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JPS6038896B2 - Frequency characteristic correction circuit - Google Patents
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JPS6038896B2 - Frequency characteristic correction circuit - Google Patents

Frequency characteristic correction circuit

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Publication number
JPS6038896B2
JPS6038896B2 JP5197178A JP5197178A JPS6038896B2 JP S6038896 B2 JPS6038896 B2 JP S6038896B2 JP 5197178 A JP5197178 A JP 5197178A JP 5197178 A JP5197178 A JP 5197178A JP S6038896 B2 JPS6038896 B2 JP S6038896B2
Authority
JP
Japan
Prior art keywords
correction circuit
resistor
phase
frequency characteristic
case
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
JP5197178A
Other languages
Japanese (ja)
Other versions
JPS54144161A (en
Inventor
奉文 中谷
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 JP5197178A priority Critical patent/JPS6038896B2/en
Publication of JPS54144161A publication Critical patent/JPS54144161A/en
Publication of JPS6038896B2 publication Critical patent/JPS6038896B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は周波数特性補正回路(以下補正回路とする。[Detailed description of the invention] The present invention relates to a frequency characteristic correction circuit (hereinafter referred to as a correction circuit).

)に関する。従来の補正回路としては例えば第1図の様
な高城補正回路等が公知であった。
) regarding. As a conventional correction circuit, for example, a Takagi correction circuit as shown in FIG. 1 has been known.

図において21は入力端子22,24は抵抗、23はボ
リューム、26,27はコンデンサ、25は出力端子で
ある。この場合出力端子25における位相特性は、第2
図に示す様に低域及び高城周波数では00であるが、中
城周波数ではボリューム23の設定位置に応じて位相が
大幅に変化する。従って左右2チャンネルを有するオー
ディオアンプ等において、上述のような補正回路を各チ
ャンネル毎に挿入すると、各補正回路の特性設定状態に
応じて、位相差も第2図の様に異なるから、中城周波数
では左右のチャンネル間位相差が非常に大きくなる。
In the figure, 21 is an input terminal 22, 24 is a resistor, 23 is a volume, 26, 27 is a capacitor, and 25 is an output terminal. In this case, the phase characteristic at the output terminal 25 is
As shown in the figure, the phase is 00 at the low frequency and Takagi frequency, but the phase changes significantly depending on the setting position of the volume 23 at the Nakagusuku frequency. Therefore, in an audio amplifier having two left and right channels, if a correction circuit as described above is inserted for each channel, the phase difference will differ as shown in Figure 2 depending on the characteristic settings of each correction circuit. In terms of frequency, the phase difference between the left and right channels becomes very large.

本発明の目的は上述の様な欠点のない補正回路を提供す
ることにあり、以下図面に従って詳細に説明する。
An object of the present invention is to provide a correction circuit free from the above-mentioned drawbacks, and will be described in detail below with reference to the drawings.

第3図は本発明による高城補正回路の一実施例である。FIG. 3 shows an embodiment of the Takagi correction circuit according to the present invention.

図において入力端子1に印加された入力信号は2分岐し
て、一方は抵抗2を介して広帯域増幅器4の反転端子6
に印加され、他方は可変抵抗器8とコンデンサー9の分
圧回路を介して広帯域増幅器4の非反転端子7に加えら
れる。増幅器4の出力は、出力端子5に接続されると共
に、可変抵抗器3を介して反転端子6に帰還されている
。又可変抵抗器3及び8は運動になされている。
In the figure, the input signal applied to the input terminal 1 is branched into two branches, one being connected to the inverting terminal 6 of the broadband amplifier 4 via the resistor 2.
and the other is applied to the non-inverting terminal 7 of the broadband amplifier 4 via a voltage divider circuit including a variable resistor 8 and a capacitor 9. The output of the amplifier 4 is connected to an output terminal 5 and fed back to an inverting terminal 6 via a variable resistor 3. Also, variable resistors 3 and 8 are put into motion.

