JPS6247367B2 - - Google Patents
Info
- Publication number
- JPS6247367B2 JPS6247367B2 JP54113799A JP11379979A JPS6247367B2 JP S6247367 B2 JPS6247367 B2 JP S6247367B2 JP 54113799 A JP54113799 A JP 54113799A JP 11379979 A JP11379979 A JP 11379979A JP S6247367 B2 JPS6247367 B2 JP S6247367B2
- Authority
- JP
- Japan
- Prior art keywords
- transistor
- collector
- output
- current
- vcc
- 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
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03F—AMPLIFIERS
- H03F1/00—Details of amplifiers with only discharge tubes, only semiconductor devices or only unspecified devices as amplifying elements
- H03F1/52—Circuit arrangements for protecting such amplifiers
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Amplifiers (AREA)
Description
【発明の詳細な説明】
本発明はトランジスタ回路に関し、回路の定常
動作状態で動作中、出力端子が電源の1端に接触
した場合の異常大電流によるトランジスタの破壊
を防止する保護回路を備えた増幅器に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a transistor circuit, and includes a protection circuit that prevents the transistor from being destroyed by an abnormally large current when an output terminal contacts one end of a power supply while the circuit is operating in a steady state. Regarding amplifiers.
第1図は従来の保護回路内蔵の増幅器を示し
た。第1図においてR1……R9は抵抗、RLは負荷
抵抗、C1……C3はコンデンサ、Q1……Q10はトラ
ンジスタ、D1……D3はダイオード、aは信号の
入力端子、bは信号の出力端子、e,gは電源の
正負端子、I0は電流がI0の定電流源、Vcc1は電圧
がVcc1の電源を示す。この従来例の保護回路
は、トランジスタQ10のコレクタに出力トランジ
スタQ7のコレクタ電流に比例する電流を流し、
トランジスタQ9で出力トランジスタQ7のコレク
タ電位とコレクタ電流の位相をトランジスタQ9
で検出し、正常動作時にはこれらの位相関係が同
じであるのでトランジスタQ9は遮断状態を保つ
が出力短絡等の異常動作時にはこの位相関係が著
しく異なり、トランジスタQ9,Q8を導通せしめ
て駆動トランジスタQ3を遮断状態とする保護回
路である。今、出力短絡していない正常動作時、
出力波形が入力波形と相似の時では、全オーデイ
オ周波数帯域、及び出力波形飽和時では、周波数
50Hzを超える周波数帯域で第4図にトランジスタ
Q9のエミツタ電位を実線で又ベース電位を一点
鎖線で示すように、トランジスタQ9のベース、
エミツタ間は常に同相で逆バイアスになつている
ため、トランジスタQ9は導通せずトランジスタ
Q8〜Q10の保護回路は誤動作しない。ところが出
力波形飽和時、周波数が50Hz以下では、コンデン
サC2,C3の充放電の時定数差により、トランジ
スタQ7のコレクタ電位とコレクタ電流の間に位
相差を生じ、第5図トランジスタQ9のエミツタ
電位を実線で又ベース電位を一点鎖線で示すよう
にA―B間で、トランジスタQ9のベース・エミ
ツタ間が一時的に順バイアスとなつてトランジス
タQ9が導通してトランジスタQ8〜Q10の保護回路
が動作するという欠点があつた。ここで、この種
の保護回路としては、
(1) 正常動作時いかなる電流値でも保護回路は動
作してはならない。 FIG. 1 shows a conventional amplifier with a built-in protection circuit. In Figure 1, R 1 ... R 9 are resistors, R L are load resistances, C 1 ... C 3 are capacitors, Q 1 ... Q 10 are transistors, D 1 ... D 3 are diodes, and a is a signal An input terminal, b is a signal output terminal, e and g are positive and negative terminals of a power supply, I 0 is a constant current source with a current of I 0 , and Vcc 1 is a power supply with a voltage of Vcc 1 . This conventional protection circuit allows a current proportional to the collector current of the output transistor Q7 to flow through the collector of the transistor Q10 ,
The phase of the collector potential and collector current of output transistor Q 7 is changed by transistor Q 9.
