JPH0442612B2 - - Google Patents
Info
- Publication number
- JPH0442612B2 JPH0442612B2 JP57062314A JP6231482A JPH0442612B2 JP H0442612 B2 JPH0442612 B2 JP H0442612B2 JP 57062314 A JP57062314 A JP 57062314A JP 6231482 A JP6231482 A JP 6231482A JP H0442612 B2 JPH0442612 B2 JP H0442612B2
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- pressure sensor
- constant current
- voltage
- circuit
- 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 - Lifetime
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L1/00—Measuring force or stress, in general
- G01L1/20—Measuring force or stress, in general by measuring variations in ohmic resistance of solid materials or of electrically-conductive fluids; by making use of electrokinetic cells, i.e. liquid-containing cells wherein an electrical potential is produced or varied upon the application of stress
- G01L1/22—Measuring force or stress, in general by measuring variations in ohmic resistance of solid materials or of electrically-conductive fluids; by making use of electrokinetic cells, i.e. liquid-containing cells wherein an electrical potential is produced or varied upon the application of stress using resistance strain gauges
- G01L1/2268—Arrangements for correcting or for compensating unwanted effects
- G01L1/2281—Arrangements for correcting or for compensating unwanted effects for temperature variations
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Fluid Pressure (AREA)
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
Description
【発明の詳細な説明】
本発明は、集積型圧力センサに係り、特に、セ
ンサ部分と圧力検出信号の増幅回路部分との半導
体集積化に好適な温度補償回路に関するものであ
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an integrated pressure sensor, and more particularly to a temperature compensation circuit suitable for semiconductor integration of a sensor portion and a pressure detection signal amplification circuit portion.
半導体圧力センサの感度の温度による変動を補
償する回路には、例えばUSP3836796号に記載さ
れたものがある。その原理的構成を第1図に示
す。この補償回路は、トランジスタ1とそのコレ
クタ・ベース間に接続された抵抗R1とベース・
エミツタ間に接続された抵抗R2とからなり、ブ
リツジ構成されたストレンゲージG1〜G4の回路
と直列接続されている。この温度補償回路は、一
般にnVbe回路として知られている回路である。 A circuit for compensating for temperature-related variations in the sensitivity of a semiconductor pressure sensor is described, for example, in US Pat. No. 3,836,796. The basic configuration is shown in Figure 1. This compensation circuit consists of transistor 1, a resistor R1 connected between its collector and base, and a resistor R1 connected between its collector and base.
It consists of a resistor R 2 connected between the emitters, and is connected in series with a bridge-configured strain gauge circuit G 1 to G 4 . This temperature compensation circuit is generally known as an nVbe circuit.
補償回路の端子間電圧Vcomは、トランジスタ
1のベース・エミツタ間電圧Vbeを抵抗R1と抵
抗R2とにより決まる定数倍した電圧となる。そ
こで、抵抗R1と抵抗R2とを適当に選び、電圧
Vcomの温度特性で、圧力センサの感度を補償し
ている。 The inter-terminal voltage Vcom of the compensation circuit is a voltage obtained by multiplying the base-emitter voltage Vbe of the transistor 1 by a constant determined by the resistors R1 and R2 . Therefore, select resistor R 1 and resistor R 2 appropriately, and set the voltage
The temperature characteristics of Vcom compensate for the sensitivity of the pressure sensor.
圧力センサの感度は、一般に、高温になると低
くなる。この感度の低下を補償するには、圧力セ
ンサのブリツジ端子電圧を高くすればよい。すな
わち、補償回路の端子間電圧Vcomを低くすれば
よい。トランジスタ1のベース・エミツタ間電圧
Vbeは温度上昇にともなつて低くなるので、補償
回路の端子間電圧Vcomが低くなり、圧力センサ
のブリツジ端子電圧を高くすることができる。 The sensitivity of pressure sensors generally decreases at higher temperatures. To compensate for this decrease in sensitivity, the bridge terminal voltage of the pressure sensor can be increased. That is, it is sufficient to lower the voltage Vcom between the terminals of the compensation circuit. Base-emitter voltage of transistor 1
Since Vbe decreases as the temperature rises, the inter-terminal voltage Vcom of the compensation circuit decreases, making it possible to increase the bridge terminal voltage of the pressure sensor.
この種の温度補償回路には、特開昭49−119675
号公報に記載のものもある。この補償回路は、固
定抵抗と可変抵抗および感熱素子として用いたト
ランジスタにより、温度に応じた電流を圧力セン
サのブリツジ回路に供給する手段、または、さら
にツエナーダイオード等を追加して、温度に応じ
た電圧を圧力センサのブリツジ回路に供給する手
段を提案している。 This type of temperature compensation circuit has Japanese Patent Application Laid-open No. 49-119675.
