JPS6271827A - Temperature detection circuit - Google Patents

Temperature detection circuit

Info

Publication number
JPS6271827A
JPS6271827A JP21294985A JP21294985A JPS6271827A JP S6271827 A JPS6271827 A JP S6271827A JP 21294985 A JP21294985 A JP 21294985A JP 21294985 A JP21294985 A JP 21294985A JP S6271827 A JPS6271827 A JP S6271827A
Authority
JP
Japan
Prior art keywords
temperature
resistance part
diode
potential side
electric current
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
JP21294985A
Other languages
Japanese (ja)
Inventor
Jiro Koide
二郎 小出
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.)
Seiko Epson Corp
Original Assignee
Seiko Epson 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 Seiko Epson Corp filed Critical Seiko Epson Corp
Priority to JP21294985A priority Critical patent/JPS6271827A/en
Publication of JPS6271827A publication Critical patent/JPS6271827A/en
Pending legal-status Critical Current

Links

Landscapes

  • Measuring Temperature Or Quantity Of Heat (AREA)

Abstract

PURPOSE:To detect simply temperature with a small-scale circuit by constituting a temperature detection part of a reverse bias state of a P-N junction diode and a high resistance part and using a MOS logic circuit for a decision circuit. CONSTITUTION:As to a reverse bias electrical current of the P-N junction diode 1, since a diffusion current component is dominant in a state over about 1V in the reverse direction in case of silicon, the electric current in the ordinary direction is increased exponentially as the temperature rises. When the high resistance part 2 connected in series with the diode 1 is changed only about several % with respect to the ultrahigh temperature, even if a constant is set so that the diode electric current is made <<the high resistance part electric current in a normal temperature area, the large and small relation is throughly reversed in a high-temperature area. Accordingly, when a temperature sensing resistance part 1 is connected with the high electric potential side like (a) in diagram, an output terminal 3 inclines to the high electric potential side in the temperature area to make the diode electric current > the high resistance part electric current and when the temperature sensing resistance part 1 is connected with the low electric potential side like (b) in diagram, an output signal inclined to the low electric potential side is obtained on the contrary. The output signal obtained there can be decided using a logic circuit.

Description

【発明の詳細な説明】 〔技南分舒〕 本発明は集積化成子回路分野に於ける!IJ[検出技術
に属する。
[Detailed Description of the Invention] [Ginan Bunshu] The present invention is in the field of integrated circuits! IJ [belongs to detection technology.

〔、概要〕〔,overview〕

この発明はMOSあるいはバイポーラ集噴回路に於いて
、PN接合ダイオード逆方向漏れt流の舗度特性が指数
的に変化する性質を利用し、池の高抵抗手段と直列接続
した場合、高儒域で高抵抗手段との素子イノビーダンス
が極度にτツバランスとなる事を利用し、高抵抗手段の
特性との兼ね会いによって簡易に、かつ不規4莫回硲で
偏度検出をaT能にするものである。
This invention utilizes the property that the pavement characteristics of a PN junction diode reverse leakage current changes exponentially in a MOS or bipolar integrated circuit, and when connected in series with a high resistance means of a pond, a high Utilizing the fact that the element innovation dance with the resistance means is extremely τ-balanced, and in combination with the characteristics of the high-resistance means, it is possible to easily and irregularly detect the deviation in 4 times. be.

〔従来の技術〕[Conventional technology]

PN接合の1匿特性を利用した偏度検出の方法は従来よ
りあった。しかしWK値そのものを計測するような用途
についての技術が多く、例えばバイポーラトランジスタ
のペース・エミッタ+&f3 ’=t 圧の温度係数、
PN接合ダイオード順方同降下1圧の濡髪係数、MOS
FETのゲート閾値は圧の温度係数がそれぞれ約−2〜
5 mV / ℃で変化する事を利用したものばかりで
あった。
There has been a conventional method for detecting polarity using the unilateral characteristic of a PN junction. However, there are many technologies for applications such as measuring the WK value itself, such as the temperature coefficient of the pace emitter of a bipolar transistor +&f3'=t pressure,
PN junction diode forward same drop 1 pressure wetting coefficient, MOS
The FET gate threshold has a pressure temperature coefficient of approximately -2 to
Most of them took advantage of the fact that it changes at 5 mV/°C.

