JPS6240883B2 - - Google Patents
Info
- Publication number
- JPS6240883B2 JPS6240883B2 JP14837686A JP14837686A JPS6240883B2 JP S6240883 B2 JPS6240883 B2 JP S6240883B2 JP 14837686 A JP14837686 A JP 14837686A JP 14837686 A JP14837686 A JP 14837686A JP S6240883 B2 JPS6240883 B2 JP S6240883B2
- Authority
- JP
- Japan
- Prior art keywords
- resistor
- circuit
- capacitor
- input
- phase
- 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
Links
- 239000003990 capacitor Substances 0.000 claims description 8
- 230000003321 amplification Effects 0.000 claims description 2
- 238000003199 nucleic acid amplification method Methods 0.000 claims description 2
- 238000010586 diagram Methods 0.000 description 4
- 230000004807 localization Effects 0.000 description 1
Landscapes
- Networks Using Active Elements (AREA)
Description
(産業上の利用分野)
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。
(発明が解決しようとする問題点)
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同位相差が非常
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図は本発明による高域補正回路の一実施例
である。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は連動になされている。
この様な回路において、今抵抗2の抵抗値をR0
とし、可変抵抗器3及び8の抵抗設定値をそれぞ
れKR0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ω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、前記分圧回路の時定数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)式を(2)式に代
入して
となる。
よつ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運動変化させる
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
値は高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に
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(jω)は
G(jω)=K−jωCR/1+jωCR…
(6)
となり、位相特性arqG(jω)は
arqG(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、分圧回路の時
定数CRは(7)式より
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1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3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9の容量Cを固定
にし、可変抵抗器8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
比例す様に設定してもよい。
又例えば第1図の場合、抵抗3の各Kの値
K1K2…Koに対応する抵抗値K1R0,K2R0…KoR0
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8の抵抗値Rを
(Industrial Application 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, 24 is a resistor, 23 is a volume,
26 and 27 are capacitors, and 25 is an output terminal. In this case, the phase characteristics at the output terminal 25 are:
As shown in FIG. 2, the phase is 0° at low and high frequencies, but the phase changes significantly at mid-range frequencies depending on the setting position of the volume 23. (Problem to be Solved by the Invention) 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 also change depending on the characteristic settings of each correction circuit. Because they are different as shown in Figure 2,
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. (Embodiment) FIG. 1 shows an embodiment of a high frequency correction circuit according to the present invention. In the figure, the input signal applied to the input terminal 1 is branched into two, one being applied to the inverting terminal 6 of the broadband amplifier 4 via the resistor 2, and the other being applied to the inverting terminal 6 of the wideband amplifier 4 via the variable resistor 8 and the capacitor 9. and is applied to the non-inverting terminal 7 of the broadband amplifier 4. amplifier 4
The output of is connected to the output terminal 5 and fed back to the inverting terminal 6 via the variable resistor 3. Further, the variable resistors 3 and 8 are interlocked.
In such a circuit, the resistance value of resistor 2 is now R 0
Assuming that the resistance setting values of variable resistors 3 and 8 are KR 0 and R, respectively, the capacitance of capacitor 9 is C, and the angular velocity of the input signal is ω, 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 the phase becomes 90° at the point where the angular velocity ω becomes ω 0 . Then, the time constant CR of the voltage divider circuit is given by equation (2). becomes. Now, by substituting equation (3) into equation (1) and finding the amplitude characteristic, Then, the phase characteristic in this case is obtained by substituting equation (3) into equation (2). becomes. 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 be changed according to equation (4) according to each value of K. It can be seen that it changes and becomes as shown in Figure 4. Note that since the value of K is equal to the degree of amplification for the high frequency range, it is converted into decibels and shown in the figure. In addition, the phase characteristics change according to equation (5) according to the value of K, as shown in Figure 5,
In the low range of angular velocity, it is approximately 0°, at angular velocity ω 0 , it is -90°, and in the high range, it 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 (-
10db) and K is 2 (+6db) 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 like 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 9 and the resistor 8 of the voltage dividing circuit in the embodiment shown in FIG. Further detailed explanations of the reference numerals and configurations will be omitted. The transfer function G(jω) of such a circuit is G(jω)=K−jωCR/1+jωCR…
(6), and the phase characteristic arqG(jω) becomes arqG(jω)=tan −1 ωCR/K+tan −1 ωCR (7). Therefore, if we assume that the phase is 90° at the point where the angular velocity ω becomes ω 0 , the time constant CR of the voltage divider circuit is given by equation (7). Then, substituting equation (8) into equation (6), we get Also, substituting equation (8) into equation (7), we get becomes. Therefore, as in the case of the embodiment shown in FIG.
