JPH03257607A - Constant voltage current circuit - Google Patents

Constant voltage current circuit

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Publication number
JPH03257607A
JPH03257607A JP2058404A JP5840490A JPH03257607A JP H03257607 A JPH03257607 A JP H03257607A JP 2058404 A JP2058404 A JP 2058404A JP 5840490 A JP5840490 A JP 5840490A JP H03257607 A JPH03257607 A JP H03257607A
Authority
JP
Japan
Prior art keywords
transistor
base
emitter
current
constant
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.)
Pending
Application number
JP2058404A
Other languages
Japanese (ja)
Inventor
Seiichiro Kikuyama
菊山 誠一郎
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP2058404A priority Critical patent/JPH03257607A/en
Publication of JPH03257607A publication Critical patent/JPH03257607A/en
Pending legal-status Critical Current

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  • Amplifiers (AREA)
  • Control Of Electrical Variables (AREA)

Abstract

PURPOSE:To control both the constant-current and constant-voltage temperature characteristics a by canceling the constant current temperature characteristic of a base/emitter voltage in the first transistor by utilizing the base/emitter voltage of the 4th transistor equipped with the temperature characteristic in a reverse direction to the first transistor. CONSTITUTION:A current flows into a second transistor 4 with the value obtained by dividing the value, which is the constant voltage generated by a band gap type constant voltage circuit 30 subtracted by the base/emitter voltage of a first transistor 13, by the resistance value 24 of the first resistor. Therefore, the above mentioned current multiplied by the value obtained by adding '1' to the ratio between the emitter areas between second and third transistors 4 and 5 flows from the first potential of the circuit 30. On the other hand, a current also flows from the first potential with a value dividing the base/emitter voltage of the second transistor 4 with the value of a second resis tor 25. Thus, the both temperature characteristics of the constant voltage and the constant current can be controlled.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、定電圧定電流回路に関し、特にその定電流部
分の温度特性を補償するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a constant voltage constant current circuit, and particularly to compensating the temperature characteristics of the constant current portion thereof.

〔従来の技術〕[Conventional technology]

従来、上記の定電圧電流回路には、第2図に示すような
ものかある。これは、例えば半導体集積回路中に設けら
れるものてあって、電源端子(100)と出力端端(3
00)との間に、バンドギャップ型定電圧回路(30)
か設けられている。なお、(200)は2接地端子であ
る。この、バンドギャップ型定電圧回路(30)は、N
PNトランジスタ(1)、(2)、(3)とPNPトラ
ンジスタ(10)、(11)、(12)と、抵抗器(2
0)、(21)、(22)、(23)とから構成されて
いる。ここて、NPN)ランシスタ(1)、(2)のエ
ミツタ面積比をN、、抵抗器(20)、(21)の抵抗
比をR+、抵抗器(21)、(22)の抵抗比を82、
NPN)−ランジスタ(3)のベース・エミッタ間電圧
をVBEffとすると、電源端子(100)と出力端子
(300)との間には、(1)式で示すような定電圧V
IIEFか発生する。
Conventionally, the above-mentioned constant voltage current circuit includes one as shown in FIG. This is provided, for example, in a semiconductor integrated circuit, and includes a power terminal (100) and an output terminal (3).
00), a band gap type constant voltage circuit (30)
Or is provided. Note that (200) is a 2-ground terminal. This band gap type constant voltage circuit (30) has N
PN transistors (1), (2), (3), PNP transistors (10), (11), (12), and resistor (2)
0), (21), (22), and (23). Here, the emitter area ratio of NPN) run transistors (1) and (2) is N, the resistance ratio of resistors (20) and (21) is R+, and the resistance ratio of resistors (21) and (22) is 82. ,
NPN) - If the base-emitter voltage of the transistor (3) is VBEff, there is a constant voltage V between the power supply terminal (100) and the output terminal (300) as shown in equation (1).
IIEF occurs.

VRcr= VaE:+”R2”V7”In(N+”R
+)””(1)但し、vTは熱電圧kT/Qて、Kはボ
ルツマン定数、Tは絶対温度、qは電子の電荷である。
VRcr= VaE:+”R2”V7”In(N+”R
+)"" (1) However, vT is the thermal voltage kT/Q, K is Boltzmann's constant, T is the absolute temperature, and q is the charge of the electron.

