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JPS6217302B2 - - Google Patents
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JPS6217302B2 - - Google Patents

Info

Publication number
JPS6217302B2
JPS6217302B2 JP5989080A JP5989080A JPS6217302B2 JP S6217302 B2 JPS6217302 B2 JP S6217302B2 JP 5989080 A JP5989080 A JP 5989080A JP 5989080 A JP5989080 A JP 5989080A JP S6217302 B2 JPS6217302 B2 JP S6217302B2
Authority
JP
Japan
Prior art keywords
signal
signal path
sub
main
compression
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
Application number
JP5989080A
Other languages
Japanese (ja)
Other versions
JPS56157135A (en
Inventor
Yoshuki Takizawa
Fumihiko Yokogawa
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.)
Pioneer Corp
Original Assignee
Pioneer Electronic Corp
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 Pioneer Electronic Corp filed Critical Pioneer Electronic Corp
Priority to JP5989080A priority Critical patent/JPS56157135A/en
Publication of JPS56157135A publication Critical patent/JPS56157135A/en
Publication of JPS6217302B2 publication Critical patent/JPS6217302B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03GCONTROL OF AMPLIFICATION
    • H03G9/00Combinations of two or more types of control, e.g. gain control and tone control
    • H03G9/02Combinations of two or more types of control, e.g. gain control and tone control in untuned amplifiers
    • H03G9/025Combinations of two or more types of control, e.g. gain control and tone control in untuned amplifiers frequency-dependent volume compression or expansion, e.g. multiple-band systems

Landscapes

  • Signal Processing Not Specific To The Method Of Recording And Reproducing (AREA)
  • Reduction Or Emphasis Of Bandwidth Of Signals (AREA)

Description

【発明の詳細な説明】 本発明は雑音が信号に導入される伝送路、或は
磁気記録再生装置に用いられる信号の圧縮及び伸
長回路に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a signal compression and expansion circuit used in a transmission line in which noise is introduced into a signal or in a magnetic recording/reproducing device.

一般に音声信号を扱う伝送媒体の中でも磁気記
録再生を行うテープデツキにおいては、磁気テー
プ等の制約からそのSN比は50〜60dB程度であ
る。この為圧縮器と伸長器とを備えた雑音の低減
装置、いわゆるノイズリダクシヨン装置が用いら
れている。この中でも代表的なものとして和差方
式と呼ばれているノイズリダクシヨン装置があ
る。
Among transmission media that generally handle audio signals, tape decks that perform magnetic recording and reproduction have an S/N ratio of about 50 to 60 dB due to limitations of magnetic tape and the like. For this purpose, a noise reduction device including a compressor and an expander, a so-called noise reduction device, is used. Among these, a typical one is a noise reduction device called a sum-difference method.

第1図はこの方式のノイズリダクシヨン装置の
概略構成図であり、圧縮器1では信号X1を利得
1で通過させる主信号路11と、信号X1を非線
形に変形させる為の伝達関数F(S)を有する副
信号路12とを備え、通過した各々の信号をフイ
ードホワード的に加算回路13にて加算し、レベ
ル圧縮信号Y1を得、また伸長器では利得1の主
信号路21を通過した信号を伝達関数F(S)を
有する副信号路22を通してフイードバツク的に
減算回路23にて減算しレベル伸長信号Z1を得る
ように構成されている。図中Tは伝送媒体、例え
ばテープデツキ等の磁気記録再生装置である。こ
のときの入出力信号の関係は次のようになる。
FIG. 1 is a schematic diagram of a noise reduction device using this method. The compressor 1 includes a main signal path 11 that passes the signal X 1 with a gain of 1, and a transfer function F that nonlinearly transforms the signal X 1 . (S), each passing signal is added in an adder circuit 13 in a feedforward manner to obtain a level compressed signal Y 1 , and the main signal path 21 with a gain of 1 is added in an expander. The passed signal is passed through a sub-signal path 22 having a transfer function F(S) and is subtracted by a subtraction circuit 23 in a feedback manner to obtain a level expanded signal Z1 . In the figure, T is a transmission medium, for example, a magnetic recording/reproducing device such as a tape deck. The relationship between input and output signals at this time is as follows.

Y1={1+F(S)}X1 Z1=1/{1+F(S)}Y1 従つて信号X1=レベル伸長信号Z1となり、入
力信号X1と出力信号Z1とが同一となるものであ
る。
Y 1 = {1+F(S)}X 1 Z 1 = 1/{1+F(S)}Y 1 Therefore, signal X 1 = level expanded signal Z 1 , and input signal It is what it is.

また第2図は第1図の副信号路の具体的構成図
を示したものでハイパスフイルタHPFと、副信
号路増幅器As及び帰還系に接続される利得xの
電圧利得制御器VCA、および積分器Iで構成さ
れる。電圧利得制御器VCAの利得xは出力信号
V0(S)の高域成分を直流に変換して得られる
制御電圧Vcで制御される(直流変換部は図示せ
ず)。第2図より副信号路の伝達関数F(S)は
次のようになる。
Furthermore, Fig. 2 shows a specific configuration diagram of the sub-signal path in Fig. 1, including a high-pass filter HPF, a sub-signal path amplifier As, a voltage gain controller VCA with a gain of x connected to the feedback system, and an integrator. It consists of vessel I. The gain x of the voltage gain controller VCA is the output signal
It is controlled by a control voltage Vc obtained by converting the high frequency component of V 0 (S) into direct current (the direct current converter is not shown). From FIG. 2, the transfer function F(S) of the sub-signal path is as follows.