Some of them are described in the publication. This compensation circuit uses a fixed resistor, a variable resistor, and a transistor used as a heat-sensitive element to supply a current according to the temperature to the bridge circuit of the pressure sensor, or a Zener diode or the like is added to supply a current according to the temperature. A means for supplying voltage to a bridge circuit of a pressure sensor is proposed.
上記USP3836796の圧力センサでは、電源電圧
Vccが変化したとき、トランジスタを含む補償回
路の端子電圧Vcomがほとんど影響を受けないの
に対して、ブリツジ端子電圧は、1対1に影響を
受ける。したがつて、温度変化に伴うVcomの変
化量は、電源電圧Vccの変化の影響をほとんど受
けずに一定であるため、電源電圧Vccが上昇する
と、端子電圧Vcomの全体に占める割合が小さく
なり、温度補償が不足し、電源電圧が低下したと
きは、過補償となる欠点があつた。 For the above USP3836796 pressure sensor, the power supply voltage
When Vcc changes, the terminal voltage Vcom of the compensation circuit including transistors is hardly affected, whereas the bridge terminal voltage is affected one-to-one. Therefore, the amount of change in Vcom due to temperature changes is almost unaffected by changes in power supply voltage Vcc and remains constant; therefore, as power supply voltage Vcc increases, the proportion of terminal voltage Vcom in the total decreases. When temperature compensation is insufficient and the power supply voltage drops, there is a drawback of overcompensation.
一方、特開昭49−119675号公報の圧力センサで
は、ブリツジ回路部分のみに対して温度に応じた
電流または電圧を供給しているが、小型化特に集
積化に対する配慮が無く、また、ブリツジの圧力
検知信号を増幅し次段に出力する増幅回路の温度
特性も含めた補償については、なんら配慮が無か
つた。 On the other hand, in the pressure sensor disclosed in JP-A-49-119675, current or voltage depending on the temperature is supplied only to the bridge circuit, but there is no consideration given to miniaturization, especially integration, and the bridge circuit is No consideration was given to compensation including the temperature characteristics of the amplifier circuit that amplifies the pressure detection signal and outputs it to the next stage.
ところで、最近は、圧力センサを小型化しまた
は信号の取り扱いを容易にする目的で、圧力セン
サ部分とその圧力検出信号の増幅回路部分とを集
積化する方式が提案されている。その際、圧力セ
ンサのブリツジを構成する拡散ゲージ抵抗は、例
えばシリコンダイアフラム面上に拡散されて形成
される。また、増幅回路部分の増幅度を決定する
抵抗も、前記シリコン基板のダイヤフラム領域外
の面上に形成されている。 Incidentally, recently, for the purpose of downsizing the pressure sensor or making it easier to handle the signal, a method has been proposed in which the pressure sensor part and the amplification circuit part of the pressure detection signal are integrated. In this case, the diffusion gauge resistor constituting the bridge of the pressure sensor is formed, for example, by diffusion on the surface of the silicon diaphragm. Further, a resistor that determines the amplification degree of the amplifier circuit portion is also formed on the surface of the silicon substrate outside the diaphragm region.
前記ブリツジの出力Voutが一般に数10mVで
あるのに対して、後述のセンサ出力Eoutは、こ
の出力Eoutを受け取る機器側の要求から、数V
が必要となる。したがつて、シリコン基板上に集
積化された増幅回路部分の増幅度は、少なくとも
100倍必要となる。そのため、入力側に接続され
る抵抗に対するフイードバツク抵抗の比は、100
倍以上となり、例えば数100kΩの抵抗値となつ
てしまう。この抵抗をオンチツプ化すると、莫大
な面積が必要となり、面積の確保が困難になると
ともに、チツプのコスト等に反映する。そこで、
チツプ上に薄膜で形成したり、厚膜抵抗で形成し
た方が実用的とされている。 While the bridge output Vout is generally several tens of mV, the sensor output Eout, which will be described later, is several volts due to the requirements of the equipment that receives this output Eout.
Is required. Therefore, the amplification degree of the amplifier circuit integrated on the silicon substrate is at least
100 times more required. Therefore, the ratio of the feedback resistance to the resistance connected to the input side is 100
The resistance value becomes more than twice that, for example, several 100 kΩ. Making this resistor on-chip requires a huge amount of area, which makes it difficult to secure the area and also increases the cost of the chip. Therefore,
It is considered more practical to form a thin film on a chip or a thick film resistor.
