JPS6410965B2 - - Google Patents

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Publication number
JPS6410965B2
JPS6410965B2 JP14837786A JP14837786A JPS6410965B2 JP S6410965 B2 JPS6410965 B2 JP S6410965B2 JP 14837786 A JP14837786 A JP 14837786A JP 14837786 A JP14837786 A JP 14837786A JP S6410965 B2 JPS6410965 B2 JP S6410965B2
Authority
JP
Japan
Prior art keywords
resistor
circuit
capacitor
phase
amplifier
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
JP14837786A
Other languages
Japanese (ja)
Other versions
JPS63119312A (en
Inventor
Tomofumi Nakatani
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 JP14837786A priority Critical patent/JPS63119312A/en
Publication of JPS63119312A publication Critical patent/JPS63119312A/en
Publication of JPS6410965B2 publication Critical patent/JPS6410965B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】[Detailed description of the invention]

(技術分野) 本発明は周波数特性補正回路(以下補正回路と
する。)に関する。 (従来技術) 従来の補正回路としては例えば第3図の様な高
域補正回路等が公知であつた。図において21は
入力端子、22,24は抵抗、23はボリユー
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域周波数では0゜
であるが、中域周波数ではボリユーム23の設定
位置に応じて位相が大幅に変化する。 従つて左右2チヤンネルを有するオーデイオア
ンプ等において、上述のような補正回路を各チヤ
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、
中域周波数では左右のチヤンネル間位相差が非常
に大きくなる。 (目的) 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、以下図面に従つて詳細に
説明する。 (実施例) 第1図は本発明の一実施例である。図において
入力端子11に印加された入力信号は2分岐して
一方は抵抗12を介して広帯域増幅器14の反転
入力端子16に印加され、他方は可変抵抗器18
を介して出力端子15に印加される。広帯域増幅
器14の非反転入力端子17は接地され、出力は
2分岐して一方はコンデンサ19を介して出力端
子15に印加され、他方は可変抵抗器13を介し
て前記反転入力端子16に負帰還される。可変抵
抗器13及び18は連動可変となされている。 この回路において抵抗12の抵抗値をR0とし、
可変抵抗器13及び18の設定抵抗値をそれぞれ
K・R0及びRとし、コンデンサ19の容量をC
とするとこの回路の伝達函数G(jω)は G(jω)=1−jωKCR/1+jωCR ……(1) 従つてこの位相特性arqG(jω)は arqG(jω)=−(tan-1KωCR+tan-1ωCR) ……(2) 今角速度ωがω0となる点で位相が90゜になるも
のとすると、可変抵抗器18及びコンデンサ19
の直列回路の時定数CRは(2)式より となる。今(3)式を(1)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(3)式に代入して となる。 よつて前記直列回路の時定数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(4)式に従つて変
化して第4図の様になることがわかる。なおKの
値は低域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)式に従つて変化し、第5図の様にな
り、角速度の低域においてはほぼ0゜、角速度ω0
おいては−90゜、高域においてはほぼ−180゜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
基準として、Kが3.16(+10dB)又は1/3.16(−
10dB)の場合と、Kが2(+6dB)又は1/2(−
6dB)の場合の特性の変化分を示したもので、こ
の場合最大±4.5゜程度の位相差しか生じないこと
がわかる。 従つて多チヤンネル増幅器において、各チヤン
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、各チヤンネル間の位相差は非常に少ない
ことがわかる。 第7図に本発明による低域補正回路の一実施例
を示す。 即ち本実施例は第1図の実施例における前記直
列回路のコンデンサ19と抵抗18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(jω)は G(jω)=−K−jωCR/1+jωCR ……(6) となり、位相特性argG(jω)は arg(jω)=tan-1ωCR/K+tan-1ωCR ……(7) となる。従つて今角速度ωがω0となる点におい
て位相が90゜になるものとすると、直列回路の時
定数CRは(7)より となり(8)式を(6)式に代入すると 又(8)式を(7)式に代入すると、 となる。従つて第3図の実施例における場合と同
様に、直列回路の時定数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図の様になり周波数の低域に
おいてはほぼ180゜、角速度ω0においては90゜高域
においてはほぼ0゜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ずるが、第1図の実
施例と同様にこの変化は非常に小さい。 第10図に本実施例においてKが1の場合を基
準としてKが3.16(+10dB)又は1/3.16(−
10dB)の場合と、Kが2(+6dB)又は1/2(−
6dB)の場合との位相特性の変動分を示す。 以上の実施例ではコンデンサ19の容量Cを固
定にし、可変抵抗器18の抵抗値を、第1図の実
施例の場合は√に反比例させ、第7図の実施例
の場合は√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
1図の場合は√に反比例、第7図の場合は√
に正比例する様に設定してもよい。 又例えば第3図の場合、抵抗13のKの値K1
K2、…KNに対応する抵抗値K1R0、K2R0、…KN
R0を切換スイツチにより切換る様にし、これと
連動した切換スイツチにより抵抗18の抵抗値R
(Technical Field) The present invention relates to a frequency characteristic correction circuit (hereinafter referred to as a correction circuit). (Prior Art) As a conventional correction circuit, for example, a high frequency correction circuit as shown in FIG. 3 has been known. In the figure, 21 is an input terminal, 22 and 24 are resistors, 23 is a volume, 26 and 27 are capacitors, and 25 is an output terminal. In this case, the phase characteristic at the output terminal 25 is 0° at low and high frequencies, as shown in FIG. 2, but the phase changes significantly at mid-range frequencies depending on the setting position of the volume 23. Therefore, in an audio amplifier or the like 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 Fig. 2, depending on the characteristic setting state of each correction circuit.
At mid-range frequencies, the phase difference between the left and right channels becomes very large. (Objective) An object of the present invention is to provide a correction circuit that does not have the above-mentioned drawbacks, and will be described in detail below with reference to the drawings. (Example) FIG. 1 shows an example of the present invention. In the figure, an input signal applied to an input terminal 11 is branched into two, one being applied to an inverting input terminal 16 of a broadband amplifier 14 via a resistor 12, and the other being applied to a variable resistor 18.