この様な回路において、今抵抗2の抵抗値をRoとし、
可変抵抗器3及び8の抵抗設定値をそれぞれKRo及び
Rとし、コンデンサ9の容量をCとし、入力信号の角速
度をwとするとこの回路の伝達函数G(W)はGM=三
笠叢R .・・.・則 従ってこの位相特性argG(jw)は arg○(iw)=一(tan【IKwCR+ねn‐I
WCR),..,..■今度速度wがwoとなる点で位
相が900になるものとすると、前記分圧回路の時定数
CRは‘2)式より1 ..・
・・・‘3’CR=両雨となる。
In such a circuit, let the resistance value of resistor 2 be Ro,
Let the resistance setting values of the variable resistors 3 and 8 be KRo and R, respectively, the capacitance of the capacitor 9 be C, and the angular velocity of the input signal be w, then the transfer function G(W) of this circuit is GM=Mikasaso R.・・・.・Accordingly, this phase characteristic argG(jw) is arg○(iw)=1(tan[IKwCR+nen-I
WCR),. .. 、. .. ■If we assume that the phase becomes 900 at the point where the speed w becomes wo, the time constant CR of the voltage dividing circuit is 1. ..・
...'3'CR = both rain.

今{3}式を{1ー式に代入して振幅特性を求めるとと
なり、又この場合の位相特性は湖式を‘2}式に代入し
てargG(iW)=−tan‐1党K−tan−・(
希)・R・…側 となる。
Now, by substituting equation {3} into equation {1-, the amplitude characteristic is obtained, and in this case, the phase characteristic is obtained by substituting the lake equation into equation '2} to obtain argG(iW)=-tan-1 party K. -tan-・(
Rare)・R・…side.

よって前記分圧回路の時定数CRを、Kの変化に応じて
{3}式の関係を保つ様に連動変化させると、振幅特性
はKの各値に応じて■式に従って変化して第4図の様に
なることがわかる。
Therefore, if the time constant CR of the voltage divider circuit is changed in accordance with the change in K so as to maintain the relationship of equation {3}, the amplitude characteristic will change according to the equation (2) according to each value of K, and the fourth You can see that it looks like the figure.

なおKの値は高城に対する増幅度に等しいのでこれをデ
シベル換算して図中に示した。又位相特性はKの値に応
じて‘5}式に従って変化し第5図の様になり、角速度
の低域においてはほぼoo角速度woにおいては−90
o、高域においてはほぼ−1800となり、Kの値を変
化させてもこの関係に変化はない。上述の周波数の3つ
のポイント以外の部分では、前記Kの値に応じて若干の
位相特性の変動を生ずるが、第2図に示した従来例にお
ける様な大幅な位相の変動を生ずることはない。第6図
は上述の実施例においてKが1の場合を基準とい・肋3
.16(十1瓜b)拠点(−IMb)の場合と、Kが2
(十母b)又は芸(−&&)の場合の特性の変化分を示
したもので、この場合最大士4.50程度の位相差しか
生じないことがわかる。
Note that since the value of K is equal to the degree of amplification with respect to Takagi, it is converted into decibels and shown in the figure. In addition, the phase characteristic changes according to the equation '5} according to the value of K, as shown in Figure 5, and in the low range of angular velocity it is approximately oo and -90 at angular velocity wo.
o, it becomes approximately -1800 in the high range, and this relationship does not change even if the value of K is changed. In areas other than the three frequency points mentioned above, slight fluctuations in phase characteristics occur depending on the value of K, but there is no large fluctuation in phase as in the conventional example shown in Figure 2. . Figure 6 is based on the case where K is 1 in the above embodiment.
.. In the case of 16 (11 melon b) bases (-IMb) and K is 2
It shows the change in characteristics in the case of (10 mob) or gei (-&&), and it can be seen that in this case, only a maximum phase difference of about 4.50 occurs.

従って多チャンネル増幅器において、各チャンネルの各
々に上述の様な補正回路を用いれば、これら各補正回路
の調整状態を互いに関連なく設定しても、各チャンネル
間の位相差は非常に少ないことがわかる。
Therefore, in a multi-channel amplifier, if a correction circuit such as the one described above is used for each channel, it can be seen that even if the adjustment states of these correction circuits are set independently of each other, the phase difference between each channel will be very small. .

第7図に本発明による低域補正回路の−実施例を示す。FIG. 7 shows an embodiment of the low frequency correction circuit according to the present invention.