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 and 90° at the angular velocity ω 0 .
In the high range, it is approximately 0°, and this relationship does not change even if the value of K is changed. Although a slight change in phase occurs depending on the value of K in areas other than the above-mentioned three points, this change is very small as in the embodiment shown in FIG. Figure 10 shows that in this example, K is 3.16 (+10db) or 1/3.16 (-
10db) and K is 2 (+6db) or 1/2 (-
6db). In the above embodiments, the capacitance C of the capacitor 9 is fixed, and the resistance value of the variable resistor 8 is inversely proportional to √ in the embodiment shown in FIG. 1, and directly proportional to √ in the embodiment shown in FIG. However, the resistance value R may be fixed and the capacitance C may be set to be inversely proportional to √ in the case of FIG. 1, and directly proportional to √ in the case of FIG. For example, in the case of Fig. 1, the value of each K of resistor 3
K 1 K 2 ...Resistance value corresponding to K o K 1 R 0 , K 2 R 0 ... K o R 0
is changed by a changeover switch, and the resistance value R of resistor 8 is changed by a changeover switch linked with this.
【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2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
2と例えば可変抵抗器8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ヤンネル間
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。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 2. In this case, the input resistor 2 and, for example, the variable resistor 8 may be made variable in conjunction with each other. (Effects) As described above, according to the present invention, even if the adjustment states of the respective frequency characteristic correction circuits are different, the phase difference between channels is small, so it is possible to eliminate uncertainty in sound image localization.
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。
3,8……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. 3, 8...variable resistor, 14...wideband amplifier.
Claims (1)
段と、上記第1の入力端子に入力信号を印加する
入力抵抗と、上記入力信号を分圧する抵抗及びコ
ンデンサの直列接続回路からなる分圧回路と、上
記抵抗及びコンデンサ同志の接続点を上記第2の
入力端子に接続する手段と、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、前記抵抗とコンデンサの直列接続回
路の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 A voltage divider consisting of a differential amplifying means having first and second input terminals, an input resistor for applying an input signal to the first input terminal, and a series-connected circuit of a resistor and a capacitor for dividing the voltage of the input signal. a circuit, means for connecting a connection point between the resistor and the capacitor to 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 the time constant of the series connection circuit of the resistor and the capacitor and the feedback coefficient of the negative feedback means are variable in conjunction with each other.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14837686A JPS6290016A (en) | 1986-06-25 | 1986-06-25 | Frequency characteristic correction circuit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14837686A JPS6290016A (en) | 1986-06-25 | 1986-06-25 | Frequency characteristic correction 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 |
|---|---|
| JPS6290016A JPS6290016A (en) | 1987-04-24 |
| JPS6240883B2 true JPS6240883B2 (en) | 1987-08-31 |
Family
ID=15451374
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14837686A Granted JPS6290016A (en) | 1986-06-25 | 1986-06-25 | Frequency characteristic correction circuit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6290016A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP3764483B2 (en) * | 1995-11-09 | 2006-04-05 | 新潟精密株式会社 | Tuning control method |
| KR100350399B1 (en) * | 1995-11-09 | 2002-12-18 | 타케시 이케다 | Tunning Control System |
-
1986
- 1986-06-25 JP JP14837686A patent/JPS6290016A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6290016A (en) | 1987-04-24 |
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