JPS6338575Y2 - - Google Patents
Info
- Publication number
- JPS6338575Y2 JPS6338575Y2 JP10758481U JP10758481U JPS6338575Y2 JP S6338575 Y2 JPS6338575 Y2 JP S6338575Y2 JP 10758481 U JP10758481 U JP 10758481U JP 10758481 U JP10758481 U JP 10758481U JP S6338575 Y2 JPS6338575 Y2 JP S6338575Y2
- Authority
- JP
- Japan
- Prior art keywords
- output
- amplifier
- distortion
- stage
- output stage
- 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
- 230000003321 amplification Effects 0.000 description 15
- 238000003199 nucleic acid amplification method Methods 0.000 description 15
- 230000001052 transient effect Effects 0.000 description 4
- 230000006866 deterioration Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000001934 delay Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
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- Amplifiers (AREA)
Description
【考案の詳細な説明】
本考案は、電力増幅回路の主に出力段の歪みの
改良に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention mainly relates to improvement of distortion in the output stage of a power amplifier circuit.
一般に、電力増幅器は電圧増幅段と大振巾電圧
励振段と、電力増幅段(出力段)で構成される
が、該電力増幅器の歪みの大半は電力増幅段(出
力段)から発生している。該電力増幅段は通常エ
ミツタホロワ(ソースホロワ)プツシユプル回路
が用いられ、エミツタホロワ(ソースホロワ)回
路自体100%負帰還回路であり、歪みは本来少な
いのであるが、一般の電圧増幅段に比べ負荷イン
ピーダンスが非常に低い為かなりの歪みを発生し
てしまう。そして電力増幅段自体100%負帰還回
路であるので、該電力増幅段単体では負帰還によ
る改善はこれ以上望めず、出力トランジスタを多
数並列接続したり、あるいは出力端から初段に多
量の負帰還をかけなければ歪みの改善を計ること
は出来ない。しかし、この様な初段への多量の負
帰還は周知の通り回路の過渡特性を悪化させ、過
渡的な歪みを発生したり、発振不安定性を生じた
りする欠点を有する。 Generally, a power amplifier consists of a voltage amplification stage, a large amplitude voltage excitation stage, and a power amplification stage (output stage), but most of the distortion in the power amplifier is generated from the power amplification stage (output stage). . The power amplification stage usually uses an emitter follower (source follower) push-pull circuit, and the emitter follower (source follower) circuit itself is a 100% negative feedback circuit, so distortion is inherently low, but the load impedance is very high compared to a general voltage amplification stage. Because it is low, considerable distortion occurs. Since the power amplification stage itself is a 100% negative feedback circuit, no further improvement can be expected from negative feedback in the power amplification stage alone, so it is necessary to connect a large number of output transistors in parallel, or to provide a large amount of negative feedback from the output end to the first stage. Unless it is applied, distortion cannot be improved. However, as is well known, such a large amount of negative feedback to the first stage deteriorates the transient characteristics of the circuit, causing transient distortion and oscillation instability.
本考案は、上述の様な欠点にかんがみ成された
もので増幅器の中で一番多くの歪を発生する、ド
ライバーを含む出力段の歪みを低減させ、低歪率
電力増幅器を提供するものである。 The present invention was created in consideration of the above-mentioned drawbacks, and aims to provide a low distortion power amplifier by reducing distortion in the output stage including the driver, which generates the most distortion among amplifiers. be.
第1図は本考案による一実施例である。入力端
子1は、ドライバーを含む第1の電力増幅回路、
即ち出力段2の入力端子及び差動増幅器として動
作するOPアンプ4の非反転入力端子に共通接続
すると共に、加算器11を介して第2の電力増幅
回路即ち出力段3の入力端子に接続する。前記出
力段2及び出力段3の出力端子はそれぞれ第1の
インピーダンス7及び第2のインピーダンス8を
介して出力端子10に共通接続すると共に、抵抗
5及び抵抗6を介して前記OPアンプ4の反転入
力端子に接続する。OPアンプ4の出力端子は加
算器11に接続し、出力端子10は負荷抵抗9を
介して接地する。 FIG. 1 shows an embodiment of the present invention. Input terminal 1 is a first power amplifier circuit including a driver,
That is, it is commonly connected to the input terminal of the output stage 2 and the non-inverting input terminal of the OP amplifier 4 which operates as a differential amplifier, and is also connected to the input terminal of the second power amplifier circuit, that is, the output stage 3 via the adder 11. . The output terminals of the output stage 2 and the output stage 3 are commonly connected to an output terminal 10 through a first impedance 7 and a second impedance 8, respectively, and are connected in common to an output terminal 10 through a resistor 5 and a resistor 6. Connect to input terminal. The output terminal of the OP amplifier 4 is connected to an adder 11, and the output terminal 10 is grounded via a load resistor 9.
