JPH0248865B2 - - Google Patents
Info
- Publication number
- JPH0248865B2 JPH0248865B2 JP55043108A JP4310880A JPH0248865B2 JP H0248865 B2 JPH0248865 B2 JP H0248865B2 JP 55043108 A JP55043108 A JP 55043108A JP 4310880 A JP4310880 A JP 4310880A JP H0248865 B2 JPH0248865 B2 JP H0248865B2
- Authority
- JP
- Japan
- Prior art keywords
- resistance
- resistor
- adjustment
- parallel
- zero point
- 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
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D3/00—Indicating or recording apparatus with provision for the special purposes referred to in the subgroups
- G01D3/028—Indicating or recording apparatus with provision for the special purposes referred to in the subgroups mitigating undesired influences, e.g. temperature, pressure
- G01D3/036—Indicating or recording apparatus with provision for the special purposes referred to in the subgroups mitigating undesired influences, e.g. temperature, pressure on measuring arrangements themselves
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Temperature Or Quantity Of Heat (AREA)
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
- Indication And Recording Devices For Special Purposes And Tariff Metering Devices (AREA)
- Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
Description
【発明の詳細な説明】
本発明はブリツジ回路、特に物理量変化に応じ
て抵抗値が変化する抵抗素子を4辺に配設したフ
ルブリツジ回路における零点調整あるいは零点移
動温度補償等を行う調整回路を付加したブリツジ
回路の改良に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention adds an adjustment circuit for zero point adjustment or zero point movement temperature compensation in a bridge circuit, particularly a full bridge circuit in which resistance elements whose resistance value changes according to changes in physical quantities are arranged on four sides. This paper relates to improvements to bridge circuits.
一般に、圧力、長さその他の物理量変化に応じ
て抵抗値が変化する例えば半導体歪みゲージ等の
抵抗素子を4辺に配設したフルブリツジ回路が電
気的測定手段として広範囲に用いられており、各
種の測定条件下においても簡便で正確な電気的測
定信号が検出し得るという利点を有する。この種
のブリツジ回路においては、ブリツジの検出精度
を向上させる為にブリツジ出力の零点調整及び零
点移動温度補償が必要となる。すなわち、零点調
整は、物理量が加わらない状態でブリツジ出力を
零にする測定条件を得る為に、4辺の抵抗値のア
ンバランスに起因するブリツジ出力(オフセツト
電圧)を零に調整することであり、また零点移動
温度補償は抵抗素子が物理量とは無関係に温度変
化の影響による熱応力あるいは素子自体の抵抗温
度特性のバラツキ等によつて生じるブリツジ回路
の零点出力の温度による移動(零点移動温度特
性)を補償するものである。前記各補償作業はブ
リツジ回路において不可欠なものであり、特に各
抵抗素子として半導体歪みゲージ等のように抵抗
温度係数の大きい素子を用いる場合、あるいは物
理量変化を極めて高精度で且つ安定に検出する場
合に正確な零点移動温度補償を行うことが必要と
される。 Generally, full-bridge circuits, in which resistance elements such as semiconductor strain gauges are arranged on four sides and whose resistance value changes according to changes in pressure, length, and other physical quantities, are widely used as electrical measurement means, and various types of It has the advantage that a simple and accurate electrical measurement signal can be detected even under measurement conditions. In this type of bridge circuit, zero point adjustment of the bridge output and zero point shift temperature compensation are required to improve bridge detection accuracy. In other words, zero point adjustment is the adjustment of the bridge output (offset voltage) caused by the unbalance of the resistance values on the four sides to zero in order to obtain measurement conditions that make the bridge output zero without any physical quantities being added. In addition, zero point shift temperature compensation is the shift of the zero point output of a bridge circuit due to temperature, which is caused by thermal stress due to the influence of temperature changes or variations in the resistance temperature characteristics of the element itself, regardless of physical quantities (zero point shift temperature compensation). ). Each of the above-mentioned compensation operations is essential in a bridge circuit, especially when using elements with large resistance temperature coefficients such as semiconductor strain gauges as each resistance element, or when detecting changes in physical quantities with extremely high precision and stability. It is necessary to perform accurate zero-point shift temperature compensation.
第1図には零点調整及び零点移動温度補償回路
が付加された従来のブリツジ回路が示され、ブリ
ツジ回路10の4辺には抵抗素子12,14,1
6及び18がそれぞれ設けられ、前記補償を行う
為に、抵抗素子12には直列抵抗rsが又抵抗素子
18には並列抵抗rPが接続され、両抵抗rS及びrP
の抵抗値を調整することによつて4辺の抵抗値と
抵抗温度係数を同時にバランスさせて零点調整と
零点移動温度補償とが行われている。前記両抵抗
rS及びrPは温度変化に対して実質的に抵抗変化を
生じないすなわち抵抗温度係数の小さい抵抗素子
からなる。 FIG. 1 shows a conventional bridge circuit to which a zero point adjustment and zero point movement temperature compensation circuit is added, and the four sides of the bridge circuit 10 have resistive elements 12, 14,
6 and 18, respectively, and in order to perform the compensation, a series resistor rs is connected to the resistive element 12, and a parallel resistor r P is connected to the resistive element 18, and both resistors r S and r P
By adjusting the resistance values of the four sides, the resistance values and resistance temperature coefficients of the four sides are simultaneously balanced, and zero point adjustment and zero point shift temperature compensation are performed. Both resistances
rS and rP are resistive elements that do not substantially change their resistance with respect to temperature changes, that is, have a small temperature coefficient of resistance.
第1図において、零点調整はブリツジ回路10
の4辺の抵抗値が2組の相対する2辺の抵抗値の
積が等しくなるように各挿入抵抗rS、rPの抵抗値
を調整することにより行われるが、勿論、この零
点調整のみを行えば調整辺の抵抗温度係数は変化
することが明らかである。一方、零点移動温度補
償は抵抗温度係数の大きい辺に挿入した調整抵抗
にて当該辺の抵抗温度係数を小さくし、4辺の抵
抗温度係数がバランスが得られるが、勿論この場
合においても、調整された辺の抵抗値は変化し、
零点が移動することは明らかである。すなわち、
零点調整及び抵抗移動温度補償は互に相関性を有
しているので、実際の調整時においては、直列抵
抗rSと並列抵抗rPの各抵抗値とこれらを接続する
辺とを適宜選択することにより零点調整と零点移
動温度補償とを同時に行い、この時の各抵抗値の
選択は周知のように下記近似式にて設定される。 In FIG. 1, the zero point adjustment is performed by the bridge circuit 10.