また、この定電圧電流回路では、電源端子(100)か
ら流れ込む電流値を一定値にするために、(1)式で示
した定電圧VPIEFを利用して、抵抗値R24の抵抗
器(24)と、PNP )−ランジスタ(13)のベー
ス・エミッタ間電圧VIIE r 3とによって、PN
P )−ランシスタ(13)のコレクタ電流IC+3を
Ic+3=(VRl:r−Ve!++)/R2< ・”
(2)に定めている。このコレクタ電流1el 3か、
カレントミラー接続されているNPNI−ランジスタ(
4)、(5)のトランジスタ(4)に流れるのて、トラ
ンジスタ(4)、(5)のエミツタ面積比をN2とする
と、電源端子(100)から流れ込む電m s、、、は
、出力端子(30(1)のインピーダンスか高い場合に
は、1*tr= (N2+1)”(V*Er−VB2+
:+)/R2<”(3)となる。
In addition, in this constant voltage current circuit, in order to make the current value flowing from the power supply terminal (100) a constant value, the constant voltage VPIEF shown in equation (1) is used to connect the resistor (24) with a resistance value R24. and the base-emitter voltage VIIEr3 of the transistor (13), PNP
P) - Collector current IC+3 of Lancistor (13) is Ic+3=(VRl:r-Ve!++)/R2< ・”
(2). This collector current 1el 3,
NPNI transistor connected to current mirror (
When the emitter area ratio of transistors (4) and (5) is N2, the current flowing from the power supply terminal (100) m s is the output terminal. (If the impedance is 30(1) or higher, 1*tr= (N2+1)"(V*Er-VB2+
:+)/R2<”(3).

この定電圧電流回路における定電圧特性’VREFを考
えると、(1)式の右辺第1項は、トランジスタ(3)
のベース・エミッタ間電圧VllF:3の温度特性によ
って決まり、〜般に負の温度特性を持つ。同右辺第2項
は、抵抗比R1,R2とエミツタ面積比N、て温度係数
か定められるか、その温度係数は必ず正の値になる。従
って、抵抗比R1、R2とエミツタ面積比N、の値を可
変することによって、右辺第1項の負の温度特性を打ち
消すことかできる。
Considering the constant voltage characteristic 'VREF in this constant voltage current circuit, the first term on the right side of equation (1) is
It is determined by the temperature characteristics of the base-emitter voltage VllF:3, and generally has negative temperature characteristics. The second term on the right side determines the temperature coefficient by the resistance ratios R1 and R2 and the emitter area ratio N, and the temperature coefficient is always a positive value. Therefore, by varying the values of the resistance ratios R1 and R2 and the emitter area ratio N, the negative temperature characteristic in the first term on the right side can be canceled out.

定電流IREFの温度特性は、上記のようにして定電圧
VFIEFの温度特性をOにすると、PNP )−ラン
ジスタ(13)のベース・エミッタ間電圧vEll13
と抵抗R24の温度特性とて決る。
The temperature characteristics of the constant current IREF are as follows: When the temperature characteristics of the constant voltage VFIEF are set to O as described above, the voltage between the base and emitter of the transistor (13) is
is determined by the temperature characteristics of resistor R24.

(発明か解決しようとする課題) 従来の定電圧電流回路は、上記のように構成されている
のて、定電圧VREFの温度特性は、抵抗比RI、R2
を変えることによって小さくすることかできるか、定電
流IR□の温度特性は、集積回路の製造プロセスで決る
PNP)ランシスタ(13)のベース・エミッタ間電圧
VIIE I :Iと抵抗R24の温度特性に依存して
いるので、設計段階において定電流IREFの温度特性
を制御することかできないという問題点かあった。
(Problem to be solved by the invention) Since the conventional constant voltage current circuit is configured as described above, the temperature characteristics of the constant voltage VREF are determined by the resistance ratios RI and R2.
The temperature characteristics of the constant current IR□ are determined by the integrated circuit manufacturing process depending on the base-emitter voltage VIIE I:I of the PNP transistor (13) and the temperature characteristics of the resistor R24. Therefore, there was a problem in that the temperature characteristics of constant current IREF could only be controlled at the design stage.