During normal operation, these phase relationships are the same, so transistor Q 9 remains cut off, but during abnormal operation such as an output short circuit, this phase relationship changes significantly and transistors Q 9 and Q 8 are turned on and driven. This is a protection circuit that turns off transistor Q3 . Now, during normal operation with no output short circuit,
When the output waveform is similar to the input waveform, the entire audio frequency band, and when the output waveform is saturated, the frequency
In the frequency band above 50Hz, the transistor shown in Figure 4
The base of transistor Q 9 ,
Since the emitters are always in phase and reverse biased, transistor Q9 is not conductive and the transistor
The protection circuits of Q8 to Q10 will not malfunction. However, when the output waveform is saturated and the frequency is below 50 Hz, a phase difference occurs between the collector potential and collector current of transistor Q 7 due to the difference in the charging and discharging time constants of capacitors C 2 and C 3 . As shown by the solid line showing the emitter potential and the dashed-dotted line showing the base potential, between A and B, the base and emitter of transistor Q 9 temporarily become forward biased, transistor Q 9 becomes conductive, and transistors Q 8 - The drawback was that the Q10 's protection circuit was activated. Here, for this type of protection circuit: (1) During normal operation, the protection circuit must not operate at any current value.
(2) 異常時はできるだけ少ない消費電力(又は電
流)に制限し、素子の破壊を防止しなければな
らない。(2) In the event of an abnormality, power consumption (or current) must be limited to the lowest possible level to prevent element destruction.
という要求特性があり、従来の保護回路では(1)の
条件を満足できない場合がある。Conventional protection circuits may not be able to satisfy condition (1).
本発明は、上述のごとく従来技術による保護回
路の定常動作時における誤動作を防止したトラン
ジスタ回路を提供するものである。 The present invention provides a transistor circuit which prevents the malfunction of the conventional protection circuit during normal operation as described above.
本発明を採用した一実施例を第2図に示し、第
2図に従つて本発明の原理を説明する。第2図に
おいて、R1……R9は抵抗、RLは負荷抵抗、C1…
…C3はコンデンサ、Q1……Q10はトランジスタ、
D1……D4はダイオード、aは信号の入力端子、
bは信号の出力端子、e,gは電源の正負端子、
I0は電流がI0の定電流源、Vcc1は電圧がVcc1の電
源を示す。出力短絡のない定常動作時、出力トラ
ンジスタQ7のコレクタ電流に比列して、トラン
ジスタQ10のコレクタにI0=(VBEQ7−VBEQ10)/
R9なる電流が流れる。(ここで、VBEQ7,VBEQ10
は、トランジスタQ7、Q10のベース―エミツタ間
電圧を表わしている。)今、抵抗R8での電圧降下
が、ダイオードD4のブレークダウン電圧VZD4よ
り小さいVZD4>I0R8の時、トランジスタQ9のベ
ース電位VBQ9はVBQ9=Vcc1−I0R8で表わされ抵
抗R8での電圧降下が、ダイオードD4のブレーク
ダウン電圧VZD4より大きいVZD4≦I0R8の時、ト
ランジスタQ9のベース電位VBQ9はVBQ9=Vcc1−
VZD4で表わされるため、トランジスタQ9のベー
ス電位の最高値はVZD4にて決まる。故に、第6
図,第7図にそれぞれトランジスタQ9のベース
電位VBQ9を一点鎖線で又エミツタ電位VBQ9を実
線で示すように、定常動作時、全周波数帯域中
で、出力波形が過飽和時でも、ダイオードD4の
ブレークダウン電圧VZD4をトランジスタQ9のベ
ース―エミツタ間電圧の位相が逆転しない値に、
つまりC点の電位(Vcc1−VZD4)に選び、かつ
出力短絡等の異常動作時、トランジスタQ9を充
分駆動できる値に、すなわち、(Vcc1−VBEQ11)
≫(Vcc1−VZD4)(ここでVBEQ11はトランジス
タQ11のベース―エミツタ間電圧を示している)
に選べば、保護回路は、定常動作時は誤動作せ
ず、出力短絡等の異常動作時は十分その機能を働
らかせることができる。上述のように、ダイオー
ドD4のブレークダウン電圧VZD4を適切な値に設
定すれば、定常動作状態中、実使用のあらゆる条
件下、誤動作しない保護回路を内蔵した増幅器を
実現できる。 An embodiment employing the present invention is shown in FIG. 2, and the principle of the present invention will be explained with reference to FIG. In Figure 2, R 1 ... R 9 is a resistance, R L is a load resistance, C 1 ...