This is done by adjusting the resistance values of each insertion resistor r S and r P so that the resistance values of the four sides of the two pairs of resistance values of two opposing sides are equal, but of course, only this zero point adjustment It is clear that if this is done, the temperature coefficient of resistance of the adjusted side will change. On the other hand, in zero-point movement temperature compensation, the resistance temperature coefficient of the four sides is balanced by using an adjustment resistor inserted in the side with the large resistance temperature coefficient, and the resistance temperature coefficient of the four sides can be balanced, but of course, even in this case, the adjustment The resistance value of the side changes,
It is clear that the zero point moves. That is,
Since zero point adjustment and resistance movement temperature compensation have a mutual correlation, during actual adjustment, the resistance values of the series resistance r S and parallel resistance r P and the side connecting them should be selected appropriately. As a result, zero point adjustment and zero point movement temperature compensation are performed at the same time, and the selection of each resistance value at this time is set using the following approximate formula, as is well known.
rS=2R△VT/Vio・R/△R−△VO/Vio …(1)式
rP=R/2(△VO/Vin+△VT/Vin・R/△R)…(2
)式
上式においてRは各抵抗素子12,14,1
6,18として拡散型半導体歪みゲージを用いた
時の同一の各素子抵抗値、△Rは各抵抗素子1
2,14,16,18の温度変化△Tに対する抵
抗変化量、Vioはブリツジ回路10の入力端子間
電圧、△VOは零点出力電圧、△VTは温度変化△
Tに対する零点移動量である。 r S = 2R△V T /V io・R/△R−△V O /V io …(1) formula r P = R/2 (△V O /Vin+△V T /Vin・R/△R) …(2
) formula In the above formula, R is each resistance element 12, 14, 1
6 and 18 are the same resistance values of each element when diffused semiconductor strain gauges are used, and △R is the resistance value of each resistance element 1.
2, 14, 16, and 18 with respect to temperature change △T, V io is the voltage between the input terminals of bridge circuit 10, △V O is the zero point output voltage, △V T is the temperature change △
This is the zero point movement amount with respect to T.
なお、上式は近似解である為、実際の調整は、
いづれか一方の抵抗rS,rPを所定辺に接続した
後、他方の抵抗をブリツジ回路10の零点出力が
実際に零となるように調整した状態で行われる。 Note that the above equation is an approximate solution, so the actual adjustment is
After one of the resistors r S and r P is connected to a predetermined side, the other resistor is adjusted so that the zero point output of the bridge circuit 10 actually becomes zero.
従来のブリツジ回路においては、抵抗素子1
2,14,16,18を半導体歪みゲージで形成
しその抵抗値が1〜2キロオームの場合、前記直
列抵抗rSを100オーム程度以下そして並列抵抗rP
を数10キロオーム以上とすることが一般的であ
り、このような実際のブリツジ回路においては各
調整抵抗rS及びrPの値を微調整することが極めて
困難であるという欠点があつた。すなわち、零点
出力を例えば±0.1mV程度以下に微調整しようと
する場合、前記直列抵抗rSの微調整によれば0.1
オーム以下の値まで細かく調整する必要が生じ、
この為に前記直列抵抗rSを調整可能な小さな抵抗
値を有する複数の固定抵抗の組合わせで構成した
りあるいは1オーム程度の可変抵抗を用いなけれ
ばならないという問題を生じる。しかしながら、
複数の固定抵抗の組合わせはブリツジ回路を複雑
及び高価格とする欠点を有し、又抵抗値の低い可
変抵抗はその形状が大型化するという欠点があつ
た。そして、前記微調整を並列抵抗rPで行う場合
には、並列抵抗rPの形状が大型化し、又適当な抵
抗素子が得られないという問題があり、又並列抵
抗値を更に大きくする場合には、その挿入辺を変
更しなければならないという問題が生じ、いずれ
も場合においてもその微調整が極めて困難になる
という欠点があつた。 In the conventional bridge circuit, the resistor element 1
2, 14, 16, and 18 are formed by semiconductor strain gauges and the resistance value is 1 to 2 kilohms, the series resistance r S is about 100 ohms or less, and the parallel resistance r P
is generally several tens of kilohms or more, and in such an actual bridge circuit, there is a drawback that it is extremely difficult to finely adjust the values of each adjustment resistor r S and r P . In other words, when trying to finely adjust the zero point output to, for example, about ±0.1 mV or less, the fine adjustment of the series resistor r S requires 0.1 mV or less.
It becomes necessary to finely adjust the value to below ohm.
For this reason, a problem arises in that the series resistor r S must be constructed from a combination of a plurality of fixed resistors having adjustable small resistance values, or a variable resistor of about 1 ohm must be used. however,
The combination of a plurality of fixed resistors has the disadvantage of making the bridge circuit complicated and expensive, and the variable resistor with a low resistance value has the disadvantage of increasing its size. When the above-mentioned fine adjustment is performed using a parallel resistor r P , there is a problem that the shape of the parallel resistor r P becomes large and that an appropriate resistance element cannot be obtained. However, the problem arises that the insertion edge must be changed, and in both cases, fine adjustment is extremely difficult.