このような構造では、増幅回路の増幅度を決め
るために入力側に接続される抵抗とフイードバツ
ク抵抗との材質や構成が異なるところから、両抵
抗の温度係数に差が生じ、上記各種従来技術によ
り、圧力センサのブリツジ部分の温度による感度
低下を十分に補償したとしても、集積化された圧
力センサから得られる出力電圧Voutは、この増
幅回路部分の増幅度の温度による変化の影響を受
けることになる。 In such a structure, the resistor connected to the input side to determine the amplification degree of the amplifier circuit and the feedback resistor are made of different materials and have different configurations, resulting in a difference in temperature coefficient between the two resistors. Even if the decrease in sensitivity due to temperature in the bridge section of the pressure sensor is sufficiently compensated for, the output voltage Vout obtained from the integrated pressure sensor will be affected by changes in the amplification degree of the amplifier circuit section due to temperature. Become.
増幅回路も含めた集積化に対する配慮を欠いた
上記従来技術では、いずれも、増幅回路も含めた
精密な温度補償ができないという欠点があつた。 All of the above-mentioned conventional techniques, which lack consideration for integration including the amplifier circuit, have the drawback of not being able to perform precise temperature compensation including the amplifier circuit.
本発明の目的は、ダイアフラムを形成した基板
上に集積化された圧力センサ部分とその増幅回路
部分のうち、圧力センサ部分の温度による感度の
変動のみならず、増幅回路部分の増幅度を決める
抵抗等の温度による変動も含めて総合的に温度補
償し、しかも電源電圧が変動してもその温度補償
特性が変化しない補償手段を備えた圧力センサを
提供することである。 Among the pressure sensor part and its amplifier circuit part integrated on a substrate on which a diaphragm is formed, the object of the present invention is to not only change the sensitivity of the pressure sensor part due to temperature, but also to improve the resistance of the pressure sensor part that determines the amplification degree of the amplifier circuit part. It is an object of the present invention to provide a pressure sensor equipped with a compensating means that comprehensively compensates for temperature including fluctuations caused by temperature, and furthermore, its temperature compensation characteristics do not change even if the power supply voltage fluctuates.
本発明は、上記目的を達成するために、裏面を
ダイアフラムに加工した半導体基板の表面上に圧
力に応じて抵抗値が変わる複数の拡散抵抗からな
る応力感知素子を形成し、この応力感知素子から
の信号を所定の増幅率で増幅するために半導体基
板表面上に形成され温度に応じて抵抗値が変わる
増幅率設定抵抗を含む増幅回路を半導体基板の前
記ダイアフラム外の表面上に配置した集積型圧力
センサにおいて、前記半導体基板表面上に形成さ
れ応力感知素子の複数の拡散抵抗を定電流駆動し
電源電圧の影響を除去する定電流駆動手段と、半
導体基板表面上に形成されたトランジスタと拡散
抵抗素子とを含み温度に応じて変わるトランジス
タのVbe電圧および拡散抵抗素子の抵抗値の変化
に基づいて定電流駆動手段の設定電流を変更する
定電流変更手段とからなり、電源電圧の変化と応
力感知素子の温度による感度特性変化および増幅
回路の温度による増幅率変化とを総合的に補償す
る補償回路を設けた集積型圧力センサを提案する
ものである。 In order to achieve the above object, the present invention forms a stress sensing element consisting of a plurality of diffused resistors whose resistance value changes depending on pressure on the front surface of a semiconductor substrate whose back surface is processed into a diaphragm, and from this stress sensing element. An integrated type in which an amplifier circuit including an amplification factor setting resistor formed on the surface of a semiconductor substrate and whose resistance value changes depending on temperature is arranged on the surface of the semiconductor substrate outside the diaphragm in order to amplify the signal at a predetermined amplification factor. In the pressure sensor, a constant current driving means is formed on the surface of the semiconductor substrate and drives a plurality of diffused resistors of the stress sensing element with a constant current to remove the influence of a power supply voltage, and a transistor and a diffused resistor are formed on the surface of the semiconductor substrate. and a constant current changing means that changes the set current of the constant current driving means based on changes in the Vbe voltage of the transistor that changes depending on the temperature and the resistance value of the diffused resistance element, and detects changes in power supply voltage and stress. This paper proposes an integrated pressure sensor equipped with a compensation circuit that comprehensively compensates for changes in sensitivity characteristics due to temperature of the element and changes in amplification factor due to temperature of the amplifier circuit.