従来より行なわれている上記構出方法は、温度測足用と
して確かに技術t?9に浸れたものである。
The above-mentioned construction method, which has been conventionally used, is certainly the best technology for temperature measurement. 9.

ところが梢Wl測定以外の用途への応用を考えてみると
、 (1)1見出用素子を顧ハイ了スで利用するので、@A
動毫流が大きくなる。
However, when considering applications other than treetop Wl measurement, (1) Since one indexing element is used at the rear end, @A
The motion becomes larger.

(2)  バイアス回路を工夫しな(八とうまく信号と
して利用できない。
(2) The bias circuit must be devised (it cannot be used effectively as a signal.

(コ)  得られ6検出部号処理システムが高11II
iになる。
(J) The obtained 6 detection part processing system is high 11II
Become i.

f4+  上記(3)と関連し7、回路規模が大きくな
る。
f4+ Related to (3) above, the circuit scale increases.

i51  システム構成回路の湛If将性も考慮する必
要があるため、簡易的L6用性に乏しい。
i51 Because it is necessary to consider the generality of the system configuration circuit, it is not suitable for simple L6 use.

等β欠截ばかりが目立ち、極めて柔軟性が少々い事がわ
かる。
Only the equiβ truncations are noticeable, and it can be seen that the flexibility is quite low.

〔発明がイ央しようとする問題点及び目的〕本発明は粂
膚化の観点に立ち、上記欠点の中がら特に回路規模、動
咋隠流、S用性について問題をメg決することを目的と
して・ρる。
[Problems and objectives to be addressed by the invention] The present invention aims to solve the above-mentioned drawbacks, particularly in terms of circuit scale, hidden flow, and S usability, from the viewpoint of scalability. As・ρru.

〔間I立点解決のための手段〕[Means for resolving the gap]

本発明では、湯度検出部ll+成をPNN接合ダイオニ
 −)’、7)逆バイアス状態と高抵抗部とで行ない、
検出部底流をa m11すると共に、判定回路はCM 
OS。
In the present invention, the hot water temperature detection section ll+ is formed in a PNN junction diode -)', 7) in a reverse bias state and a high resistance section,
The undercurrent of the detection part is a m11, and the judgment circuit is CM
O.S.

NMo53のVOS論理回IM’に用いている。It is used in the VOS logic circuit IM' of NMo53.

〔作用〕[Effect]

峡初に、本発明の霊度模出回路について、検出部を中心
として作用の説明をする。
First, we will explain the operation of the spirituality simulating circuit of the present invention, focusing on the detection section.

小1)司/、)及び1llilF図(b)は本発明によ
る温度検出部の基本戊成図である。図中1は感占抵抗部
、2は高抵抗部、5は出力1子である。
Figure (b) is a basic diagram of the temperature detection section according to the present invention. In the figure, 1 is a sensitive resistance section, 2 is a high resistance section, and 5 is one output child.

PN接合ダイオードの逆バイアス11mは、シリコンの
場合逆方向、杓IV以上の状態で、拡散電流成分が支配
的となるv);え 11euk : K −ni” −Aj= KAjex
p [Kg/FIT 〕・it+と表現できる。ここで
01:真性キャリアIIk度Aj :接合部面積 工g : Si禁削帝幅 R:ボルソマン定数 従って1品区上昇につれ、並方向7区流は指収関数的に
増加する事になる。
The reverse bias 11m of the PN junction diode is in the reverse direction in the case of silicon, and in a state of IV or higher, the diffusion current component becomes dominantv);
It can be expressed as p [Kg/FIT]・it+. Here, 01: Intrinsic carrier IIk degree Aj: Joint area g: Si forbidden width R: Bolsomann constant Therefore, as the 1-product area increases, the parallel direction 7-area flow increases like an index function.