特に、前記微調整はブリツジ回路10を圧力変
換器として用いた場合等に大きな問題を生じる場
合がある。すなわち、ブリツジ回路にて絶対圧型
の圧力変換器を構成し、大気圧の変動あるいは大
気圧以上の圧力変動を気圧変動も含めて絶対圧変
化として検出する際、標準大気圧の時にブリツジ
出力を零とする調整が必要となるが、この時、前
述した調整困難な場合が生じやすい。一般に、圧
力変換器に作用する圧力が零(真空)であつて、
起歪部に歪みが発生していない状態で、出力電圧
がほぼ零値になり、又その時の温度による出力変
化が小さい状態が得られた場合においても、標準
大気圧における零点出力はそれ自体零点移動温度
特性を有し、この特性が第2図に示される。すな
わち、零点出力として標準大気圧出力に相当する
電圧△VOを設定した時には、零点移動温度特性
として第2図に示される標準大気圧出力△VOの
出力低下に相当する零点移動△VTが生じる。そ
こで、第2図の零点出力△VO及び零点移動△VT
をいずれも零とするように前記直列抵抗rS及び並
列抵抗rPの値を求めると、並列抵抗rPは一般に
100キロオーム以上となり、又その接続辺も第1
図の素子16あるいは18のいずれかに分れ、そ
の設定が極めて困難になるという問題がある。こ
れは直列抵抗rSによつて素子12の辺の抵抗値を
大きくして零点出力を負側へ移行させると同時に
この辺の抵抗温度係数を小さくして零点移動温度
特性を正側に変化させ直列抵抗rSだけで零点出力
を零にする効果及び零点移動温度補償の効果がほ
とんど得られてしまい、並列抵抗rPはわずかな零
点出力の調整だけに使用されることとなる為であ
る。 In particular, the fine adjustment may cause a big problem when the bridge circuit 10 is used as a pressure transducer. In other words, when configuring an absolute pressure transducer with a bridge circuit and detecting atmospheric pressure fluctuations or pressure fluctuations above atmospheric pressure as absolute pressure changes, including atmospheric pressure fluctuations, the bridge output is set to zero at standard atmospheric pressure. However, at this time, the above-mentioned difficulty in adjustment is likely to occur. Generally, the pressure acting on the pressure transducer is zero (vacuum) and
Even if the output voltage becomes almost zero with no strain occurring in the strain-generating part, and the output change due to temperature at that time is small, the zero point output at standard atmospheric pressure is itself zero point. It has a moving temperature characteristic, which is shown in FIG. In other words, when the voltage △V O corresponding to the standard atmospheric pressure output is set as the zero point output, the zero point shift △V T corresponds to the output decrease of the standard atmospheric pressure output △V O shown in Figure 2 as the zero point movement temperature characteristic. occurs. Therefore, the zero point output △V O and zero point movement △V T in Figure 2
If the values of the series resistance r S and parallel resistance r P are determined so that both are zero, then the parallel resistance r P is generally
It is more than 100 kilohms, and the connection side is also the first
There is a problem that the device is separated into either the element 16 or 18 shown in the figure, and its setting becomes extremely difficult. This is done by increasing the resistance value on the side of the element 12 using the series resistor r S to shift the zero point output to the negative side, and at the same time decreasing the resistance temperature coefficient on this side to change the zero point shift temperature characteristic to the positive side. This is because the effect of reducing the zero point output to zero and the effect of zero point movement temperature compensation can be obtained only with the resistor r S , and the parallel resistor r P is used only for slightly adjusting the zero point output.
いずれにおいても、従来装置では、直並列抵抗
の抵抗値が調整の行いにくい範囲にある為に正確
な微調整を得ることが極めて困難であるという欠
点があつた。 In either case, the conventional device has the disadvantage that it is extremely difficult to obtain accurate fine adjustment because the resistance values of the series-parallel resistors are in a range that is difficult to adjust.
本発明は上記従来の課題に鑑みなされたもので
あり、その目的は、零点の微調整を極めて容易に
行うことができる改良されたブリツジ回路を提供
することにある。 The present invention has been made in view of the above-mentioned conventional problems, and an object of the present invention is to provide an improved bridge circuit that allows fine adjustment of the zero point to be performed extremely easily.
上記目的を達成する為に、本発明は、4辺のそ
れぞれに物理量変化に応じて抵抗値が変化する抵
抗素子が接続され、相対する一対の電源端子間に
電源を接続し、他の一対の出力端子から出力電圧
を取出すブリツジ回路において、前記ブリツジ回
路の任意の1辺にその辺の抵抗素子より十分に大
きな抵抗値を有するバイアス用並列抵抗を予め接
続し、このバイアス用並列抵抗の接続されたブリ
ツジ辺と隣接するブリツジ辺に調整用の並列抵抗
を接続し、更に他のブリツジ辺に調整用の直列抵
抗を接続し、前記バイアス用並列抵抗、調整用並
列抵抗及び直列抵抗を温度変化に対して実質的に
抵抗変化を生じない抵抗素子から形成し、バイア
ス用並列抵抗を予め接続しておくことによつてそ
の後に接続する調整用の並列抵抗値を前記バイア
ス用並列抵抗と同程度の抵抗値範囲に設定し、調
整用の直列抵抗及び並列抵抗によつてブリツジ回
路の零点調整及び零点移動温度補償を行うことを
特徴とする。 In order to achieve the above object, the present invention connects a resistive element whose resistance value changes according to a change in physical quantity to each of the four sides, connects a power source between a pair of opposing power terminals, and connects a power source between a pair of opposing power terminals. In a bridge circuit that extracts an output voltage from an output terminal, a bias parallel resistor having a sufficiently larger resistance value than the resistance element on that side is connected in advance to any one side of the bridge circuit, and the bias parallel resistor is connected in advance. A parallel resistor for adjustment is connected to the bridge side adjacent to the bridge side, and a series resistor for adjustment is connected to the other bridge side, and the bias parallel resistor, parallel adjustment resistor, and series resistor are connected to temperature changes. By forming a resistance element that does not substantially change the resistance and connecting a bias parallel resistance in advance, the value of the adjustment parallel resistance to be connected subsequently can be set to the same level as the bias parallel resistance. It is characterized in that the resistance value is set within a range, and the zero point adjustment and zero point movement temperature compensation of the bridge circuit are performed using a series resistor and a parallel resistor for adjustment.
以下図面に基づいて本発明の好適な実施例を説
明する。 Preferred embodiments of the present invention will be described below based on the drawings.