前記定電流変更手段は、より具体的には、エミ
ツタ面積が異なる複数の前記トランジスタのVbe
電圧に基づいて絶対温度に比例した電圧を得る回
路と、不純物濃度が異なる複数の前記拡散抵抗素
子を含み前記絶対温度に比例した電圧を定電流駆
動手段の設定電流に変換する電圧−電流変換回路
とからなる。 More specifically, the constant current changing means changes the Vbe of the plurality of transistors having different emitter areas.
A voltage-current conversion circuit that includes a circuit that obtains a voltage proportional to absolute temperature based on the voltage, and a plurality of the diffusion resistance elements having different impurity concentrations, and converts the voltage proportional to the absolute temperature into a set current of the constant current driving means. It consists of.
本発明においては、まず、電源電圧の変動がブ
リツジ構成の応力感知素子の検知信号に与える影
響は、基本的に前記ブリツジを定電流駆動して排
除する。 In the present invention, first, the influence of fluctuations in power supply voltage on the detection signal of the stress sensing element having a bridge configuration is basically eliminated by driving the bridge at a constant current.
次に、応力感知素子と増幅器とを集積化し小型
化する要求に答えるには、温度係数が小さい金属
膜抵抗と温度係数が大きい拡散抵抗とを増幅器の
増幅率決定素子に混用せざるを得ないので、金属
膜抵抗と拡散抵抗との混用による温度変化の全体
出力感度への影響は、上記定電流回路の設定電流
を温度に応じて変更する。 Next, in order to meet the demand for integrating and miniaturizing stress-sensing elements and amplifiers, it is necessary to mix a metal film resistor with a small temperature coefficient and a diffused resistor with a large temperature coefficient in the amplification factor determining element of the amplifier. Therefore, the influence of temperature change on the overall output sensitivity due to the mixed use of a metal film resistor and a diffused resistor is determined by changing the set current of the constant current circuit according to the temperature.
具体的には、トランジスタのVbeの温度依存性
を利用し、2つのトランジスタのVbeの差ΔVbe
をパラメータとして用いる。また、複数の拡散抵
抗の温度係数を不純物濃度で調整し、前記差電圧
ΔVbeに基づいて、定電流回路の設定電流を温度
に応じて変更する。 Specifically, by using the temperature dependence of Vbe of a transistor, the difference in Vbe of two transistors ΔVbe
is used as a parameter. Furthermore, the temperature coefficients of the plurality of diffused resistors are adjusted by the impurity concentration, and the set current of the constant current circuit is changed according to the temperature based on the differential voltage ΔVbe.
第2図は、シリコンダイアフラム型圧力センサ
の温度に対する感度の変化の一例を示す図であ
る。この特性は、第1図に示したブリツジ構成の
圧力センサを定電圧駆動した場合の特性である。 FIG. 2 is a diagram showing an example of a change in sensitivity with respect to temperature of a silicon diaphragm pressure sensor. This characteristic is the characteristic when the pressure sensor having the bridge configuration shown in FIG. 1 is driven at a constant voltage.
詳しくは、1981年9月25日に開催された日本機
械学会・精密機械学会共催の日立地方講演会の
〓講演論文集〓No.105「工業計器用半導体圧力セン
サの構造解析」に示されているように、拡散抵抗
の不純物濃度の感度への影響は大きくないが、シ
リコンダイアフラムとそれを取り付けるダイの線
膨張係数の違いという機械的要因の感度への影響
が大きい。すなわち、本来は圧力のみによつてシ
リコンダイアフラムに生ずる応力の値が熱歪の影
響を受け、圧力センサの感度の変化となつて現れ
る。 For details, see ``Structural Analysis of Semiconductor Pressure Sensors for Industrial Instruments,'' No. 105 of the Proceedings of the Hitachi Regional Conference, jointly sponsored by the Japan Society of Mechanical Engineers and the Japan Society of Precision Mechanical Engineers, held on September 25, 1981. As shown, the impurity concentration of the diffused resistance does not have a large effect on sensitivity, but the mechanical factor of the difference in linear expansion coefficient between the silicon diaphragm and the die to which it is attached has a large effect on sensitivity. That is, the value of stress that would normally occur in the silicon diaphragm only due to pressure is affected by thermal strain, resulting in a change in the sensitivity of the pressure sensor.
さて、第2図は、より具体的に説明すると、シ
リコンダイアフラムをホウケイ酸ガラスに接着し
た圧力センサの特性である。この特性は次の実験
式で表される。 More specifically, FIG. 2 shows the characteristics of a pressure sensor in which a silicon diaphragm is bonded to borosilicate glass. This characteristic is expressed by the following empirical formula.