is applied to the output terminal 15 via. The non-inverting input terminal 17 of the wideband amplifier 14 is grounded, and the output is branched into two, one being applied to the output terminal 15 via the capacitor 19, and the other being negatively fed back to the inverting input terminal 16 via the variable resistor 13. be done. The variable resistors 13 and 18 are variable in conjunction with each other. In this circuit, the resistance value of resistor 12 is R 0 ,
The set resistance values of the variable resistors 13 and 18 are K・R 0 and R, respectively, and the capacitance of the capacitor 19 is C.
Then, the transfer function G(jω) of this circuit is G(jω)=1−jωKCR/1+jωCR ……(1) Therefore, this phase characteristic arqG(jω) is arqG(jω)=−(tan -1 KωCR+tan -1 ωCR) ...(2) Now assuming that the phase is 90° at the point where the angular velocity ω becomes ω 0 , the variable resistor 18 and capacitor 19
The time constant CR of the series circuit is given by equation (2). becomes. Now, by substituting equation (3) into equation (1) and finding the amplitude characteristic, And the phase characteristic in this case can be substituted into equation (3) as becomes. Therefore, if the time constant CR of the series 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 each value of K according to equation (4). It can be seen that the result is as shown in Figure 4. Note that since the value of K is equal to the degree of amplification for the low frequency range, it is converted into decibels and shown in the figure. In addition, the phase characteristics change according to equation (5) depending on the value of K, as shown in Figure 5, and are approximately 0° in the low range of angular velocity, -90° at angular velocity ω 0 , and -90° in the high range. is approximately -180°, 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. . FIG. 6 shows that K is 3.16 (+10 dB) or 1/3.16 (-
10 dB) and K is 2 (+6 dB) or 1/2 (-
6dB), and it can be seen that in this case, only a maximum phase difference of about ±4.5° occurs. Therefore, in a multi-channel amplifier, if a correction circuit such as the one described above is used for each channel, the phase difference between each channel will be very small even if the adjustment states of these correction circuits are set independently of each other. Recognize. FIG. 7 shows an embodiment of the low frequency correction circuit according to the present invention. That is, in this embodiment, the connection between the capacitor 19 and the resistor 18 in the series circuit in the embodiment shown in FIG. A more detailed explanation of the configuration will be omitted. The transfer function G(jω) of such a circuit is G(jω)=−K−jωCR/1+jωCR ...(6), and the phase characteristic argG(jω) is arg(jω)=tan -1 ωCR/K+tan -1 ωCR ……(7) becomes. Therefore, if we assume that the phase becomes 90° at the point where the angular velocity ω becomes ω 0 , the time constant CR of the series circuit is given by (7). Then, substituting equation (8) into equation (6), we get Also, substituting equation (8) into equation (7), we get becomes. Therefore, as in the embodiment of FIG. 3, the time constant CR of the series circuit can be adjusted according to the change in K.
If we change them in conjunction to maintain the relationship in equation (8), we get
The change in amplitude characteristics with respect to the value of K is as shown in FIG. The phase characteristics are as shown in Figure 9, approximately 180° in the low frequency range, 90° at angular velocity ω 0 , and approximately 0° in the high range, and this relationship does not change even if the value of K is changed. do not have. 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. 1, this change is very small. Figure 10 shows that in this example, K is 3.16 (+10 dB) or 1/3.16 (-
10 dB) and K is 2 (+6 dB) or 1/2 (-
6dB). In the above embodiments, the capacitance C of the capacitor 19 is fixed, and the resistance value of the variable resistor 18 is inversely proportional to √ in the embodiment of FIG. 1, and directly proportional to √ in the embodiment of FIG. The resistance value R is fixed, and the capacitance C is inversely proportional to √ in the case of Fig. 1, and √ in the case of Fig. 7.
It may be set so that it is directly proportional to . For example, in the case of FIG. 3, the value of K of the resistor 13 K 1 ,
Resistance values K 1 R 0 , K 2 R 0 ,…K N corresponding to K 2 ,…K N
R 0 is changed over by a changeover switch, and the changeover switch linked to this changes the resistance value R of the resistor 18.
of