一方、PN接合ダイオードと直列接続された旨抵抗部が
・%々侶度に対して数壬程咽の変化しかなければ、常温
域でダイオード電流(高抵抗部電流となるような足数投
足であっても、高温域で十分大小関係が反転する事がわ
かる。
On the other hand, if the resistance part connected in series with the PN junction diode changes only by a few inches with respect to temperature, the diode current (high resistance part current) at room temperature will change Even so, it can be seen that the magnitude relationship is sufficiently reversed in the high temperature range.

ゆえiC9−1tv (a3のようにダイオード感渦抵
抗部を高電位側に接続すれば、ダイオード電流〉高抵抗
部!、流なる烏度域で出力端子5は高電位側へ偏り、第
1図(b)のように接続すれば逆に低電位側へ輔った出
力1g号が得られる。
Therefore, iC9-1tv (If you connect the diode eddy-sensing resistance part to the high potential side as in A3, the output terminal 5 will be biased towards the high potential side in the irradiance region where the diode current > high resistance part!, as shown in Fig. 1). If the connection is made as shown in (b), on the other hand, an output of 1g, which is shifted to the low potential side, can be obtained.

そこで得られた出刃信号を判定するには、最もli!l
卓な方法として論理回路を用いればよい。
To judge the Deba signal obtained there, the most li! l
A simple method is to use a logic circuit.

〔実施例〕〔Example〕

第2図は本発明の具体的実施列である。 FIG. 2 is a specific implementation sequence of the present invention.

図中IUPN接合ダイオードによる感搗抵抗部、2は高
抵抗部になるPチャネルデプリ−7コン形MC8FKT
定′i11流譚、4は検出判定用クロソフトインバータ
、5はプルダウン抵抗、6は判足出力記1出R−8ラン
チ、7は出力端子、8は6のラッチ同格クリア端子、9
?taのクロソクトインハータサ°メプリング信号端子
である〇本冥捲例では高抵抗部にMO8定電流源を用い
ている。それ故抵抗部の湿度特性は、定電流値を1゜と
すれば 1゜ミーβP (VT? )1        ・・・
(2)ここで βP :PチャネルMo5FP!Tt流
係数VTP : pチャネルゲート蘭値電圧と表せるか
ら、ゲート閾+i! ’!圧の温度特性が1次の飄度債
存をもつゆえ、1゜は【高度に対し、2次の特性を示す
ことになる。
In the figure, the sensing resistance section is made of an IUPN junction diode, and 2 is a P channel depletion-7 contact type MC8FKT that becomes a high resistance section.
4 is a software inverter for detection and judgment, 5 is a pull-down resistor, 6 is a foot output record 1 output R-8 launch, 7 is an output terminal, 8 is a latch equivalent clear terminal of 6, 9
? In this example, which is the crossover signal terminal of TA, an MO8 constant current source is used in the high resistance part. Therefore, if the constant current value is 1°, the humidity characteristic of the resistance part is 1° Me βP (VT?)1...
(2) Here βP: P channel Mo5FP! Tt current coefficient VTP: Since it can be expressed as p channel gate value voltage, gate threshold + i! '! Since the temperature characteristic of pressure has a first-order altitude characteristic, 1° exhibits a second-order characteristic with respect to altitude.

一方、ダイオード特性は前記flJ式のように1度て関
し指数的変化を示すため、双方がつり合いを示す1度(
絶対藺度) TIは を満たす高度となる。
On the other hand, since the diode characteristics show an exponential change with respect to 1 degree as in the above flJ equation, the diode characteristics exhibit an exponential change with respect to 1 degree (
(absolute degree) TI is the altitude that satisfies.