Vout(T)=Vout(T0){1+ξ(1/T−1/T
0)}…(1)
ただし、ξはサンプルによつて異なるが、例え
ば233Kである。 Vout(T)=Vout(T 0 ) {1+ξ(1/T-1/T
0 )}...(1) However, ξ differs depending on the sample, but is, for example, 233K.
本発明による温度補償手段を備え集積化された
圧力センサの基本的系統構成の一例を第3図に示
す。圧力センサ部分のブリツジを構成する拡散ゲ
ージ抵抗G1〜G4は、シリコンダイアフラム面上
に拡散されている。2は本発明による温度補償回
路、3は抵抗R3,R4とともに検出信号増幅回路
を形成する増幅器である。 An example of the basic system configuration of an integrated pressure sensor equipped with temperature compensation means according to the present invention is shown in FIG. Diffusion gauge resistors G1 to G4 constituting the bridge of the pressure sensor section are diffused on the silicon diaphragm surface. 2 is a temperature compensation circuit according to the present invention, and 3 is an amplifier forming a detection signal amplification circuit together with resistors R 3 and R 4 .
すでに述べたように、ブリツジG1〜G4の出力
Voutが一般に数10mVであるのに対して、増幅
回路3からのセンサ出力Eoutは数Vが要求され
る。したがつて、シリコン基板上に集積化された
増幅回路部分3,R3,R4の増幅度は、少なくと
も100倍必要となる。そのため、入力側に接続さ
れる抵抗R3に対するフイードバツク抵抗R4の比
は100倍以上となり、例えば数100kΩの抵抗値に
なつてしまう。この抵抗R4をオンチツプ化する
と、莫大な面積が必要となり、チツプのコスト等
にも反映する。そこで、このような値の抵抗は、
チツプ上に薄膜で形成したり、厚膜で形成する。 As already mentioned, the output of bridges G 1 to G 4
While Vout is generally several tens of mV, the sensor output Eout from the amplifier circuit 3 is required to be several volts. Therefore, the amplification degree of the amplifier circuit portion 3, R 3 and R 4 integrated on the silicon substrate must be at least 100 times. Therefore, the ratio of the feedback resistor R 4 to the resistor R 3 connected to the input side is 100 times or more, resulting in a resistance value of several hundred kΩ, for example. If this resistor R4 is made on-chip, a huge area will be required, which will also be reflected in the cost of the chip. Therefore, a resistance of such a value is
It can be formed as a thin film or as a thick film on the chip.
このように、増幅回路の増幅度を決めるために
増幅器3の入力側に接続される抵抗R3とフイー
ドバツク抵抗のR4との材質が異なるところから、
両抵抗R3,R4の温度係数に差が生じ、圧力セ
ンサのブリツジ部分の温度による感度低下を十分
に補償したとしても、集積化された圧力センサか
ら得られる出力電圧Eoutは、この増幅回路部分
3,R3,R4の増幅度の温度による変化の影響を
受けることになる。 In this way, since the materials of the resistor R3 connected to the input side of the amplifier 3 and the feedback resistor R4 are different to determine the amplification degree of the amplifier circuit,
Even if a difference occurs in the temperature coefficients of both resistors R3 and R4 and the decrease in sensitivity due to temperature of the bridge portion of the pressure sensor is sufficiently compensated for, the output voltage Eout obtained from the integrated pressure sensor is , R 3 , and R 4 due to temperature changes.
そこで、次に、この増幅回路部分3,R3,R4
の増幅度の温度による変化の影響の補償も含めた
温度補償の原理を説明する。 Therefore, next, this amplifier circuit part 3, R 3 , R 4
The principle of temperature compensation, including compensation for the influence of changes in the degree of amplification due to temperature, will be explained.
前記拡散ゲージ抵抗G1〜G4で形成されている
ブリツジが、定電流Ib(T)で駆動されているとする
と、圧力センサの出力Eoutは、
Eout(T)=R4/R3Vout(T) …(2)
Vout(T)=K(1+αdr)Ib(T) …(3)
(3)式を(2)式に代入して、
Eout(T)=R4/R3(1+αr)K(1+αdr)
Ib(T)…(4)
ただし、K:比例定数
αdr:定電流駆動ブリツジの感度の温度変
化分
ar:抵抗の温度変化分
となる。 Assuming that the bridge formed by the diffusion gauge resistors G 1 to G 4 is driven by a constant current Ib(T), the output Eout of the pressure sensor is Eout(T)=R 4 /R 3 Vout( T) …(2) Vout(T)=K(1+αdr)Ib(T) …(3) Substituting equation (3) into equation (2), Eout(T)=R 4 /R 3 (1+αr) K(1+αdr)
Ib(T)...(4) where K: proportionality constant αdr: temperature change in sensitivity of constant current drive bridge ar: temperature change in resistance.