【式】【formula】

【式】【formula】

【式】の如く切換る様にしても よい。 第7図の場合についても同様である。なお角速
度ω0は、上述において固定にした容量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12を可変抵抗器にするこ
とにより変えることも出来る。この場合は入力抵
抗12と例えば可変抵抗器18とを連動可変にす
ればよい。 (効果) 以上の様に本発明によれば、極めて簡単な構成
により、高域又は低域の周波数帯域のうち、一方
の周波数帯域については減衰又は増強特性となる
様に補正量を変化させ、もう一方の周波数帯域に
ついては補正量を変化させない様な補正特性を有
する周波数特性補正回路を得ることが出来る。
又、位相特性の変動も小さくすることが出来るの
で、ステレオ装置等で複数の周波数特性補正回路
を用いる場合等に適用すれば、これら各周波数特
性補正を、回路の調整状態が各々異なつていても
音像定位を良好に、行うことが出来る。
It is also possible to switch as shown in [Formula]. The same applies to the case of FIG. Note that the angular velocity ω 0 can be easily changed by changing the value of the capacitance C or the resistance R, which is fixed in the above. The value of K can also be changed by using a variable resistor as the input resistor 12. In this case, the input resistor 12 and, for example, the variable resistor 18 may be made variable in conjunction with each other. (Effects) As described above, according to the present invention, with an extremely simple configuration, the correction amount is changed so that one frequency band of the high frequency band or the low frequency band has attenuation or enhancement characteristics, As for the other frequency band, it is possible to obtain a frequency characteristic correction circuit having a correction characteristic that does not change the correction amount.
In addition, fluctuations in phase characteristics can also be reduced, so if applied when multiple frequency characteristic correction circuits are used in a stereo device, etc., each frequency characteristic correction can be performed by adjusting the adjustment state of each circuit differently. It is also possible to perform sound image localization well.

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

第3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1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。 13,18……可変抵抗器、14……広帯域増
幅器。
Fig. 3 shows a conventional frequency characteristic correction circuit, Fig. 2 shows its phase characteristic diagram, Fig. 1 shows a circuit diagram of an embodiment of the present invention, and Figs. 4, 5, and 6 show its characteristics. FIG. 7 is a circuit diagram showing another embodiment of the present invention, and FIGS. 8, 9, and 10 are diagrams showing its characteristics. 13, 18...variable resistor, 14...wideband amplifier.

Claims (1)

【特許請求の範囲】[Claims] 1 外部入力端子に加えられた入力信号を増幅す
る増幅度が可変になされた増幅器と、該増幅器の
出力を上記入力端子に負帰還する抵抗とコンデン
サとの直列回路と、上記抵抗とコンデンサとの直
列接続点に設けられた外部出力端子とを有し、上
記抵抗とコンデンサとによる時定数と上記増幅器
の増幅度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. An amplifier with variable amplification for amplifying an input signal applied to an external input terminal, a series circuit of a resistor and a capacitor that negatively feeds back the output of the amplifier to the input terminal, and a series circuit of the resistor and capacitor. 1. A frequency characteristic correction circuit, comprising an external output terminal provided at a series connection point, and wherein a time constant of the resistor and capacitor and an amplification degree of the amplifier are variable in conjunction with each other.
JP14837786A 1986-06-25 1986-06-25 Frequency characteristic correcting circuit Granted JPS63119312A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14837786A JPS63119312A (en) 1986-06-25 1986-06-25 Frequency characteristic correcting circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14837786A JPS63119312A (en) 1986-06-25 1986-06-25 Frequency characteristic correcting circuit

Related Parent Applications (1)

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

Publications (2)

Publication Number Publication Date
JPS63119312A JPS63119312A (en) 1988-05-24
JPS6410965B2 true JPS6410965B2 (en) 1989-02-22

Family

ID=15451398

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14837786A Granted JPS63119312A (en) 1986-06-25 1986-06-25 Frequency characteristic correcting circuit

Country Status (1)

Country Link
JP (1) JPS63119312A (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4078205A (en) * 1975-11-03 1978-03-07 Sundstrand Data Control, Inc. Electronic filter circuit

Also Published As

Publication number Publication date
JPS63119312A (en) 1988-05-24

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