第3図には本発明にかかるブリツジ回路の第1
実施例が示され、第1図の従来回路と同一部材に
は同一符号を付して説明を省略する。第3図の各
抵抗素子12,14,16,18は拡散型半導体
歪みゲージからなり、このブリツジ回路10は例
えば圧力変換として利用することができ、第4,
5図にはブリツジ回路10を含む圧力変換器の好
適な実施例が示されている。 FIG. 3 shows the first bridge circuit according to the present invention.
An embodiment is shown, and the same members as those in the conventional circuit shown in FIG. Each resistance element 12, 14, 16, 18 in FIG.
A preferred embodiment of a pressure transducer including a bridge circuit 10 is shown in FIG.
第4,5図においてシリコン単結晶の薄板から
なるシリコンダイアフラム20がその周縁部にて
基台22に真空中でガラス接着されており、その
中央部には薄肉状の起歪部24が形成され、該起
歪部24の表面中央部に拡散型半導体歪みゲージ
からなる抵抗素子12,16が、又周縁部に同じ
く拡散型半導体歪みゲージからなる抵抗素子1
4,18がそれぞれ拡散手法にて形成されてい
る。そして、各素子12,14,16,18はシ
リコンダイアフラム20上に形成された拡散リー
ド部又は蒸着アルミ配線によつて直列に接続さ
れ、その両端及び3個の接続点はシリコンダイア
フラム20の周縁に設けられたアルミ電極リード
端子26〜34に接続され、第3図のブリツジ回
路10が形成されている。従つて、前記シリコン
ダイアフラム20に圧力が作用すると抵抗素子1
2,16と抵抗素子14,18には引張側及び圧
縮側の反対方向の歪みが加わり、抵抗値がそれぞ
れ反対方向に変化し、圧力を正確に電気的に検出
することが可能となる。なお、第5図から明らか
なように、起歪部24と基台22との間には真空
の基準圧室36が形成され、絶対圧型の圧力変換
器を構成しているが、鎖線で示されるように、基
準圧室36を基台22に設けられた背圧孔38に
て外部と導通することによつて、ゲージ圧型又は
差圧型の圧力変換器を構成することができる。 In FIGS. 4 and 5, a silicon diaphragm 20 made of a thin plate of silicon single crystal is glass-bonded to a base 22 at its periphery in a vacuum, and a thin strain-generating portion 24 is formed in its center. , resistance elements 12 and 16 made of diffused type semiconductor strain gauges are disposed at the center of the surface of the strain-generating portion 24, and resistance elements 1 also made of diffused type semiconductor strain gauges are disposed at the periphery.
4 and 18 are each formed by a diffusion method. Each of the elements 12, 14, 16, and 18 is connected in series by a diffusion lead portion or vapor-deposited aluminum wiring formed on the silicon diaphragm 20, and both ends and three connection points are connected to the periphery of the silicon diaphragm 20. The bridge circuit 10 shown in FIG. 3 is connected to the provided aluminum electrode lead terminals 26 to 34 to form the bridge circuit 10 shown in FIG. Therefore, when pressure is applied to the silicon diaphragm 20, the resistance element 1
2 and 16 and the resistance elements 14 and 18 are subjected to strains in opposite directions on the tension side and compression side, and the resistance values change in opposite directions, making it possible to accurately detect pressure electrically. As is clear from FIG. 5, a vacuum reference pressure chamber 36 is formed between the strain generating part 24 and the base 22, and constitutes an absolute pressure type pressure transducer. By communicating the reference pressure chamber 36 with the outside through the back pressure hole 38 provided in the base 22, a gauge pressure type or differential pressure type pressure transducer can be constructed.
以上のようにして、本発明にかかるブリツジ回
路10は第4,5図の圧力変換器その他として用
いることができ、次に、第3図における本発明の
調整回路の構造を説明する。 As described above, the bridge circuit 10 according to the present invention can be used as the pressure transducer shown in FIGS. 4 and 5, etc. Next, the structure of the regulating circuit according to the present invention shown in FIG. 3 will be explained.
第3図において、ブリツジ回路10の相対する
電源端子40,42はそれぞれ電源44の正極及
び負極に接続され、ブリツジ回路10に直流電圧
が供給されている。そして、ブリツジ回路10の
他方の相対する一対の出力端子46,48はそれ
ぞれ正出力端子50及び負出力端子52に接続さ
れている。 In FIG. 3, opposing power supply terminals 40 and 42 of the bridge circuit 10 are connected to the positive and negative poles of a power supply 44, respectively, and a DC voltage is supplied to the bridge circuit 10. The other pair of opposing output terminals 46 and 48 of the bridge circuit 10 are connected to a positive output terminal 50 and a negative output terminal 52, respectively.
そして、ブリツジ回路10の各4辺から任意に
選択された辺例えば実施例において抵抗素子12
の辺に調整用の直列抵抗54が接続されている。
更に、例えば実施例において抵抗素子16が接続
されている辺にはバイアス用並列抵抗56が、又
この辺と隣接する辺実施例においては抵抗素子1
8が接続されている辺に調整用並列抵抗58が接
続されている。前記直列抵抗54及び両並列抵抗
56,58は拡散型半導体歪みゲージから成る抵
抗素子12,14,16,18の抵抗温度係数と
比して充分小さい抵抗温度係数を有し、実質的に
温度変化によつて抵抗変化を生じない抵抗素子か
ら形成されている。 Then, on each of the four sides of the bridge circuit 10, for example, the resistance element 12 is
A series resistor 54 for adjustment is connected to the side.
Furthermore, for example, in the embodiment, a bias parallel resistor 56 is connected to the side to which the resistance element 16 is connected, and in the embodiment, the resistance element 1 is connected to the side adjacent to this side.
A parallel adjustment resistor 58 is connected to the side to which 8 is connected. The series resistor 54 and both parallel resistors 56 and 58 have temperature coefficients of resistance that are sufficiently small compared to the temperature coefficients of resistance of the resistance elements 12, 14, 16, and 18 made of diffused semiconductor strain gauges, and are substantially free from temperature changes. It is formed from a resistance element that does not cause a change in resistance due to the change in resistance.