本発明は、上記の問題点を解決した定電圧電流回路を提
供することを目的とする。
An object of the present invention is to provide a constant voltage current circuit that solves the above problems.

(課題を解決するための手段) 上記の目的を達成するために、本発明は、第1及び第2
の電位間に設けられたバンドギャップ定電圧回路と、第
1の電位に第1の抵抗器を介してエミッタか接続され、
ベースが第2の電位に接続されたPNPの第1トランジ
スタと、第3の電位にエミッタか、第1トランジスタの
コレクタにコレクタが、接続されたNPNの第2トラン
ジスタと、第3の電位にエミッタか、第2の電位にコレ
クタが接続され、ベースが第2トランジスタのベースに
接続されたNPNの第3トランジスタと、第2トランジ
スのベースとエミッタとの間に接続された第2の抵抗器
と、第2電位にコレクタか、第1トランジスタのベース
にエミッタか接続され、ベースか第1のトランジスタの
コレクタに接続されたNPNの第4トランジスタとを、
具備するものである。
(Means for Solving the Problems) In order to achieve the above object, the present invention provides first and second
a bandgap constant voltage circuit provided between the potentials of the emitter and the emitter connected to the first potential via the first resistor;
A first PNP transistor whose base is connected to a second potential, an emitter connected to a third potential, or a second NPN transistor whose collector is connected to the collector of the first transistor, and an emitter connected to a third potential. or a third NPN transistor whose collector is connected to the second potential and whose base is connected to the base of the second transistor; and a second resistor connected between the base and the emitter of the second transistor. , a fourth NPN transistor whose collector is connected to the second potential or whose emitter is connected to the base of the first transistor, and whose base is connected to the collector of the first transistor;
It is equipped with.

(作用) 本発明によれば、上述した従来のものと同様に、バンド
ギャップ型定電圧回路による定電圧から第1のトランジ
スタのベース・エミッタ間電圧を減算した値を第1の抵
抗器の抵抗値て除算した値の電流か、第2のトランジス
タに流れる。これによって、上記電流に第2のトランジ
スタと第3のトランジスタのエミツタ面積比に1を加算
した値を乗算した値の電流か、第1の電位から流れ込む
。一方、第2トランジスタのベース・エミッタ間電圧を
第2の抵抗器の値で除算した値の電流も第1の電位から
流れ込む。
(Function) According to the present invention, similarly to the conventional device described above, the value obtained by subtracting the base-emitter voltage of the first transistor from the constant voltage by the bandgap type constant voltage circuit is determined by the resistance of the first resistor. A current equal to the value divided by the current value flows through the second transistor. As a result, a current equal to the value obtained by multiplying the above current by a value obtained by adding 1 to the emitter area ratio of the second transistor and the third transistor flows from the first potential. On the other hand, a current having a value obtained by dividing the base-emitter voltage of the second transistor by the value of the second resistor also flows from the first potential.

〔実施例〕〔Example〕

この実施例は、第2図に示す従来の定電圧電流回路にお
いて、第1図に点線て囲んで示すように新たに抵抗器(
25)と、NPN )−ランジスタ(6)を追加したも
のである。
In this embodiment, in the conventional constant voltage current circuit shown in FIG. 2, a new resistor (
25) and an NPN)-transistor (6) is added.

即ち、第2図の回路ては、NPNトランジスタ(4)の
コレクタと工よツタとを直結していたのに対し、この実
施例ては、上記の接続を解き、NPNトランジスタ(4
)のコレクタにNPN)ランシスタ(6)のベースを接
続し、このNPN l−ランシスタ(6)のコレクタを
出力端子(300)に接続し、同トランジスタ(6)の
エミッタをNPN)−ランシスタ(4)のベースに接続
しである。さらに、抵抗器(25)を、トランジスタ(
4)のベース・エミッタ間に接続しである。
That is, in the circuit of FIG. 2, the collector of the NPN transistor (4) was directly connected to the base, whereas in this embodiment, the above connection was removed and the collector of the NPN transistor (4) was directly connected to the collector of the NPN transistor (4).
) is connected to the base of an NPN)-runsistor (6), the collector of this NPN l-runsistor (6) is connected to the output terminal (300), and the emitter of the same transistor (6) is connected to the NPN)-runsistor (4). ) is connected to the base. Furthermore, the resistor (25) is connected to the transistor (
4) is connected between the base and emitter.