以上の構成に於ける動作について説明する。入
力端子1に入力信号e1が印加され、第1の出力段
2のノンリニアな成分を含む増幅度をA2とする
と、該第1の出力段2の出力信号e2は、
e2=A2・e1 ……(1)
第2の出力段3のノンリニアな成分を含む増幅
度をA3、OPアンプ4の増幅度をA4としA4は充
分に大きな増幅度を有するものとしA4≒∞とみ
なせるものとすると、該OPアンプ4の出力信号
e4は第2の出力段3で増幅された後、抵抗6を介
して該OPアンプ4の反転入力端子に負帰還がな
されているから、周知の負帰還の作用により該
OPアンプ4の反転入力端子即ち抵抗5及び抵抗
6の共通接続点のレベルは入力信号e1のレベルに
等しくなる。従つて抵抗5及び抵抗6に流れる電
流i1は、抵抗5及び抵抗6の抵抗値をそれぞれR5
及びR6とすると
i1=e2−e1/R5=A2−1/R5e1 ……(2)
従つて、第2の出力段3の出力信号e3は、
e3=e1−i1・R6=(1−A2−1/R5・R6)e1
=(R5+R6/R5−R6/R5・A2)e1 ……(3)
ここで、第1のインピーダンス7及び第2のイ
ンピーダンス8のインピーダンスをそれぞれZ7及
びZ8とし、それぞれに流れる電流をi2及びi3とす
ると、負荷抵抗9に供給される出力信号e5は、
e5=(i2+i3)・R9 ……(4)
(但し、負荷抵抗9の抵抗値をR9とする)又i2
及びi3は
i2=e2−e5/Z7 ……(5)
i3=e3−e5/Z8 ……(6)
以上の式から出力信号e5は
e5=1/R9+1/Z7+1/Z8
(A2/Z7−R6/R5A2/Z8)e1+R5+R6/R5Z8e1……
(7)
従つて、式(7)の右辺のカツコ内の項をゼロとす
れば出力信号e5は、第1の出力段2のノンリニア
な成分を含んだ増幅度A2に関係なく、歪みの無
い出力を得ることが出来る。そこで、式(7)の右辺
のカツコ内の項をゼロにする為には、
R6/R5=Z8/Z7 ……(8)
この様に抵抗5及び6の抵抗値とインピーダン
ス7及び8のインピーダンス値を式(8)の条件を満
足する様に設定すれば出力信号は無歪みとなり、
この時のe5は
e5=R9/(Z7Z8)+R9・e1 ……(9)
この様に第2の出力属3のノンリニアな成分を
含む増幅度A3によつて発生する歪みは抵抗6を
介してOPアンプ4に負帰還されるから、上記増
幅度A3のノンリニア成分によつて増幅器3の出
力端子に生ずる歪みは無視出来る程度の非常に小
さな値に減少する。次に第1の出力段2のノンリ
ニアな成分を含む増幅度A2によつて生ずる歪み
は、上記の負帰還回路を介して増幅器3にも加え
られ、増幅器3の出力端子には増幅器2の出力端
子に現われる歪みと逆相の歪みが現われており、
この歪みが第2のインピーダンス8を介して出力
端子10に加えられ、増幅器2の歪みと相殺され
て式(9)で求まる歪みの無い出力信号を得ることが
出来る。又この場合OPアンプ4を介して負帰還
されるのは歪み成分だけであり、入力信号は第1
及び第2の出力段と第1及び第2のインピーダン
スを介して負荷に供給されるので従来の負帰還回
路における様な負帰還信号中の入力信号成分の遅
れ等による過渡的な歪みが発生することがない。 The operation in the above configuration will be explained. When the input signal e 1 is applied to the input terminal 1 and the amplification degree including the nonlinear component of the first output stage 2 is A 2 , the output signal e 2 of the first output stage 2 is as follows: e 2 =A 2・e 1 ...(1) Let A 3 be the amplification factor of the second output stage 3 including non-linear components, and A 4 be the amplification factor of the OP amplifier 4, and A 4 should have a sufficiently large amplification factor. Assuming that 4 ≒∞, the output signal of the OP amplifier 4
After e 4 is amplified by the second output stage 3, negative feedback is provided to the inverting input terminal of the OP amplifier 4 via the resistor 6, so that the signal e 4 is
The level of the inverting input terminal of the OP amplifier 4, that is, the common connection point of the resistors 5 and 6 becomes equal to the level of the input signal e1 . Therefore, the current i 1 flowing through the resistor 5 and the resistor 6 increases the resistance value of the resistor 5 and the resistor 6, respectively, by R 5
and R 6 , i 1 = e 2 - e 1 / R 5 = A 2 - 1 / R 5 e 1 ...(2) Therefore, the output signal e 3 of the second output stage 3 is e 3 = e 1 −i 1・R 6 = (1 − A 2 − 1 / R 5・R 6 ) e 1 = (R 5 + R 6 / R 5 − R 6 / R 5・A 2 ) e 1 ……(3 ) Here, if the impedances of the first impedance 7 and the second impedance 8 are Z 7 and Z 8 respectively, and the currents flowing through them are i 2 and i 3 , then the output signal e 5 supplied to the load resistor 9 is, e 5 = (i 2 + i 3 )・R 9 ...(4) (However, the resistance value of the load resistor 9 is R 9 ) and i 2