本発明の第1実施例は以上の構成からなり、そ
の調整作用を以下の調整手順に従つて説明する。 The first embodiment of the present invention has the above configuration, and its adjustment operation will be explained according to the following adjustment procedure.
(1) バイアス用並列抵抗56としてその抵抗値を
拡散型半導体歪みゲージより大きく好ましくは
10倍以上の大きさを有する値で、且つ抵抗値の
選択調整が容易で実際上最も使用しやすい範囲
から任意の抵抗値を選択してブリツジ回路10
の任意の1辺実施例においては抵抗素子16の
接続辺に接続する。半導体歪みゲージの抵抗値
がおよそ1〜2キロオームの場合、この並列抵
抗56の抵抗値は数10キロオーム〜100キロオ
ーム程度の範囲から選択することが好適であ
る。(1) The resistance value of the bias parallel resistor 56 is preferably larger than that of the diffused semiconductor strain gauge.
The bridge circuit 10 is constructed by selecting an arbitrary resistance value from a range that is 10 times or more larger, and which is easy to select and adjust, and which is actually the easiest to use.
In the embodiment of any one side, it is connected to the connecting side of the resistive element 16. When the resistance value of the semiconductor strain gauge is approximately 1 to 2 kilohms, the resistance value of the parallel resistor 56 is preferably selected from a range of several tens of kilohms to 100 kilohms.
(2) 第3図の直列抵抗54及び調整用並列抵抗5
8が接続されていない状態すなわち直列抵抗5
4が短絡した状態で圧力変換器を零点状態(ブ
リツジ出力を零にしたい状態)として零点出力
の値と零点移動温度特性を求める。(2) Series resistor 54 and adjustment parallel resistor 5 in Figure 3
8 is not connected, that is, the series resistance 5
4 is short-circuited and the pressure transducer is set to the zero point state (the state in which the bridge output is desired to be zero), and the value of the zero point output and the zero point shift temperature characteristic are determined.
(3) 前2項で求めた零点出力の値を零にし且つ零
点移動温度特性を温度補償するに必要な直列抵
抗54及び調整用並列抵抗58の抵抗値及びこ
れらの抵抗接続辺を前述した(1)、(2)式により求
める。(3) The resistance values of the series resistor 54 and adjustment parallel resistor 58 necessary to set the value of the zero point output obtained in the previous two sections to zero and to compensate for the temperature of the zero point shift temperature characteristic and the connection sides of these resistors are as described above ( Calculated using equations 1) and (2).
(4) 前3項より求められた計算結果に対応する直
列抵抗54及び調整用並列抵抗58を所定辺に
接続し、次にブリツジ回路10の零点出力が実
際に零となるように調整用並列抵抗58の抵抗
値を調整する。(なお、調整用並列抵抗58の
抵抗値は接続後に直接調整することも可能であ
り、この場合には前記(2)式の計算は不用とな
る。)
(5) 零点移動温度補償を更に高精度に行う為に、
前4項の調整後再度零点出力の値と零点移動温
度特性を求め、これに基づいて3,4項の計算
及び調整を行う。この時、3項では直列抵抗5
4の補正値を求め、4項では直列抵抗54の値
に前記補正値に従つた補正を加え、その後、調
整用並列抵抗58の抵抗値を調整して零点出力
の微調整を行う。以下この微調整を必要回数繰
り返すことにより、本発明の零点微調整を行う
ことができる。(4) Connect the series resistor 54 and the adjusting parallel resistor 58 corresponding to the calculation results obtained from the previous three items to the predetermined sides, and then connect the adjusting parallel resistor 58 so that the zero point output of the bridge circuit 10 actually becomes zero. Adjust the resistance value of the resistor 58. (In addition, the resistance value of the parallel adjustment resistor 58 can also be adjusted directly after connection, and in this case, the calculation of equation (2) above is unnecessary.) (5) Zero point shift temperature compensation can be further enhanced. In order to do it accurately,
After the adjustment in the previous four terms, the value of the zero point output and the zero point movement temperature characteristic are determined again, and based on these, the calculations and adjustments in the third and fourth terms are performed. At this time, in term 3, the series resistance 5
The correction value of 4 is obtained, and in the 4th term, the value of the series resistor 54 is corrected according to the correction value, and then the resistance value of the parallel adjustment resistor 58 is adjusted to finely adjust the zero point output. By repeating this fine adjustment a necessary number of times, the zero point fine adjustment of the present invention can be performed.
以上説明したように、第1実施例回路によれ
ば、抵抗値の選択が容易で且つ実際上最も使用し
やすい範囲から任意に選択されたバイアス用並列
抵抗56を予めブリツジ回路10の任意1辺すな
わち実施例における抵抗素子16の接続辺に接続
した後、零点調整と零点移動温度補償の為の直列
抵抗54及び調整用並列抵抗58の値を求めるの
で、必然的に、調整用並列抵抗58の抵抗値は予
め抵抗値の定められているバイアス用並列抵抗5
6の抵抗値に近接した値となり、その接続辺も電
源端子40,42を挾む隣接する辺に必然的に定
められることとなる。すなわち、ブリツジ回路1
0の互に隣接する2辺に同一抵抗値の並列抵抗を
接続すれば、両ブリツジ辺の抵抗値に対して同様
の変化を与え、又両ブリツジ辺の抵抗温度係数も
同様の変化を示すことから、このような両列抵抗
の隣接辺への接続ではブリツジ回路10の零点出
力及び零点移動温度特性になんら影響を与えない
こととなり、調整用に用いられる並列抵抗58の
抵抗値を調整に容易な抵抗値範囲とし且つ零点調
整及び零点移動温度補償を確実に行う為には、予
め並列抵抗58の抵抗値を設定する為のバイアス
用として用いる並列抵抗56を任意のブリツジ辺
に設ければ良いことが理解される。 As explained above, according to the first embodiment circuit, the parallel bias resistor 56, whose resistance value is easily selected and arbitrarily selected from the range that is most easily used in practice, is installed in advance on any side of the bridge circuit 10. That is, after connecting to the connection side of the resistance element 16 in the embodiment, the values of the series resistor 54 and the adjusting parallel resistor 58 for zero point adjustment and zero point movement temperature compensation are determined, so naturally, the values of the adjusting parallel resistor 58 are determined. The resistance value is a bias parallel resistor 5 whose resistance value is determined in advance.