この定電圧電流回路では、第2図に示した従来のものと
同様に、電源端子(100)と出力端子(300)との
間の定電圧V□、は(1)式て示した値となる。
In this constant voltage current circuit, as in the conventional circuit shown in Fig. 2, the constant voltage V□ between the power supply terminal (100) and the output terminal (300) is the value shown by equation (1). Become.

また、出力端子(100)から流れ込む電流I。Fは、
出力端子(300)のインピーダンスか高い場合、新た
にトランジスタ(6)と抵抗器(25)とを追加したこ
とにより、(3)式に示した値にVBE4/R2Sか追
加され、 IFIEF= (N2”l)”(VREF−VBEI3
)/R24”VBE4/R25・・・・・・・(4) となる。但し、VBE4はNPN)−ランシスタ(4)
のベース・エミッタ間電圧、R2Sは抵抗器(25)の
抵抗値である。トランジスタ(4)、 (5)かカレン
トミラー回路として機能するのは、トランジスタ(6)
のベース・エミッタ間のタイオートを介してトランジス
タ(4)のベース・エミッタ間を接続しているからであ
る。
Further, a current I flows from the output terminal (100). F is
If the impedance of the output terminal (300) is high, by adding a new transistor (6) and resistor (25), VBE4/R2S is added to the value shown in equation (3), and IFIEF = (N2 “l)” (VREF-VBEI3
)/R24"VBE4/R25...(4). However, VBE4 is NPN) - Runsistor (4)
The base-emitter voltage of R2S is the resistance value of the resistor (25). Transistors (4) and (5) or transistor (6) that functions as a current mirror circuit.
This is because the base and emitter of the transistor (4) are connected through the tie-out between the base and emitter of the transistor (4).

この定電圧電流回路における定電圧VREFの温度特性
は、第2図に示した従来のものと同様にOとすることが
できる。定電流IREFの温度特性は、定電圧の温度特
性か0であるとすると、(4)式の右辺第1項の温度特
性と同第2項の温度特性で決まり、第1項の温度特性は
、PNPトランジスタ(13)のベース・エミッタ間電
圧VBE I 3と抵抗器(24)との温度特性て決ま
る。一般にこれはPNPトランジスタ(13)のベース
・エミッタ間電圧VBE I 3と抵抗器(24)の抵
抗値R24か正の温度特性を有しているのて、正の温度
特性を持つ。一方、第2項の温度特性は、この第2項か
負の温度特性を持つNPN)−ランシスタ(4)のベー
ス・エミッタ間電圧VBE4と正の温度特性を持つ抵抗
器(24)の抵抗値R21の商であるので、負の温度特
性を有する。従って、抵抗器(25)の抵抗値R25を
可変することによって、第2項の温度特性を制御し、第
1項の温度特性を打ち消すことかてきる。
The temperature characteristic of the constant voltage VREF in this constant voltage current circuit can be set to O as in the conventional circuit shown in FIG. The temperature characteristics of constant current IREF are determined by the temperature characteristics of the first term and the second term on the right side of equation (4), assuming that the temperature characteristics of constant voltage are 0, and the temperature characteristics of the first term are , is determined by the base-emitter voltage VBE I3 of the PNP transistor (13) and the temperature characteristics of the resistor (24). Generally, this has a positive temperature characteristic because the base-emitter voltage VBE I3 of the PNP transistor (13) and the resistance value R24 of the resistor (24) have positive temperature characteristics. On the other hand, the temperature characteristics of the second term are the base-emitter voltage VBE4 of the NPN)-Lancistor (4), which has negative temperature characteristics, and the resistance value of the resistor (24), which has positive temperature characteristics. Since it is a quotient of R21, it has negative temperature characteristics. Therefore, by varying the resistance value R25 of the resistor (25), the temperature characteristics of the second term can be controlled and the temperature characteristics of the first term can be canceled.