... C3 is a capacitor, Q1 ... Q10 is a transistor,
D 1 ...D 4 is a diode, a is a signal input terminal,
b is the signal output terminal, e and g are the positive and negative terminals of the power supply,
I 0 indicates a constant current source with a current of I 0 , and Vcc 1 indicates a power source with a voltage of Vcc 1 . During steady operation with no output short circuit, I 0 = ( V BEQ7 − V BEQ10 ) /
A current R9 flows. (Here, V BEQ7 , V BEQ10
represents the base-emitter voltage of transistors Q 7 and Q 10 . ) Now, when the voltage drop across the resistor R 8 is smaller than the breakdown voltage V ZD4 of the diode D 4 (V ZD4 > I 0 R 8) , the base potential V BQ9 of the transistor Q 9 is V BQ9 = Vcc 1 − I 0 When V ZD4 ≦I 0 R 8 , where the voltage drop across resistor R 8 , represented by R 8 , is greater than the breakdown voltage V ZD4 of diode D 4 , the base potential V BQ9 of transistor Q 9 is V BQ9 = Vcc 1 −
Since it is expressed as V ZD4 , the highest value of the base potential of transistor Q9 is determined by V ZD4 . Therefore, the sixth
As shown in Figures 1 and 7, the base potential VBQ9 of transistor Q9 is shown by a dashed line and the emitter potential VBQ9 is shown by a solid line. Set the breakdown voltage V ZD4 of transistor Q 9 to a value that does not reverse the phase of the base-emitter voltage of transistor Q 9 .
In other words, select the potential at point C (Vcc 1 - V ZD4 ), and select a value that can sufficiently drive transistor Q 9 during abnormal operation such as an output short circuit, that is, (Vcc 1 - V BEQ11 ).
≫(Vcc 1 - V ZD4 ) (Here, V BEQ11 indicates the voltage between the base and emitter of transistor Q11 )
If selected, the protection circuit will not malfunction during normal operation, and will be able to fully perform its function during abnormal operation such as an output short circuit. As described above, by setting the breakdown voltage V ZD4 of the diode D4 to an appropriate value, it is possible to realize an amplifier with a built-in protection circuit that does not malfunction under all conditions of actual use during steady operation.