The resistance value is close to the resistance value of No. 6, and the connection side is also necessarily set to the adjacent side sandwiching the power supply terminals 40 and 42. That is, bridge circuit 1
If parallel resistors of the same resistance value are connected to two adjacent sides of 0, the resistance value of both bridge sides will change in the same way, and the resistance temperature coefficient of both bridge sides will also show a similar change. Therefore, such connection of both column resistors to adjacent sides has no effect on the zero point output and zero point movement temperature characteristics of the bridge circuit 10, and the resistance value of the parallel resistor 58 used for adjustment can be easily adjusted. In order to obtain a suitable resistance value range and to ensure zero point adjustment and zero point movement temperature compensation, it is sufficient to provide a parallel resistor 56 used as a bias for setting the resistance value of the parallel resistor 58 in advance on any bridge side. That is understood.
以上のように、本発明によれば、予めバイアス
用並列抵抗をブリツジ回路の任意辺に接続するこ
とによつて、調整用並列抵抗の抵抗値を所望の抵
抗値範囲から任意に選択することが可能となる。 As described above, according to the present invention, by connecting the bias parallel resistor to any side of the bridge circuit in advance, the resistance value of the adjusting parallel resistor can be arbitrarily selected from a desired resistance value range. It becomes possible.
具体例として、前述した絶対圧型圧力変換器で
標準大気圧時の出力を零にしようとする場合、ブ
リツジ回路10の入力直流電圧Vio=6V、各抵抗
素子12,14,16,18の抵抗値R=1800オ
ーム、その抵抗温度係数1℃当り0.14%、圧力零
(真空)時の出力電圧を±30mV、標準大気圧に
おける出力感度を60mVそして出力の感度温度係
数を1℃当り−0.14%(これより1℃当りの△VT
は−0.084mVとなる。)とし、直列抵抗54、バ
イアス用並列抵抗56及び調整用の並列抵抗58
の各抵抗値をそれぞれr54、r56、r58とすると、
第1図の従来装置においては、r54=約50〜90オ
ーム(抵抗素子12に直列接続)そしてr58=約
200キロオーム〜∞(抵抗素子16又は18に並
列接続)となるのに対し、第3図の本実施例にお
いては、バイアス用並列抵抗値r56を100キロオー
ムにすれば、直列抵抗値r54は従来と同様の約50
〜90オーム(抵抗素子12に直列接続)となる
が、調整用の並列抵抗r58は約50〜100キロオーム
(抵抗素子18に並列接続)となり、このことか
ら、調整用の並列抵抗値r58をバイアス用並列抵
抗r56に近い値に設定することができ調整が極め
て容易となり、又その接続するブリツジ辺も特定
のブリツジ辺実施例においては抵抗素子18の接
続辺に定まることとなる。 As a specific example, when trying to make the output of the above-mentioned absolute pressure transducer zero at standard atmospheric pressure, the input DC voltage V io of the bridge circuit 10 = 6V, the resistance of each resistance element 12, 14, 16, 18. Value R = 1800 ohm, its resistance temperature coefficient is 0.14% per 1℃, the output voltage at zero pressure (vacuum) is ±30mV, the output sensitivity at standard atmospheric pressure is 60mV, and the output sensitivity temperature coefficient is -0.14% per 1℃. (From this, △V T per 1℃
becomes −0.084mV. ), a series resistor 54, a bias parallel resistor 56, and an adjustment parallel resistor 58.
Assuming that the resistance values of are r54, r56, and r58, respectively,
In the conventional device shown in Figure 1, r54 = approximately 50 to 90 ohms (connected in series with resistive element 12) and r58 = approximately
200 kilohms to ∞ (connected in parallel to resistive element 16 or 18), whereas in this embodiment shown in Fig. 3, if the bias parallel resistance value r56 is set to 100 kilohms, the series resistance value r54 becomes the same as before. about 50 similar
~90 ohms (connected in series with resistor element 12), but the parallel resistance r58 for adjustment is approximately 50 to 100 kilo ohms (connected in parallel to resistor element 18), and from this, the parallel resistance value r58 for adjustment is biased. The parallel resistance r56 can be set to a value close to that of the parallel resistance r56, making adjustment extremely easy, and the bridge side to which it is connected is also determined to be the connecting side of the resistor element 18 in a particular bridge side embodiment.
以上のようにして、直列抵抗54及び並列抵抗
58の低抗値を求め、これを各特定のブリツジ辺
に接続した後、本実施例回路の零点出力が実際に
零となるように並列抵抗58の抵抗値が調整され
る。この並列抵抗58の抵抗値はバイアス用並列
抵抗56によつて実際上最も使用しやすい範囲に
設定可能である為、零点調整は従来と比して極め
て容易に行うことができる。更に、本発明によれ
ば、調整用並列抵抗58の接続ブリツジ辺が特定
するので、従来のように調整の都度その接続辺を
変更することがなく、調整回路構成を著しく簡素
化することが可能となる。又、零点出力の微調整
は、予め並列抵抗58の調整によつて概略調整を
行つた後にバイアス用の並列抵抗56の抵抗値を
微小範囲で調整して行うことも可能であり、この
微調整は零点移動温度特性に大きな影響を与える
ことがないので、零点出力を0.1mV以下にまで微
調整しようとする場合においても、両並列抵抗5
6,58の調整にて正確な零点調整を行うことが
可能となる利点を有する。 As described above, after determining the low resistance values of the series resistor 54 and the parallel resistor 58 and connecting them to each specific bridge side, the parallel resistor 58 is connected so that the zero point output of the circuit of this embodiment actually becomes zero. The resistance value of is adjusted. Since the resistance value of this parallel resistor 58 can be set to a range that is actually most convenient for use with the bias parallel resistor 56, zero point adjustment can be performed much more easily than in the past. Furthermore, according to the present invention, since the connection bridge side of the parallel adjustment resistor 58 is specified, there is no need to change the connection side each time the adjustment is made as in the conventional case, and the configuration of the adjustment circuit can be significantly simplified. becomes. Further, fine adjustment of the zero point output can also be performed by making a rough adjustment in advance by adjusting the parallel resistor 58, and then adjusting the resistance value of the parallel resistor 56 for bias within a minute range, and this fine adjustment does not have a large effect on the zero point movement temperature characteristics, so even when trying to finely adjust the zero point output to 0.1 mV or less, both parallel resistors 5
This has the advantage that accurate zero point adjustment can be performed by adjusting the points 6 and 58.