ここで、V?P’:足[流M OS F K T (7
) fg 4 VTH。
Here, V? P': Foot [Flow M OS F K T (7
) fg 4 VTH.

To:室幅絶対1m、1f、α:ゲート蘭値電圧侶耽係
数。
To: Absolute chamber width 1m, 1f, α: Gate value voltage tolerance coefficient.

式中m2項はダイオード材料、MO8FI!jT定数、
ダイオード接置面積により一意的に定まる。
In the formula, the m2 term is the diode material, MO8FI! jT constant,
It is uniquely determined by the diode contact area.

−万里1項はMC’5FKTのゲート閾値峨圧により定
まる。
- Mari 1 term is determined by the gate threshold pressure of MC'5FKT.

次に論理U路判定系について考えれば、4のクロックド
ゲートが9の信号端子によって能動状態にある時、通常
のインバータとして動作するから論理bA値電圧: V
D1m丁はCMo5の場合で与えられる。
Next, considering the logic U path determination system, when the clocked gate 4 is activated by the signal terminal 9, it operates as a normal inverter, so the logic bA value voltage: V
D1m is given in the case of CMo5.

ここでβI弓βPはインバータを構成する8MO8゜P
lillO8FKTのtIla係ff l V’rP 
I V’rl+は上記MOSFETの各ゲート閾値電圧
である。
Here, βI bow βP is 8MO8゜P that constitutes the inverter.
lillO8FKT's tIla ff l V'rP
I V'rl+ is each gate threshold voltage of the MOSFET.

そこで素子の電流係数を等しく選ぶと vnct−(VDD−VT P+VT 11 )/ 2
      −・−f51となり、ゲートw4+IiI
!圧の偏度特性が寺し、いゆえVDITそのものはほと
んど![に依存しないと考えてよい。
Therefore, if the current coefficients of the elements are chosen equally, vnct-(VDD-VT P+VT 11 )/2
-・-f51, gate w4+IiI
! The pressure deviation characteristics are so bad that VDIT itself is almost impossible! It can be considered that it does not depend on [.

以上7)xうに素子定数を設定すれば、ゲート閾1?i
震圧VT−@ VTI’iE等しい時、論理ti+Lu
ijVnmT はt源電圧の中間点となる。
Above 7) If the element constant is set as x, the gate threshold will be 1? i
When seismic pressure VT-@VTI'iE is equal, logical ti+Lu
ijVnmT is the midpoint of the t source voltage.

従って(3)式で示されたつり合いmWTxより低い場
合、入力はH”と判断し、逆に高い温度の場合、入力は
“L”と判断する。
Therefore, if the temperature is lower than the balance mWTx shown in equation (3), the input is determined to be "H", and conversely, if the temperature is high, the input is determined to be "L".

今、4湛から徐々に温度が上昇し、TIなるY島1fを
超すと、4のインバータ出力は“H“となって6のR−
8ラツチ入力をトリガし、出力端子7へはH”が出力さ
れる。
Now, when the temperature gradually rises from 4 and exceeds 1f of the Y island TI, the inverter output of 4 becomes "H" and the R-
8 latch input is triggered, and H'' is output to output terminal 7.

逆にTxよシ低い場合には、R−8ランチ6の入力へは
”)1”が入らず、7の出力端子は−L”を保つ。
Conversely, when Tx is lower than Tx, ")1" does not enter the input of R-8 launch 6, and the output terminal of R-8 maintains -L.

温間Tx が一定時間続く場合、4のインバータは中間
レベル(H″でも“L”でもない状西)全出力するため
、6のFl−8ラッチ回路の4埋閾1直が4のインバー
4と暮しくならないように配慮する事が必要である。
When the warm Tx continues for a certain period of time, the inverter 4 outputs the full output at the intermediate level (not high or low), so the 4th threshold of the Fl-8 latch circuit 6 is the same as the inverter 4 It is necessary to take care not to live with

5のプルダウン抵抗は、4のグロソクトインパータが能
動でない時、6のラッチ入力が高イノビーダンスとなっ
て誤動作する事を防ぐだめのものである。
The pull-down resistor 5 is to prevent the latch input 6 from malfunctioning due to high innovation when the gross inverter 4 is not active.