いま、抵抗R3の不純物濃度を拡散ゲージ抵抗
と同一に選ぶと、(4)式は、
Eout=R4/R3K(1+β)Ib(T) …(5)
ただし、β=αdr−αr
となる。ここで、R4はR3と比べて抵抗温度係数
が極めて小さい金属薄膜抵抗とすると、βは、定
電流駆動ブリツジの感度の温度変化分で、(1)式の
中のξ(1/T−1/T0)で表される量である。
したがつて、Eoutは、
Eout(T)=R4/R3K{1+ξ(1/T−1/T
0)Ib(T)}…(6)
となる。この(6)式から、Eoutを温度と無関係に
するためには、
Ib(T)=Ib(T0)1/1+ξ(1/T−1/T0) …(7)
とする必要があることが分かる。(7)式をさらに変
形すると、
Ib(T)=Ib(T0)T/T0÷{1+T1−ξ/T0 2
(T−T0)}…(8)
となる。T0=293Kすなわち20℃の第2図の特性
の例では、(T0−ξ)/T0 2は、7×10-4K-1とな
り、拡散抵抗で実現し得る値である。(8)式から明
らかなように、IbはTに比例する項とそれを抑制
する項とからなる。 Now, if the impurity concentration of the resistance R 3 is chosen to be the same as that of the diffusion gauge resistance, then equation (4) becomes Eout=R 4 /R 3 K(1+β)Ib(T)...(5) However, β=αdr−αr becomes. Here, if R 4 is a metal thin film resistor whose temperature coefficient of resistance is extremely small compared to R 3 , β is the temperature change in the sensitivity of the constant current drive bridge, and ξ (1/T −1/T 0 ).
Therefore, Eout is Eout(T)=R 4 /R 3 K{1+ξ(1/T-1/T
0 )Ib(T)}...(6). From this equation (6), in order to make Eout independent of temperature, it is necessary to set Ib(T)=Ib(T 0 )1/1+ξ(1/T-1/T 0 )...(7) I understand that. Further transforming equation (7), Ib(T)=Ib(T 0 )T/T 0 ÷{1+T 1 −ξ/T 0 2
(T−T 0 )}…(8). In the example of the characteristics shown in FIG. 2 at T 0 =293K, that is, 20° C., (T 0 −ξ)/T 0 2 is 7×10 −4 K −1 , which is a value that can be realized with a diffused resistor. As is clear from equation (8), Ib consists of a term proportional to T and a term that suppresses it.
さて、(8)式で示される駆動電流の温度特性を実
現する回路である温度補償回路2の詳細な回路の
一例を第4図に示す。図において、20および3
0は、トランジスタ40および50にそれぞれ定
電流を供給する定電流源、60および70は差動
増幅器、80は電圧を電流に変換するためのトラ
ンジスタ、R5,R6,R7は拡散抵抗または薄膜抵
抗または厚膜抵抗である。 Now, FIG. 4 shows an example of a detailed circuit of the temperature compensation circuit 2, which is a circuit that realizes the temperature characteristic of the drive current shown by equation (8). In the figure, 20 and 3
0 is a constant current source that supplies constant current to transistors 40 and 50, respectively, 60 and 70 are differential amplifiers, 80 is a transistor for converting voltage into current, and R 5 , R 6 , and R 7 are diffused resistors or Thin film resistor or thick film resistor.