即ち本実施例は第3図の実施例における前記分圧回路の
コンデンサ9と抵抗8との接続を逆にしたもので、他に
変るところはないので理解を容易にするため共通部分に
ついては共通符号を付し構成についてのさらに詳細な説
明は省略する。この様な回路の伝達函数G(ふ)はG(
ふ)=・K−WCR ,.・.・・{611
十jwCRとなり、位相特性argG(jw)は argG(iW)=tan−・鱗側…R・・・・・・‘
7)となる。
That is, in this embodiment, the connection between the capacitor 9 and the resistor 8 of the voltage dividing circuit in the embodiment shown in FIG. A more detailed explanation of the reference numerals and configurations will be omitted. The transfer function G(fu) of such a circuit is G(
f)=・K-WCR,.・.. ...{611
1jwCR, and the phase characteristic argG(jw) is argG(iW)=tan-・Scale side...R...'
7).

従って今角速度wがwoとなる点において位相が900
になるものとすると、分圧回路の時定数CRは【7}式
よりCR=−−ゾR ・・・
・・・‘8}Woとなり{8}式を{6)式に代入する
と 又棚式を【7}式に代入すると、 argG(iW)=tan‐1偽未刊n−・億ノK‐‐
‐‐‐‐{IQとなる。
Therefore, at the point where the angular velocity w becomes wo, the phase is 900
Assuming that, the time constant CR of the voltage divider circuit is given by formula [7} as CR=--ZR...
...'8}Wo, and substituting the {8} formula into the {6) formula, and substituting the shelf formula into the [7} formula, argG(iW)=tan-1 false unpublished n-・billion no K--
‐‐‐‐{It becomes IQ.

従って第3図の実施例における場合と同様に、分圧回路
の時定数CRをKの変化に応じて(8}式の関係を保つ
ように連動して変化させれば、Kの値に対する振幅特性
の変化は第8図の様になる。又位相特性は第9図の様に
なり周波教の低域においてはほぼ1800、角速度w。
においては900高域においてはほぼ00となり、Kの
値を変化ざせてもこの関係に変化はない。上述の3つの
ポイント以外の部分ではKの値に応じて若干の位相の変
化を生するが、第3図の実施例と同様にこの変化は非常
に小さい。
Therefore, as in the case of the embodiment shown in FIG. The change in characteristics is as shown in Figure 8.The phase characteristic is as shown in Figure 9, with an angular velocity of approximately 1800 and an angular velocity w in the low frequency range.
is almost 00 in the 900 high range, and this relationship does not change even if the value of K is changed. In areas other than the three points mentioned above, a slight change in phase occurs depending on the value of K, but as in the embodiment of FIG. 3, this change is very small.

第10図に本実施例においてKが1の場合を基準として
■3・16(十IMb)又‘ま太(「Mb)の場合と、
Kが2(十紅b)又は享(一成b)の場合との位相特性
の変動分を示す。
Fig. 10 shows the case of ■ 3.16 (10 IMb) or 'Matai ('Mb)', based on the case where K is 1 in this embodiment, and
It shows the variation in phase characteristics when K is 2 (Jukoku b) or Kyo (Issei b).

以上の実施例ではコンデンサ9の容量Cを固定にし、可
変抵抗器8の抵抗値を、第3図の実施例の場合はノKに
反比例させ、第7図の実施例の場合はノKに正比例する
様にそれぞれ設定したものであるが、抵抗値Rを固定に
し、容量Cを第3図の場合はノKに反比例、第7図の場
合はノKに正比例する様に設定してもよい。
In the above embodiments, the capacitance C of the capacitor 9 is fixed, and the resistance value of the variable resistor 8 is made inversely proportional to K in the embodiment shown in FIG. 3, and to K in the embodiment shown in FIG. Although they are set to be directly proportional to each other, it is also possible to fix the resistance value R and set the capacitance C to be inversely proportional to K in the case of Figure 3, and directly proportional to K in the case of Figure 7. good.

又例えば第3図の場合、抵抗3の各Kの値K,,K2・
・・Knに対応する抵抗値K,,Ro,K2Ro…Kn
Roを切換スイッチにより切換る様にし、これと連動し
た切換スイッチにより抵抗8の抵抗値RI 1 端
W。
For example, in the case of FIG. 3, the values of each K of the resistor 3 are K,,K2・
...Resistance value K,, Ro, K2Ro...Kn corresponding to Kn
Ro is changed over by a changeover switch, and the resistance value RI 1 end W of the resistor 8 is changed by the changeover switch interlocked with this changeover switch.

cの女。く切換るを瓜w。A woman of c. It's a good idea to switch quickly.