なお、第3図の実施例における電源端子40,
42と出力端子46,48を任意に変更して、端
子40,42を出力端子に又端子46,48を電
源端子としても同様の効果を得ることが可能であ
る。 Note that the power terminal 40 in the embodiment of FIG.
42 and the output terminals 46, 48, the same effect can be obtained even if the terminals 40, 42 are used as output terminals and the terminals 46, 48 are used as power supply terminals.
更に、前記実施例において、電源44は通常の
場合定電圧電源とするが、抵抗素子12,14,
16,18を拡散型半導体歪みゲージで形成した
時の感度温度特性を温度補償する為に電源44を
定電流電源とすることも可能である。 Furthermore, in the embodiment, the power supply 44 is normally a constant voltage power supply, but the resistance elements 12, 14,
It is also possible to use the power source 44 as a constant current power source in order to compensate for the temperature sensitivity characteristics when the sensors 16 and 18 are formed of diffused semiconductor strain gauges.
第6図には本発明の第2実施例が示され、第3
図の第1実施例と同一部材には同一符号を付して
説明を省略する。第2実施例は零点微調整回路を
付加し、更に細かい零点調整を可能としたことを
特徴とし、抵抗素子18の一端と直列抵抗54の
一端との間に固定抵抗60及び可変抵抗62の並
列回路が接続され、該並列回路が零点微調整回路
を形成し、前記可変抵抗62の中間端子が正出力
端50に接続されている。 A second embodiment of the present invention is shown in FIG.
The same members as in the first embodiment shown in the drawings are given the same reference numerals and their explanations will be omitted. The second embodiment is characterized in that a zero point fine adjustment circuit is added to enable even finer zero point adjustment. The circuits are connected, the parallel circuit forming a zero point fine adjustment circuit, and the intermediate terminal of the variable resistor 62 is connected to the positive output terminal 50.
前記固定抵抗60と可変抵抗62との並列合成
抵抗値は該並列抵抗を流れる電流値と該並列抵抗
値との積が所定の調整電圧幅となるように設定
し、又両抵抗のうち固定抵抗60は並列合成抵抗
値に近い値とし一方可変抵抗62はその抵抗値が
できるだけ大きく且つその選択が容易で実際に使
用しやすい抵抗値に設定されている。第6図にお
ける零点微調整回路は初期組立て時からブリツジ
回路10に接続され、可変抵抗62の中間端子を
ほぼ抵抗値の中央位置に設定した状態で前記第1
実施例と同様の零点調整及び零点移動温度補償を
行つても良く、又ブリツジ回路10の零点調整及
び零点移動温度補償が行われた後にブリツジ回路
10に付加接続されても良い。なお、第6図にお
ける電源44は定電流電源から形成されている。 The parallel combined resistance value of the fixed resistor 60 and the variable resistor 62 is set so that the product of the current flowing through the parallel resistor and the parallel resistance value becomes a predetermined adjustment voltage width, and among both resistors, the fixed resistor The variable resistor 60 is set to a value close to the parallel combined resistance value, while the variable resistor 62 is set to a resistance value as large as possible, easy to select, and easy to use in practice. The zero point fine adjustment circuit in FIG. 6 is connected to the bridge circuit 10 from the time of initial assembly, and the intermediate terminal of the variable resistor 62 is set at approximately the center position of the resistance value.
The same zero point adjustment and zero point movement temperature compensation as in the embodiment may be performed, or the bridge circuit 10 may be additionally connected to the bridge circuit 10 after the zero point adjustment and zero point movement temperature compensation are performed. Note that the power source 44 in FIG. 6 is formed from a constant current power source.
本発明の第2実施例は以上の構成からなり、以
下にその作用を説明する。 The second embodiment of the present invention has the above configuration, and its operation will be explained below.
固定抵抗60及び可変抵抗62からなる零点微
調整回路には、抵抗素子12,18の電流が流
れ、固定抵抗60の両端には並列合成抵抗値と該
電流抵抗値の積に等しい電圧降下が生じる。この
時可変抵抗62の中間電位は前記零点微調整回路
が付加接続されていない第3図の第1実施例にお
ける出力端子46の電位に等しくなる。従つて可
変抵抗62の中間端子が抵抗値の中央位置にある
場合には、両出力端子50,52間に得られる出
力電圧は零点微調整回路が付加接続されていない
時の出力電圧と同一値となることが理解される。
そして、可変抵抗62の中間端子を動かせば、正
出力端子50からは可変抵抗62の中間端子移動
位置に対応した一定電圧だけ偏位した出力電圧が
得られ、可変抵抗62の調整によつてブリツジ回
路10の零点出力調整ができることとなる。この
時の調整電圧幅は前記並列合成値とその電流値と
の積に等しくなり、この電圧調整幅を小さくして
微細な調整を行う為には前記並列合成値を小さく
すれば良いことが明らかである。この並列合成抵
抗値の減少は単に固定抵抗60の抵抗値を小さく
するのみで良く、可変抵抗62の抵抗値は任意に
入手の容易な実際の使用に便利な可変抵抗値とす
ることができ、低価格で微調整容易なブリツジ回
路を得ることが可能となる。 The current of the resistance elements 12 and 18 flows through the zero point fine adjustment circuit consisting of the fixed resistor 60 and the variable resistor 62, and a voltage drop is generated across the fixed resistor 60 equal to the product of the parallel combined resistance value and the current resistance value. . At this time, the intermediate potential of the variable resistor 62 becomes equal to the potential of the output terminal 46 in the first embodiment of FIG. 3 to which the zero point fine adjustment circuit is not additionally connected. Therefore, when the intermediate terminal of the variable resistor 62 is at the center position of the resistance value, the output voltage obtained between both output terminals 50 and 52 is the same value as the output voltage when the zero point fine adjustment circuit is not additionally connected. It is understood that
Then, by moving the intermediate terminal of the variable resistor 62, an output voltage deviated by a constant voltage corresponding to the intermediate terminal movement position of the variable resistor 62 is obtained from the positive output terminal 50. This makes it possible to adjust the zero point output of the circuit 10. The adjustment voltage width at this time is equal to the product of the parallel composite value and its current value, and it is clear that in order to make fine adjustments by reducing the voltage adjustment width, the parallel composite value should be made smaller. It is. This parallel combined resistance value can be reduced by simply reducing the resistance value of the fixed resistor 60, and the resistance value of the variable resistor 62 can be arbitrarily set to a variable resistance value that is easily available and convenient for actual use. It becomes possible to obtain a bridge circuit that can be easily fine-tuned at a low cost.