〔発明の効果) 以上のように、本発明によれば、従来の定電圧電流回路
では第1のトランジスタ(実施例でいえばPNPトラン
ジスタ(13))のベース・エミッタ電圧の温度特性に
左右されていた定電流温度特性を、第1のトランジスタ
(13)とは逆方向の温度特性を有する第4のトランジ
スタ(実施例ていえばPNPトランジスタ(6))のベ
ース・エミッタ電圧を利用して、打ち消すように構成し
ている。しかも、従来のものと同様に定電圧温度特性は
0とできる。従って、安価に定電圧と定電流双方の温度
特性を制御することかてきる。
[Effects of the Invention] As described above, according to the present invention, in the conventional constant voltage current circuit, the temperature characteristics of the base-emitter voltage of the first transistor (in the embodiment, the PNP transistor (13)) By using the base-emitter voltage of the fourth transistor (for example, a PNP transistor (6)), which has a temperature characteristic in the opposite direction to that of the first transistor (13), It is configured as follows. Moreover, the constant voltage temperature characteristic can be set to 0 as in the conventional one. Therefore, it is possible to control the temperature characteristics of both constant voltage and constant current at low cost.

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

第1図は本発明による定電圧電流回路の1実施例の回路
図、第2図は従来の定電圧電流回路の回路図である。 (4)・・・・第2のトランジスタ、(5)・・・・第
3のトランジスタ、(6)・・・・・第4のトランジス
タ、(24)・・・・第1の抵抗器、(25)・・・・
第2の抵抗器、(30)・・・・バンドギャップ型定電
圧回路、(100)・・・・・電源端子(第1の電位)
 、 (200)・・・・・出力端子(第2の電位) 
、 (:1OO)・・・・・接地端子(第3の電位)。
FIG. 1 is a circuit diagram of one embodiment of a constant voltage and current circuit according to the present invention, and FIG. 2 is a circuit diagram of a conventional constant voltage and current circuit. (4)...second transistor, (5)...third transistor, (6)...fourth transistor, (24)...first resistor, (25)...
Second resistor, (30)...Band gap type constant voltage circuit, (100)...Power terminal (first potential)
, (200)...Output terminal (second potential)
, (:1OO)...Grounding terminal (third potential).

Claims (1)

【特許請求の範囲】[Claims] (1)第1及び第2の電位間に設けられたバンドギャッ
プ定電圧回路と、第1の電位に第1の抵抗器を介してエ
ミッタが接続されベースが第2の電位に接続されたPN
Pの第1トランジスタと、第3の電位にエミッタが第1
トランジスタのコレクタにコレクタが接続されたNPN
の第2トランジスタと、第3の電位にエミッタが第2の
電位にコレクタが接続されベースが第2トランジスタの
ベースに接続されたNPNの第3トランジスタと、第2
トランジスのベースと第3電位との間に接続された第2
の抵抗器と、第2電位にコレクタが第2トランジスタの
ベースにエミッタが接続されベースが第1のトランジス
タのコレクタに接続されたNPNの第4トランジスタと
を、具備する定電圧電流回路。
(1) A bandgap constant voltage circuit provided between first and second potentials, and a PN whose emitter is connected to the first potential via a first resistor and whose base is connected to the second potential.
a first transistor with an emitter at a third potential;
NPN whose collector is connected to the collector of the transistor
a third NPN transistor having an emitter connected to a third potential, a collector connected to the second potential, and a base connected to the base of the second transistor;
a second voltage connected between the base of the transistor and the third potential;
and a fourth NPN transistor, the collector of which is connected to a second potential, the emitter of which is connected to the base of the second transistor, and the base of which is connected to the collector of the first transistor.
JP2058404A 1990-03-08 1990-03-08 Constant voltage current circuit Pending JPH03257607A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2058404A JPH03257607A (en) 1990-03-08 1990-03-08 Constant voltage current circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2058404A JPH03257607A (en) 1990-03-08 1990-03-08 Constant voltage current circuit

Publications (1)

Publication Number Publication Date
JPH03257607A true JPH03257607A (en) 1991-11-18

Family

ID=13083425

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2058404A Pending JPH03257607A (en) 1990-03-08 1990-03-08 Constant voltage current circuit

Country Status (1)

Country Link
JP (1) JPH03257607A (en)

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