And i 3 is i 2 = e 2 − e 5 / Z 7 ...(5) i 3 = e 3 − e 5 / Z 8 ... (6) From the above formula, the output signal e 5 is e 5 = 1/ R 9 +1/Z 7 +1/Z 8 (A 2 /Z 7 −R 6 /R 5 A 2 /Z 8 )e 1 +R 5 +R 6 /R 5 Z 8 e 1 ...
(7) Therefore, if the term in the box on the right side of equation (7) is set to zero, the output signal e 5 will be distorted regardless of the amplification degree A 2 that includes the nonlinear component of the first output stage 2. It is possible to obtain output without Therefore, in order to make the term in the box on the right side of equation (7) zero, R 6 /R 5 =Z 8 /Z 7 ...(8) In this way, the resistance values of resistors 5 and 6 and the impedance 7 If the impedance values of and 8 are set to satisfy the condition of equation (8), the output signal will be distortion-free,
In this case, e 5 is e 5 = R 9 / (Z 7 Z 8 ) + R 9 · e 1 ...(9) In this way, by the amplification A 3 including the nonlinear component of the second output group 3, Since the generated distortion is negatively fed back to the OP amplifier 4 via the resistor 6, the distortion generated at the output terminal of the amplifier 3 due to the nonlinear component of the amplification degree A3 is reduced to an extremely small value that can be ignored. . Next, the distortion caused by the amplification A 2 including the non-linear component of the first output stage 2 is also applied to the amplifier 3 via the negative feedback circuit described above, and the output terminal of the amplifier 3 is sent to the output terminal of the amplifier 2. The distortion that appears at the output terminal and the opposite phase distortion appear,
This distortion is applied to the output terminal 10 via the second impedance 8, and is canceled out by the distortion of the amplifier 2, making it possible to obtain a distortion-free output signal determined by equation (9). Also, in this case, only the distortion component is negatively fed back via the OP amplifier 4, and the input signal is
Since it is supplied to the load via the second output stage and the first and second impedances, transient distortion occurs due to delays in the input signal components in the negative feedback signal, as in conventional negative feedback circuits. Never.
なお第1の出力段2と第2の出力段3のそれぞ
れの出力電力容量は任意に定めることが出来る。
即ち、前式(8)の条件さえ満足させれば、第2の出
力段3は、第1の出力段2とほぼ等しい出力電力
を負荷抵抗9に供給しながら、第1の出力段2の
歪みの除去が行えるし、同様にしてR5<R6、Z7
<Z8とすれば第2の出力段3は第1の出力段2に
比べて少ない電力を負荷抵抗9に供給しながら、
第1の出力段2の歪みの除去が行えるので、該第
2の出力段3に用いる出力トランジスタは電力損
失の少ない小形の出力トランジスタを用いても同
様の歪み除去効果を得ることが出来る。 Note that the output power capacities of each of the first output stage 2 and the second output stage 3 can be arbitrarily determined.
