演算器
9で畳み込み演算が行われ、増幅器10で増幅した後、
任意の空間7で聴取者12を取り巻くスピーカー11の
うち、方位角ψ(ilが含まれる部分空間にあるスピー
カーから時間遅れ△t(it、エネルギーE(itで提
示される。The audio signal output from the audio signal source 8 is subjected to a convolution operation by a convolution calculator 9, and after being amplified by an amplifier 10,
Among the speakers 11 surrounding the listener 12 in an arbitrary space 7, it is presented with a time delay Δt(it, energy E(it) from a speaker in a subspace including the azimuth angle ψ(il).
効 果
このように、上記実施例によれは、聴取位置に設置され
たダミーヘプトマイクロホン5の左および右耳に相当す
る位置でのインパルス応答を時系列内耳間相互相関関数
計測器6により情報圧縮することにより、少ない情報W
で音場の印象を再現できるという利点を有する。Effects As described above, according to the above embodiment, the impulse response at the positions corresponding to the left and right ears of the dummy Hepto microphone 5 installed at the listening position is measured by the time-series inter-cochlear cross-correlation function measuring device 6. By compressing, less information W
It has the advantage of being able to reproduce the impression of a sound field.
発明の効果
本発明は上記実施例より明らかなように、音場のインパ
ルス応答をダミーヘッドマイクロホンで測定し、さらに
時系列置耳間相互相関関数に情報圧縮するものであり、
少ない情報量で音場の印象を任意の空間に再現できると
いう利点を有する。Effects of the Invention As is clear from the above embodiments, the present invention measures the impulse response of a sound field using a dummy head microphone, and further compresses the information into a time-series inter-ear cross-correlation function.
It has the advantage of being able to reproduce the impression of a sound field in any space with a small amount of information.
第1図は本発明の一実施例における圧縮音場情報を用い
た音場再生方法に使用する構成のブロリク図である。
1・・音場、2・・・インパルス発生器、3・・・増幅
器、4・・スピーカー 5・・・ダミーヘッドマイクロ
ホン、6・・・勝系列両耳間相互相関関数計測器、7・
・・任意の空間、8・・・音声信号源、9・・・畳み込
み演算器、lO・・・増幅器、11・・スピーカー 1
2・・・聴取者。FIG. 1 is a block diagram of a configuration used in a sound field reproduction method using compressed sound field information in an embodiment of the present invention. 1...Sound field, 2...Impulse generator, 3...Amplifier, 4...Speaker 5...Dummy head microphone, 6...Katsu series binaural cross-correlation function measuring device, 7...
...Arbitrary space, 8...Audio signal source, 9...Convolution operator, lO...Amplifier, 11...Speaker 1
2...listener.
Claims (1)
定し、時系列両耳間相互相関関数を用いて音場の情報を
圧縮することにより、その音場の印象を少ない情報量で
任意の別の空間で再現する圧縮音場情報を用いた音場再
生方法。By measuring the impulse response of a sound field with a dummy head microphone and compressing the sound field information using a time-series interaural cross-correlation function, the impression of the sound field can be expressed in any other space with a small amount of information. A sound field reproduction method using compressed sound field information to be reproduced.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2068824A JP2574503B2 (en) | 1990-03-19 | 1990-03-19 | Sound field reproduction method using compressed sound field information |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2068824A JP2574503B2 (en) | 1990-03-19 | 1990-03-19 | Sound field reproduction method using compressed sound field information |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH03268699A true JPH03268699A (en) | 1991-11-29 |
JP2574503B2 JP2574503B2 (en) | 1997-01-22 |
Family
ID=13384846
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2068824A Expired - Fee Related JP2574503B2 (en) | 1990-03-19 | 1990-03-19 | Sound field reproduction method using compressed sound field information |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2574503B2 (en) |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5850812A (en) * | 1981-09-21 | 1983-03-25 | Matsushita Electric Ind Co Ltd | Transmitting circuit for audio signal |
JPS596560A (en) * | 1982-07-02 | 1984-01-13 | Matsushita Electronics Corp | Manufacture of semiconductor device |
JPS6349900U (en) * | 1986-09-19 | 1988-04-04 |
-
1990
- 1990-03-19 JP JP2068824A patent/JP2574503B2/en not_active Expired - Fee Related
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5850812A (en) * | 1981-09-21 | 1983-03-25 | Matsushita Electric Ind Co Ltd | Transmitting circuit for audio signal |
JPS596560A (en) * | 1982-07-02 | 1984-01-13 | Matsushita Electronics Corp | Manufacture of semiconductor device |
JPS6349900U (en) * | 1986-09-19 | 1988-04-04 |
Also Published As
Publication number | Publication date |
---|---|
JP2574503B2 (en) | 1997-01-22 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
LAPS | Cancellation because of no payment of annual fees |