トランジスタ40および50のエミツタ面積の
比をγとすると、両者のVbeの差ΔVbeは、
ΔVbe=Tk/qlnγ …(9)
ここで、kはボルツマン定数、qは電荷量であ
る。したがつて、出力電流Ib(T)は、
Ib(T)=TkR6/qR5R7(lnγ)=kR60/qR50R70
(lnγ)T/1+(α5+α7−α6)(T−T0)…(10)
(8)式と(10)式とから、
kR60lnγ/qR50R70=Ib(T0)/T0 …(11)
α5+α7−α6=T0−ξ/T0 2
を満足するように、温度T0におけるそれぞれの
抵抗値R50,R60,R70および抵抗温度係数を選べ
ばよいことが分かる。拡散抵抗の温度係数は、周
知のように、不純物濃度に大きく依存するので、
前記条件を満足する不純物濃度を選べばよい。第
2図の特性においては、R7を金属の薄膜または
厚膜抵抗として温度係数を極めて小さくし、R6
の不純物濃度Nsを4×1018cm-3、R5の不純物濃
度Nsを2×1019cm-3とすれば、上式を満足する抵
抗温度係数が得られ、(1)式と実験結果との間には
良い近似が見られる。 When the ratio of the emitter areas of the transistors 40 and 50 is γ, the difference in Vbe between the two is ΔVbe=Tk/qlnγ (9) where k is Boltzmann's constant and q is the amount of charge. Therefore, the output current Ib(T) is Ib(T)=TkR 6 /qR 5 R 7 (lnγ)=kR 60 /qR 50 R 70
(lnγ)T/1+( α5 + α7 − α6 )(T− T0 )…(10) From equations (8) and (10), kR 60 lnγ/qR 50 R 70 = Ib(T 0 )/T 0 …(11) α 5 + α 7 − α 6 = T 0 −ξ/T 0 2 , the respective resistance values R 50 , R 60 , R 70 and resistance temperature coefficient at temperature T 0 It turns out that you should choose . As is well known, the temperature coefficient of diffused resistance largely depends on the impurity concentration, so
An impurity concentration that satisfies the above conditions may be selected. In the characteristics shown in Figure 2, R 7 is a metal thin film or thick film resistor with an extremely small temperature coefficient, and R 6
If the impurity concentration Ns of R 5 is 4 × 10 18 cm -3 and the impurity concentration Ns of R 5 is 2 × 10 19 cm -3 , a temperature coefficient of resistance that satisfies the above equation can be obtained, and equation (1) and experimental results can be obtained. A good approximation can be seen between.
なお、シリコンダイアフラムとダイとの関係
で、第2図の傾斜が小さくなることがある。この
ときには、ξが小さくなり、(T0−ξ)/T0 2を
大きく取らなければならない場合、抵抗温度係数
に大きな差を持たせなければならないから、R7
も抵抗温度係数の大きな拡散抵抗を使う必要があ
る。 Note that the slope shown in FIG. 2 may become smaller depending on the relationship between the silicon diaphragm and the die. In this case, if ξ becomes small and (T 0 - ξ)/T 0 2 must be made large, the temperature coefficient of resistance must have a large difference, so R 7
It is also necessary to use a diffused resistor with a large resistance temperature coefficient.
以上説明してきたように、本実施例において
は、ブリツジを定電流Ibで駆動する方式とし、こ
のIbが電源電圧Vccには依存せず、トランジスタ
固有の電圧Vbeと拡散ゲージ抵抗の温度係数αに
よつて決められるように工夫しているので、温度
補償特性は、電源電圧の変動の影響を受けないこ
とが分かる。すなわち、電源電圧に影響されるこ
となく、温度に依存するトランジスタのベース・
エミツタ間電圧Vbeと拡散抵抗とにより、増幅回
路の増幅率決定素子の温度変化も含めて半導体圧
力センサ全体の感度温度補償を正確に行うことが
できる。 As explained above, in this embodiment, the bridge is driven by a constant current Ib, and this Ib does not depend on the power supply voltage Vcc, but depends on the transistor-specific voltage Vbe and the temperature coefficient α of the diffusion gauge resistance. It can be seen that the temperature compensation characteristics are not affected by fluctuations in the power supply voltage because the temperature compensation characteristics are determined in such a way that they can be determined according to the temperature control characteristics. In other words, the temperature-dependent transistor base temperature is not affected by the power supply voltage.
By using the emitter voltage Vbe and the diffusion resistance, it is possible to accurately compensate for the sensitivity temperature of the entire semiconductor pressure sensor, including the temperature change of the amplification factor determining element of the amplifier circuit.
本発明によれば、電源電圧の変動はもちろん、
増幅回路の増幅率決定素子の温度変化も含めて半
導体圧力センサ全体の感度補償を正確に実行でき
る。 According to the present invention, not only fluctuations in power supply voltage but also
It is possible to accurately compensate for the sensitivity of the entire semiconductor pressure sensor, including the temperature change of the amplification factor determining element of the amplifier circuit.