次に他の実施例を第3図に示した。第3図にお
いて、R1……R10は抵抗、RLは負荷抵抗、C1…
…C3はコンデンサ、Q1……Q10はトランジスタ、
D1……D5はダイオード、aは信号の入力端子、
bは信号の出力端子、e,gは電源の正負端子、
I0は電流がI0なる定電流源、Vcc1は電圧がVcc1の
電源を示す。出力段は一般に知られているB級シ
ングルエンデツドプツシユブル構成である。今、
この回路での定常動作時、出力トランジスタQ7
のコレクタ電流に比列して、トランジスタQ10の
コレクタにI0=(VBEQ7−VBEQ10)/R9なる電流
が流れる。(ここでVBEQ7,VBEQ10はトランジス
タQ7,Q10のベース―エミツタ間電圧を表わして
いる。)今、抵抗R8での電圧降下がダイオードD4
のブレークダウン電圧VZD4より小さいVZD4>
I0R8の時、トランジスタQ9のベース電位VBQ9は
VBQ=Vcc1−I0R8で表わされ、抵抗R8での電圧
降下がダイオードD4のブレークダウン電圧VZD4
より大きいVZD4≦I0R8の時、トランジスタQ9の
ベース電位VBQ9はVBQ9=Vcc1−VZD4で表わさ
れるため、トランジスタQ9のベース電位の最高
値はブレークダウン電圧VZD4にて決まる。故に
第6図,第7図に示すように、定常動作時、全周
波数帯域中で、出力波形が過飽和時でも、ダイオ
ードD4のブレークダウン電圧VZD4をトランジス
タQ9のベース―エミツタ間電圧の位相が逆転し
ない値に、つまり、C点の電位(Vcc1−VZD4)
に選び、かつ異常動作時、トランジスタQ9を充
分駆動できる値に、すなわち(Vcc1−VBED5)≫
(Vcc1−VZD4)(ここでVBED5はダイオードD5の
順方向導通電圧を示している。)に選べば、保護
回路は、定常動作時は誤動作せず、異常動作時
は、十分その機能を働らかせることができる。 Next, another embodiment is shown in FIG. In Fig. 3, R 1 ...R 10 is a resistance, R L is a load resistance, C 1 ...
... C3 is a capacitor, Q1 ... Q10 is a transistor,
D1 ... D5 is a diode, a is a signal input terminal,
b is the signal output terminal, e and g are the positive and negative terminals of the power supply,
I 0 indicates a constant current source whose current is I 0 , and Vcc 1 indicates a power supply whose voltage is Vcc 1 . The output stage has a generally known class B single end pushable configuration. now,
During steady operation in this circuit, the output transistor Q 7
A current of I 0 =(V BEQ7 −V BEQ10 )/R 9 flows through the collector of the transistor Q 10 in proportion to the collector current of . (Here, V BEQ7 and V BEQ10 represent the base-emitter voltages of transistors Q 7 and Q 10. ) Now, the voltage drop across resistor R 8 is the voltage drop across diode D 4.
The breakdown voltage of V ZD4 is smaller than V ZD4 >
When I 0 R 8 , the base potential V BQ9 of the transistor Q 9 is expressed as V BQ = Vcc 1 - I 0 R 8 , and the voltage drop across the resistor R 8 is the breakdown voltage of the diode D 4 V ZD4
When V ZD4 ≦I 0 R 8 , the base potential V BQ9 of transistor Q 9 is expressed as V BQ9 = Vcc 1 − V ZD4 , so the highest value of the base potential of transistor Q 9 is equal to the breakdown voltage V ZD4 . It is decided. Therefore, as shown in Figures 6 and 7, during steady operation, even when the output waveform is oversaturated in all frequency bands, the breakdown voltage V ZD4 of diode D4 is equal to the base-emitter voltage of transistor Q9 . The potential at point C (Vcc 1 −V ZD4 ) is set to a value that does not reverse the phase.
and a value that can sufficiently drive transistor Q 9 during abnormal operation, that is, (Vcc 1 −V BED5 )≫
(Vcc 1 - V ZD4 ) (where V BED5 indicates the forward conduction voltage of diode D 5 ), the protection circuit will not malfunction during normal operation and will be sufficiently protected during abnormal operation. function can be activated.
上述のように、ダイオードD4のブレークダウ
ン電圧VZD4を適当な値に設定すれば定常動作状
態中、実使用のあらゆる条件下、誤動作しない保
護回路を内蔵した増幅器を実現できる。 As described above, by setting the breakdown voltage V ZD4 of the diode D4 to an appropriate value, it is possible to realize an amplifier with a built-in protection circuit that will not malfunction under all conditions of actual use during steady operation.