〔発明の効果〕〔Effect of the invention〕

本発明によれ・ブ (11室1高時@作電流が極めて少なく、家々な4子回
路と共存しても全くデメリットを生じなし)。
Thanks to the present invention, (the operating current in the 11th room is extremely small at the time of high voltage, and there is no disadvantage at all even if it coexists with a 4-wire circuit).

、2+  現在用いられている・7リコン渠槓回路プロ
セスに於いてチップ上へ組み込みOT能である。
, 2+ It is possible to incorporate it onto a chip in the currently used .7 recon channel circuit process.

(3)  従って破産に向いている。(3) Therefore, it is suitable for bankruptcy.

(4)  回路規模が小さく、コスト的にも有利である
(4) The circuit scale is small and is advantageous in terms of cost.

(5)  一旦定数設定をす7tば、特に+4整は必要
な1/)。
(5) Once the constant is set, especially +4 integer is necessary 1/).

(6)  論理素子の徂み曾わせであって、デジタル信
号′fe吸うすべてのICへ徂み込める。
(6) The expansion of logic elements can be extended to all ICs that absorb digital signals 'fe'.

(7)  温度設定は、ダイオード接合部面積と尚抵抗
部の性′瓜で¥1ってしまうため、複誰な合わせ込みを
必要としない。
(7) Since the temperature setting depends on the area of the diode junction and the resistance of the resistor, no multiple adjustments are required.

等の利点が生まれる。Benefits such as:

〔応用〕〔application〕

本発明の応用3範囲は広い。中でも将に有効と忠われる
応用法としては、ICのチップ@度検出である。
The scope of application of the present invention is wide. Among them, an application method that is believed to be effective in the future is IC chip @ temperature detection.

:14項回路で集積度が高まると、必然的にチップの動
作を流は高まり、偏度条件は悪化する。高速、!JJ:
J作するICも高蛎になると特性劣化を生じて正常動作
が難しくなる。
: As the degree of integration increases in a 14-term circuit, the operating efficiency of the chip inevitably increases and the polarity conditions worsen. high speed,! JJ:
When the IC manufactured by J becomes high-quality, its characteristics deteriorate and normal operation becomes difficult.

本発明を例えばIC上へ組み込んでおけば、温度上昇に
よるIC+7)誤動作を検知し、V舌を出すとか、大I
I流が常時流れるドライバ段の異常発熱を検出して事前
に電流カットするようなセルフ・プロテクト回路として
の応用がuy罷となる。
For example, if the present invention is incorporated into an IC, it will be possible to detect malfunctions of the IC due to temperature rise, such as protruding V tongue or large I.
Application as a self-protect circuit that detects abnormal heat generation in a driver stage where I current always flows and cuts the current in advance is a failure.

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

第1図’(a)、 (b)は本発明の演出部構成図。第
2図は実施汐りの回路図である。 1・・・感温抵抗部FN接合ダイオード2・・・制抵抗
部 5・・・検出部出力端子 4〜6・・・論理的判定部 7・・・検出出力端子
Figures 1'(a) and 1(b) are configuration diagrams of the production section of the present invention. FIG. 2 is a circuit diagram of the implementation. 1... Temperature sensitive resistance section FN junction diode 2... Resistance control section 5... Detection section output terminals 4 to 6... Logical judgment section 7... Detection output terminal

Claims (1)