第1図は従来の圧力センサの温度補償の一例の
原理を示す図、第2図はシリコン圧力センサの温
度に対する感度の特性を示す図、第3図は本発明
による圧力センサの温度補償の原理を示す図、第
4図は第3図温度補償のより具体的な実施例を示
す図である。
2……温度補償回路、3……検出信号増幅器、
20,30……定電流源、40,50……絶対温
度比例電圧演算用トランジスタ、60,70……
差動増幅器、80……電圧/電流変換用トランジ
スタ、R5,R6,R7……温度補償用抵抗。
Fig. 1 is a diagram showing the principle of an example of temperature compensation of a conventional pressure sensor, Fig. 2 is a diagram showing the temperature sensitivity characteristics of a silicon pressure sensor, and Fig. 3 is a diagram showing the principle of temperature compensation of a pressure sensor according to the present invention. FIG. 4 is a diagram showing a more specific embodiment of the temperature compensation shown in FIG. 3. 2...Temperature compensation circuit, 3...Detection signal amplifier,
20, 30... constant current source, 40, 50... transistor for absolute temperature proportional voltage calculation, 60, 70...
Differential amplifier, 80...Transistor for voltage/current conversion, R5 , R6 , R7 ...Resistor for temperature compensation.
Claims (1)
表面上に圧力に応じて抵抗値が変わる複数の拡散
抵抗からなる応力感知素子を形成し、前記応力感
知素子からの信号を所定の増幅率で増幅するため
に前記半導体基板表面上に形成され前記温度に応
じて抵抗値が変わる増幅率設定抵抗を含む増幅回
路を前記半導体基板の前記ダイアフラム外の表面
上に配置した集積型圧力センサにおいて、 前記半導体基板表面上に形成され前記応力感知
素子の複数の拡散抵抗を定電流駆動し電源電圧の
影響を除去する定電流駆動手段と、前記半導体基
板表面上に形成されたトランジスタと拡散抵抗素
子とを含み温度に応じて変わる前記トランジスタ
のVbe電圧および前記拡散抵抗素子の抵抗値の変
化に基づいて前記定電流駆動手段の設定電流を変
更する定電流変更手段とからなり、前記電源電圧
の変化と前記応力感知素子の温度による感度特性
変化および前記増幅回路の温度による増幅率変化
とを総合的に補償する補償回路を設けたことを特
徴とする集積型圧力センサ。 2 特許請求の範囲第1項に記載の集積型圧力セ
ンサにおいて、 前記定電流変更手段が、エミツタ面積が異なる
複数の前記トランジスタのVbe電圧に基づいて絶
対温度に比例した電圧を得る回路と、不純物濃度
が異なる複数の前記拡散抵抗素子を含み前記絶対
温度に比例した電圧を前記定電流駆動手段の設定
電流に変換する電圧−電流変換回路とからなるこ
とを特徴とする集積型圧力センサ。[Claims] 1. A stress sensing element consisting of a plurality of diffused resistors whose resistance value changes depending on pressure is formed on the front surface of a semiconductor substrate whose back surface is processed into a diaphragm, and a signal from the stress sensing element is transmitted to a predetermined level. An integrated pressure sensor, wherein an amplifier circuit including an amplification factor setting resistor formed on the surface of the semiconductor substrate and whose resistance value changes depending on the temperature is disposed on the surface of the semiconductor substrate outside the diaphragm for amplification at an amplification factor. A constant current driving means formed on the surface of the semiconductor substrate and driving a plurality of diffused resistors of the stress sensing element with a constant current to remove the influence of a power supply voltage, and a transistor and a diffused resistor formed on the surface of the semiconductor substrate. constant current changing means for changing the set current of the constant current driving means based on changes in the Vbe voltage of the transistor which changes depending on the temperature and the resistance value of the diffused resistance element, What is claimed is: 1. An integrated pressure sensor comprising a compensation circuit that comprehensively compensates for changes in sensitivity characteristics due to temperature of the stress sensing element and changes in amplification factor due to temperature of the amplifier circuit. 2. The integrated pressure sensor according to claim 1, wherein the constant current changing means includes a circuit that obtains a voltage proportional to absolute temperature based on the Vbe voltage of the plurality of transistors having different emitter areas, and an impurity. An integrated pressure sensor comprising a voltage-current conversion circuit that includes a plurality of the diffusion resistance elements having different concentrations and that converts a voltage proportional to the absolute temperature into a set current of the constant current driving means.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6231482A JPS58180926A (en) | 1982-04-16 | 1982-04-16 | pressure sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6231482A JPS58180926A (en) | 1982-04-16 | 1982-04-16 | pressure sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58180926A JPS58180926A (en) | 1983-10-22 |
| JPH0442612B2 true JPH0442612B2 (en) | 1992-07-14 |
Family
ID=13196543
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6231482A Granted JPS58180926A (en) | 1982-04-16 | 1982-04-16 | pressure sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58180926A (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5647484B2 (en) * | 1973-03-15 | 1981-11-10 |
-
1982
- 1982-04-16 JP JP6231482A patent/JPS58180926A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58180926A (en) | 1983-10-22 |
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