第1図は従来例を示す回路図、第2図,第3図
はそれぞれ本発明の実施例を示す回路図、第4
図,第5図はそれぞれ従来例の回路の動作を説明
した電圧波形図、第6図,第7図は本発明の実施
例による回路の動作を説明した電圧波形図を示
す。
R1…R10……抵抗、RL……負荷抵抗、C1…C3
……コンデンサ、Q1…Q10……トランジスタ、D1
…D5……ダイオード、I0……定電流源、Vcc1……
バイアス電源、a,b,e,g……端子。
FIG. 1 is a circuit diagram showing a conventional example, FIGS. 2 and 3 are circuit diagrams showing an embodiment of the present invention, and FIG.
5 and 5 are voltage waveform diagrams illustrating the operation of a conventional circuit, respectively, and FIGS. 6 and 7 are voltage waveform diagrams illustrating the operation of a circuit according to an embodiment of the present invention. R 1 ...R 10 ...Resistance, R L ...Load resistance, C 1 ...C 3
...Capacitor, Q 1 ...Q 10 ...Transistor, D 1
...D 5 ...diode, I 0 ...constant current source, Vcc 1 ...
Bias power supply, a, b, e, g...terminals.
Claims (1)
力電流が設定値以上の電流になつたときに前記出
力トランジスタのベース電流を制限する保護回路
を備えたトランジスタ回路において、前記保護回
路は前記出力トランジスタのコレクタ電流に応じ
たコレクタ電流を発生するトランジスタと、この
トランジスタのコレクタと電源の一端との間に並
列接続された抵抗と定電圧素子と、前記出力端子
と前記トランジスタのコレクタとの電位差に応答
して前記出力トランジスタのベース電流を制限す
る手段とを備え、前記定電圧素子は前記トランジ
スタのコレクタ電流が所定値以上となつたときに
導通して前記トランジスタのコレクタの電位を規
定値にクランプすることを特徴とするトランジス
タ回路。1. In a transistor circuit including a protection circuit that limits the base current of the output transistor when the output current of the output transistor connected to the output terminal exceeds a set value, the protection circuit is connected to the collector of the output transistor. A transistor that generates a collector current according to the current, a resistor and a constant voltage element connected in parallel between the collector of this transistor and one end of a power supply, and a transistor that responds to the potential difference between the output terminal and the collector of the transistor. and means for limiting a base current of the output transistor, and the constant voltage element is configured to conduct when the collector current of the transistor exceeds a predetermined value and clamp the potential of the collector of the transistor to a predetermined value. Characteristic transistor circuit.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11379979A JPS5637713A (en) | 1979-09-05 | 1979-09-05 | Electric power amplifying circuit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11379979A JPS5637713A (en) | 1979-09-05 | 1979-09-05 | Electric power amplifying circuit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5637713A JPS5637713A (en) | 1981-04-11 |
| JPS6247367B2 true JPS6247367B2 (en) | 1987-10-07 |
Family
ID=14621363
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP11379979A Granted JPS5637713A (en) | 1979-09-05 | 1979-09-05 | Electric power amplifying circuit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5637713A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6326916U (en) * | 1986-08-04 | 1988-02-22 | ||
| JPH0310861U (en) * | 1989-06-17 | 1991-02-01 |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5992606A (en) * | 1982-11-19 | 1984-05-28 | Nec Ic Microcomput Syst Ltd | Protecting circuit of transistor amplifier |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6038047B2 (en) * | 1977-12-09 | 1985-08-29 | 日本電気株式会社 | transistor circuit |
-
1979
- 1979-09-05 JP JP11379979A patent/JPS5637713A/en active Granted
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6326916U (en) * | 1986-08-04 | 1988-02-22 | ||
| JPH0310861U (en) * | 1989-06-17 | 1991-02-01 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5637713A (en) | 1981-04-11 |
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