【特許請求の範囲】[Claims] 感温抵抗部、高抵抗部とを直列接続して成る検出部と論
理的判定手段を有し、前記検出部は前記感温抵抗部を高
電位側、前記高抵抗部を低電位側もしくは上記配置を入
れ替えた形で接続されるとともに、前記感温抵抗部と前
記高抵抗部との接続点を出力信号として前記論理的判定
手段入力端子へ接続し、一方前記感温抵抗部へはPN接
合ダイオード逆方向リーク特性を利用した事を特徴とす
る温度検出回路。
It has a detection section formed by connecting a temperature-sensitive resistance section and a high-resistance section in series, and a logical determination means, and the detection section sets the temperature-sensing resistance section to a high potential side and the high-resistance section to a low potential side or the above. The connection point between the temperature-sensitive resistance section and the high-resistance section is connected to the logical judgment means input terminal as an output signal, while a PN junction is connected to the temperature-sensitive resistance section. A temperature detection circuit characterized by utilizing diode reverse leakage characteristics.
JP21294985A 1985-09-26 1985-09-26 Temperature detection circuit Pending JPS6271827A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21294985A JPS6271827A (en) 1985-09-26 1985-09-26 Temperature detection circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21294985A JPS6271827A (en) 1985-09-26 1985-09-26 Temperature detection circuit

Publications (1)

Publication Number Publication Date
JPS6271827A true JPS6271827A (en) 1987-04-02

Family

ID=16630965

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21294985A Pending JPS6271827A (en) 1985-09-26 1985-09-26 Temperature detection circuit

Country Status (1)

Country Link
JP (1) JPS6271827A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03148861A (en) * 1989-07-19 1991-06-25 Fuji Electric Co Ltd Overheat detector of power ic and its structure
JP2009145170A (en) * 2007-12-13 2009-07-02 Fuji Electric Device Technology Co Ltd Temperature sensor circuit
CN103884441A (en) * 2012-12-20 2014-06-25 苏州工业园区新宏博通讯科技有限公司 Diode reverse leakage current temperature measuring circuit

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03148861A (en) * 1989-07-19 1991-06-25 Fuji Electric Co Ltd Overheat detector of power ic and its structure
JP2009145170A (en) * 2007-12-13 2009-07-02 Fuji Electric Device Technology Co Ltd Temperature sensor circuit
CN103884441A (en) * 2012-12-20 2014-06-25 苏州工业园区新宏博通讯科技有限公司 Diode reverse leakage current temperature measuring circuit

Similar Documents

Publication Publication Date Title
US20090174468A1 (en) Thermal Sensing Circuit Using Bandgap Voltage Reference Generators Without Trimming Circuitry
US3825778A (en) Temperature-sensitive control circuit
CN109406990A (en) A kind of built-in chip type excess temperature sluggishness protection detection circuit
JP2539899B2 (en) Input converter / driver circuit from TTL to ECL
GB1233722A (en)
US20030118079A1 (en) Threshold temperature sensor comprising room temperature test means
TW201041300A (en) Power supply voltage monitoring circuit and electronic circuit including the power supply voltage monitoring circuit
CN102338668A (en) Temperature detection circuit
JPH0399517A (en) Signal level converter
JPH07142969A (en) Integrated comparator, hysteresis comparator circuit and voltage difference change method
JPS6271827A (en) Temperature detection circuit
US6225851B1 (en) Temperature level detection circuit
GB2254175A (en) Compensation type heat sensor
JP3322553B2 (en) Temperature detection circuit and test method thereof
US5221888A (en) Current limited temperature responsive circuit
CA1102430A (en) Temperature-sensitive control circuits
JP2581492B2 (en) Input buffer circuit
JPS5972230A (en) Electronic circuit
US20230009763A1 (en) Reference current/ voltage generator and circuit system using the same
US4577119A (en) Trimless bandgap reference voltage generator
US4424457A (en) Voltage level detecting circuit
US3445777A (en) Thermal feedback for stabilization of differential amplifier unbalance
CN110955186A (en) Matrix type multiplexer output circuit based on single chip microcomputer control
JPH0575418A (en) Overcurrent detecting circuit
JPH01149520A (en) Semiconductor integrated circuit device