C脇w。C様にしてもよい。C side lol. You may choose Mr. C.

第7図の場合についても同様である。The same applies to the case of FIG.

なお角速度woは、上述において固定した容量C又は抵
抗Rの値を変えることにより容易に変えることが出来る
。又Kの値は入力抵抗2を可変抵抗器にすることにより
変えることも出来る。
Note that the angular velocity wo can be easily changed by changing the value of the capacitance C or the resistance R fixed in the above. The value of K can also be changed by using a variable resistor as the input resistor 2.

この場合は入力抵抗2と例えば可変抵抗器8とを連動可
変にすればよい。以上のように本発明によれば各周波数
特性補正回路の調整状態が各々異なつていてもチャンネ
ル間の位相差が小さいので音像定位の不確実さを除くこ
とが出来る。
In this case, the input resistor 2 and, for example, the variable resistor 8 may be made variable in conjunction with each other. As described above, according to the present invention, even if the adjustment states of the frequency characteristic correction circuits are different from each other, the phase difference between channels is small, so that uncertainty in sound image localization can be eliminated.

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

第1図は従来の周波数特性補正回路、第2図はその位相
特性図、第3図は本発明の一実施例を示す回路図、第4
図、第5図及び第6図はその特性を示す線図、第7図は
本発明の他の実施例を示す回路図、第8図、第9図及び
第10図はその特性を示す線図である。 第1図 第2図 第3図 第4図 第5図 第6図 第7図 第8図 第9図 第10図
Fig. 1 is a conventional frequency characteristic correction circuit, Fig. 2 is a phase characteristic diagram thereof, Fig. 3 is a circuit diagram showing an embodiment of the present invention, and Fig. 4 is a circuit diagram showing an embodiment of the present invention.
Figures 5 and 6 are line diagrams showing its characteristics, Figure 7 is a circuit diagram showing another embodiment of the present invention, and Figures 8, 9 and 10 are line diagrams showing its characteristics. It is a diagram. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 Figure 8 Figure 9 Figure 10

Claims (1)

【特許請求の範囲】[Claims] 1 第1及び第2の入力端子を有する差動増幅手段と、
上記第1及び第2の入力端子に入力信号を印加する第1
及び第2の入力抵抗と、上記第2の入力端子を接地する
コンデンサと、上記差動増幅手段の出力を前記第1の入
力端子に負帰還する負帰還手段とを有し、前記第2の抵
抗とコンデンサによる時定数と前記負帰還手段の帰還係
数とを連動可変にしたことを特徴とする周波数特性補正
回路。
1 differential amplification means having first and second input terminals;
A first for applying an input signal to the first and second input terminals.
and a second input resistor, a capacitor for grounding the second input terminal, and negative feedback means for negatively feeding back the output of the differential amplification means to the first input terminal, A frequency characteristic correction circuit characterized in that a time constant formed by a resistor and a capacitor and a feedback coefficient of the negative feedback means are variable in conjunction with each other.
JP5197178A 1978-04-28 1978-04-28 Frequency characteristic correction circuit Expired JPS6038896B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5197178A JPS6038896B2 (en) 1978-04-28 1978-04-28 Frequency characteristic correction circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5197178A JPS6038896B2 (en) 1978-04-28 1978-04-28 Frequency characteristic correction circuit

Related Child Applications (3)

Application Number Title Priority Date Filing Date
JP59162373A Division JPS60143015A (en) 1984-07-31 1984-07-31 Frequency characteristic correction circuit
JP14837786A Division JPS63119312A (en) 1986-06-25 1986-06-25 Frequency characteristic correcting circuit
JP14837686A Division JPS6290016A (en) 1986-06-25 1986-06-25 Frequency characteristic correction circuit

Publications (2)

Publication Number Publication Date
JPS54144161A JPS54144161A (en) 1979-11-10
JPS6038896B2 true JPS6038896B2 (en) 1985-09-03

Family

ID=12901747

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5197178A Expired JPS6038896B2 (en) 1978-04-28 1978-04-28 Frequency characteristic correction circuit

Country Status (1)

Country Link
JP (1) JPS6038896B2 (en)

Also Published As

Publication number Publication date
JPS54144161A (en) 1979-11-10

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