That is, as long as the condition of the above equation (8) is satisfied, the second output stage 3 supplies almost the same output power as the first output stage 2 to the load resistor 9, and the output power of the first output stage 2 is increased. Distortion can be removed, and in the same way R 5 < R 6 , Z 7
<Z 8 , the second output stage 3 supplies less power to the load resistor 9 than the first output stage 2, while
Since the distortion of the first output stage 2 can be removed, the same distortion removal effect can be obtained even if a small output transistor with low power loss is used as the output transistor used in the second output stage 3.
第2図は、第1図のOPアンプ4及び加算器1
1の部分を具体的に示した本考案による他の実施
例である。図に於いて、OPアンプ4は入力信号
に追従して浮動で動作する浮動の正電源11−1
と浮動の負電源11−2によつて駆動されるか
ら、OPアンプ4の差動入力信号と入力端子1に
印加された入力信号e1との加算が簡単な構成で行
えるものであり、第2図に於ける基本的な動作は
第1図に於ける動作に等しいのでその説明を省略
する。 Figure 2 shows the OP amplifier 4 and adder 1 in Figure 1.
This is another embodiment of the present invention specifically showing part 1 of the present invention. In the figure, the OP amplifier 4 is a floating positive power supply 11-1 that follows the input signal and operates in a floating manner.
Since it is driven by the floating negative power supply 11-2, the addition of the differential input signal of the OP amplifier 4 and the input signal e1 applied to the input terminal 1 can be performed with a simple configuration. The basic operation in FIG. 2 is the same as that in FIG. 1, so the explanation thereof will be omitted.
以上の様に本考案によれば、並列増幅器におい
て主として歪み成分を負帰還するので従来の負帰
還回路における様な過渡特性の悪化による性能の
劣化が少いという優れた効果を得ることが出来
る。 As described above, according to the present invention, since distortion components are mainly negatively fed back in the parallel amplifier, an excellent effect can be obtained in that there is less deterioration in performance due to deterioration of transient characteristics as in conventional negative feedback circuits.
第1図及び第2図はそれぞれ本考案の一実施例
を示す回路図である。
図中、2及び3は第1及び第2の出力段、4は
OPアンプ、5及び6は抵抗、7及び8は第1及
び第2のインピーダンス、11は加算器である。
1 and 2 are circuit diagrams each showing an embodiment of the present invention. In the figure, 2 and 3 are the first and second output stages, and 4 is the
OP amplifier, 5 and 6 are resistors, 7 and 8 are first and second impedances, and 11 is an adder.
Claims (1)
出力を第1及び第2のインピーダンスを介して加
算して成る並列増幅器において前記第1及び第2
の増幅器の出力端子間に第1及び第2の抵抗の直
列回路を接続し、上記第1及び第2の抵抗同志の
接続点の信号と入力信号との差信号を増幅して、
前記第2の増幅器の入力信号に加算することを特
徴とする増幅器。 In a parallel amplifier configured by adding the outputs of the first and second amplifiers to which input signals are applied via first and second impedances, the first and second
A series circuit of first and second resistors is connected between the output terminals of the amplifier, and a difference signal between the signal at the connection point of the first and second resistors and the input signal is amplified,
An amplifier characterized in that it is added to an input signal of the second amplifier.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10758481U JPS5813714U (en) | 1981-07-20 | 1981-07-20 | parallel amplifier |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10758481U JPS5813714U (en) | 1981-07-20 | 1981-07-20 | parallel amplifier |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5813714U JPS5813714U (en) | 1983-01-28 |
JPS6338575Y2 true JPS6338575Y2 (en) | 1988-10-12 |
Family
ID=29902014
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP10758481U Granted JPS5813714U (en) | 1981-07-20 | 1981-07-20 | parallel amplifier |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5813714U (en) |
-
1981
- 1981-07-20 JP JP10758481U patent/JPS5813714U/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPS5813714U (en) | 1983-01-28 |
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