この式よりVCAの利得xの変化に伴なつて、
遮断角周波数R/Rxωが移動することになり、 入力信号に対応した周波数特性が得られ、この種
のノイズリダクシヨン装置においては加算或は減
算後の信号が5KHz以上で最大10dBのレベル変化
を得られるようになつている。
From this formula, as the VCA gain x changes,
The cut-off angular frequency R 2 /R 30 moves, and a frequency characteristic corresponding to the input signal is obtained, and in this type of noise reduction device, the signal after addition or subtraction is 10 dB at maximum at 5 KHz or higher. Now you can get level changes.

しかしながら、このような加算或は減算による
和差方式の雑音低減装置においては、高い入力レ
ベルでは圧縮伸長が成されない為に高い周波数領
域では磁気テープの飽和が生じ、ダイナミツクレ
ンジの改善を成し得ない欠点があつた。
However, in such a noise reduction device using a sum-difference method using addition or subtraction, compression and expansion are not performed at high input levels, so saturation of the magnetic tape occurs in the high frequency range, making it difficult to improve the dynamic range. There were disadvantages that I could not get.

本発明は上述の点に鑑み成されたもので、その
目的はこのような問題を解決しようとするもので
あり、高い周波数領域での高い入力信号において
も圧縮及び伸長を実現することができる信号の圧
伸回路を提供するものである。
The present invention has been made in view of the above-mentioned points, and its purpose is to solve such problems, and to provide a signal that can be compressed and expanded even with high input signals in a high frequency region. This provides a companding circuit.

以下、図面に基づき本発明を説明する。 The present invention will be explained below based on the drawings.

第3図は本発明の概略構成図である。第1図と
同一のものは同記号を用いてある。圧縮器1で
は、入力信号X2は伝達関数K(S)を有する主
信号路11′を通過すると共に、伝達関数F
(S)を有する副信号路12を通過してフイード
ホワード的に加算されてレベル圧縮信号Y2が、
また伸長器2では伝達関数1/K(S)を有する
主信号路21′を通過した信号を伝達関数F
(S)を有する副信号路22を通してフイードバ
ツク的に減算されレベル伸長信号Z2が得られる。
入出力信号の関係を次式に示す。
FIG. 3 is a schematic configuration diagram of the present invention. Components that are the same as those in FIG. 1 are designated by the same symbols. In the compressor 1 , the input signal
(S) and is added in a feedforward manner, and the level compressed signal Y 2 is
Further, in the expander 2, the signal passing through the main signal path 21' having a transfer function 1/K(S) is converted into a transfer function F.
(S) is subtracted in a feedback manner through the sub-signal path 22, and a level expanded signal Z2 is obtained.
The relationship between input and output signals is shown in the following equation.

Y2={K(S)+F(S)}X2,Z2 =1/{K(S)+F(S)}Y2 これより、信号X2=レベル伸長信号Z2とな
り、入力信号X2と同一な出力信号Z2が得られ
る。
Y 2 = {K(S)+ F (S)}X 2 , Z 2 = 1/{K(S)+ F(S)}Y 2 From this, signal An output signal Z 2 identical to 2 is obtained.

ここで、伝達関数K(S)を第4図に示す具体
回路例のように構成すると、このときの伝達関数
K(S)は K(S)=v/vi(S)=−R(S+ω)/S+
Rω 但し ω=1/C,R=2R/2R
+R となり、第5図に示すような特性を得ることがで
きる。この伝達関数K(S)と前記伝達関数F
(S)との加算出力は第8図の実線に示す周波数
特性となり、高い周波数領域での高い入力信号に
おいてもレベル圧縮が可能になる。なお第8図の
破線は従来の和差方式のノイズリダクシヨン装置
における周波数特性である。
Here, if the transfer function K(S) is configured as shown in the specific circuit example shown in FIG. S+ ω1 )/S+
1 However, ω 1 = 1/C 1 R 1 , R = 2R 1 /2R 1
+ R2 , and the characteristics shown in FIG. 5 can be obtained. This transfer function K(S) and the transfer function F
The output of addition with (S) has a frequency characteristic shown by the solid line in FIG. 8, and level compression is possible even for high input signals in a high frequency region. The broken line in FIG. 8 is the frequency characteristic of a conventional sum-difference type noise reduction device.

次に伸長器の主信号路伝達関数1/K(S)は
第6図に示す具体回路例で構成することができ
る。1/K(S)は次式で示される。
Next, the main signal path transfer function 1/K(S) of the expander can be constructed using a specific circuit example shown in FIG. 1/K(S) is expressed by the following formula.

1/K(S)=v′/vi′(S)=−S+Rω
R(S+ω) 但し ω=1/C,R=2R/2R
+R この周波数特性は第7図に示すようになり、圧
縮時と相補な関係が得られる。第8図に示す周波
(Hz)における、圧縮及び伸長時の入力出
特性を第9図に示す。なお破線は従来のノイズリ
ダクシヨン装置における入出力特性である。
1/K(S)= v0 '/vi'(S)=-S+ Rω1 /
R(S+ω 1 ) where ω 1 =1/C 1 R 1 , R=2R 1 /2R 1
+R 2 This frequency characteristic is as shown in FIG. 7, and a complementary relationship to that during compression is obtained. FIG. 9 shows the input/output characteristics during compression and expansion at frequency 1 (Hz) shown in FIG. 8. Note that the broken line represents the input/output characteristics of the conventional noise reduction device.

なお、上記した周波数特性は、圧縮側では低域
増強形、伸長側では高域増強形になされている。
Note that the frequency characteristics described above are of a low frequency enhanced type on the compression side and a high frequency enhanced type on the expansion side.

以上述べたように本発明によれば、磁気テー
プ、ヘツド等に起因する磁気記録再生装置の欠点
である高域の狭いダイナミツクレンジを拡大する
ことが可能となり、従来のノイズリダクシヨン装
置のような雑音低減効果だけではなく、磁気テー
プの飽和による歪の発生を防ぐなどの利点が得ら
れる。
As described above, according to the present invention, it is possible to expand the narrow dynamic range in the high range, which is a drawback of magnetic recording and reproducing devices caused by magnetic tapes, heads, etc. This not only provides a significant noise reduction effect, but also has the advantage of preventing distortion due to saturation of the magnetic tape.

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

第1図は従来のノイズリダクシヨン装置の概略
構成を示す回路図、第2図は副信号路の具体的構
成を示す回路図、第3図は本発明による圧縮及び
伸長回路の概略を示す回路図、第4図及び第6図
は第3図における圧縮器及び伸長器の主信号路の
一実施例を示す回路図、第5図及び第7図は第4
図及び第5図に係る主信号路の構成における周波
数特性図、第8図は圧縮器出力の周波数特性図、
第9図は圧縮及び伸長時の入出力特性図である。 1……圧縮器、2……伸長器、11′,21′…
…主信号路、12,22……副信号路。
FIG. 1 is a circuit diagram showing a schematic configuration of a conventional noise reduction device, FIG. 2 is a circuit diagram showing a specific configuration of a sub-signal path, and FIG. 3 is a circuit diagram showing an outline of a compression and expansion circuit according to the present invention. 4 and 6 are circuit diagrams showing one embodiment of the main signal path of the compressor and expander in FIG.
FIG. 8 is a frequency characteristic diagram of the main signal path configuration according to FIG.
FIG. 9 is an input/output characteristic diagram during compression and expansion. 1... Compressor, 2... Expander, 11', 21'...
...Main signal path, 12, 22...Sub signal path.

Claims (1)

【特許請求の範囲】[Claims] 1 信号を線形のまま通過させる主信号路と、増
幅器とハイパスフイルタと電圧利得制御器と積分
器とを有して信号を非線形に変形させる副信号路
とを具備し、主信号路と副信号路より得られる
各々の信号をフイードホワード的に加算して信号
のレベル圧縮を行い、また主信号路を通過した信
号を副信号路を通してフイードバツク的に減算し
て信号のレベル伸長を行うように構成された和差
方式による信号の圧縮及び伸長装置において、圧
縮側と伸長側の主信号にあつて相補な周波数特性
を有するように、圧縮側では低域増強形、伸長側
では高域増強形としたことを特徴とする信号の圧
伸回路。
1 A main signal path through which the signal passes linearly, and a sub-signal path which includes an amplifier, a high-pass filter, a voltage gain controller, and an integrator to transform the signal into a non-linear form, and the main signal path and the sub-signal path The signal level is compressed by adding each signal obtained from the main signal path in a feed-forward manner, and the signal that has passed through the main signal path is subtracted in a feedback manner through a sub-signal path to expand the signal level. In a signal compression and expansion device using the sum-difference method, the compression side is a low-frequency amplification type and the expansion side is a high-frequency amplification type, so that the main signals on the compression side and expansion side have complementary frequency characteristics. A signal companding circuit characterized by:
JP5989080A 1980-05-08 1980-05-08 Companding circuit of signal Granted JPS56157135A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5989080A JPS56157135A (en) 1980-05-08 1980-05-08 Companding circuit of signal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5989080A JPS56157135A (en) 1980-05-08 1980-05-08 Companding circuit of signal

Publications (2)

Publication Number Publication Date
JPS56157135A JPS56157135A (en) 1981-12-04
JPS6217302B2 true JPS6217302B2 (en) 1987-04-16

Family

ID=13126159

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5989080A Granted JPS56157135A (en) 1980-05-08 1980-05-08 Companding circuit of signal

Country Status (1)

Country Link
JP (1) JPS56157135A (en)

Also Published As

Publication number Publication date
JPS56157135A (en) 1981-12-04

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