具体例として、電源44から3mAの電流が供
給され、抵抗素子12,18にはその約半分の
1.5mA程度の電流が流れるものとし、この時±
1mV程度の微調整(調整電圧幅で2mV)を行い
得る回路を構成する為には、前記並列合成抵抗値
を約1.3オームとすれば良い。そして、この時の
固定抵抗60の抵抗値を約1.3オームとすれば、
可変抵抗62としては10〜100オーム以上の抵抗
値の素子を使用すれば良く、可変抵抗として小型
な且つ標準型の素子を利用することが可能とな
る。 As a specific example, a current of 3 mA is supplied from the power supply 44, and approximately half of the current is supplied to the resistive elements 12 and 18.
Assume that a current of about 1.5mA flows, and at this time ±
In order to configure a circuit that can perform fine adjustment of about 1 mV (2 mV in adjustment voltage width), the parallel combined resistance value should be about 1.3 ohm. If the resistance value of the fixed resistor 60 at this time is approximately 1.3 ohm, then
As the variable resistor 62, an element having a resistance value of 10 to 100 ohms or more may be used, and it is possible to use a small and standard type element as the variable resistor.
又、第6図の実施例によれば、可変抵抗62に
よる調整範囲は正側から及び負側におよぶので、
ブリツジ回路10の出力を増幅する為にIC直流
増幅器等をブリツジ回路10に直結した場合に
も、ブリツジ回路10の零点出力をIC直流増幅
器の入力オフセツト電圧(IC直流増幅器の出力
を零にする入力電圧)に等しくなるように正負両
方向に調整することができ、IC直流増幅器の出
力の零点調整を容易に行うことが可能となる。 Further, according to the embodiment shown in FIG. 6, the adjustment range by the variable resistor 62 extends from the positive side to the negative side.
Even when an IC DC amplifier or the like is directly connected to the bridge circuit 10 in order to amplify the output of the bridge circuit 10, the zero point output of the bridge circuit 10 is set to the input offset voltage of the IC DC amplifier (the input that makes the output of the IC DC amplifier zero). It can be adjusted in both positive and negative directions so that it is equal to the voltage (voltage), making it possible to easily adjust the zero point of the output of the IC DC amplifier.
第7図には本発明の第3実施例が示され、第6
図の第2実施例にスパン調整抵抗を付加接続した
ことを特徴とし、第6図と同一部材には同一符号
を付して説明を省略する。 A third embodiment of the present invention is shown in FIG.
This embodiment is characterized in that a span adjustment resistor is additionally connected to the second embodiment shown in the figure, and the same members as those in FIG.
第3実施例において、零点微調整回路の固定抵
抗は抵抗値のほぼ等しい固定抵抗60a,60b
に分割され、両固定抵抗60a,60bの共通接
続点と負出力端子52との間にスパン調整抵抗6
4が付加接続されたことを特徴とする。 In the third embodiment, the fixed resistors of the zero point fine adjustment circuit are fixed resistors 60a and 60b having almost equal resistance values.
A span adjustment resistor 6 is connected between the common connection point of both fixed resistors 60a and 60b and the negative output terminal 52.
4 is additionally connected.
すなわち、スパン調整抵抗64はこの抵抗値を
小さくすれば、出力端子46,48間に得られる
電圧変化に対して出力端子46,48間の出力電
圧が低下することを利用して、出力電圧のスパン
調整を行う為の抵抗からなる。従つて、スパン調
整抵抗64の抵抗値を任意に変更することによつ
て、検出電圧を任意のレベルにスパン調整するこ
とが可能となる。第7図の実施例において、スパ
ン調整抵抗64はその一端が同一抵抗値の固定抵
抗60a,60bの接続点に接続されているの
で、零点調整時においては、スパン調整抵抗64
に電流が流れることなく、このことから、零点調
整時にはスパン調整抵抗64がなんら零点調整作
用に悪影響を与えることはない。 In other words, if the resistance value of the span adjustment resistor 64 is made small, the output voltage can be adjusted by utilizing the fact that the output voltage between the output terminals 46 and 48 decreases with respect to the voltage change obtained between the output terminals 46 and 48. Consists of resistance for span adjustment. Therefore, by arbitrarily changing the resistance value of the span adjustment resistor 64, it is possible to span-adjust the detected voltage to an arbitrary level. In the embodiment shown in FIG. 7, one end of the span adjustment resistor 64 is connected to the connection point of the fixed resistors 60a and 60b having the same resistance value, so during zero point adjustment, the span adjustment resistor 64
Therefore, during zero point adjustment, the span adjustment resistor 64 does not have any adverse effect on the zero point adjustment action.
以上説明したように、本発明によれば、フルブ
リツジ回路の抵抗素子に調整用の直列抵抗及び並
列抵抗を接続して零点調整及び零点移動温度補償
を行うブリツジ回路において、バイアス用並列抵
抗を予めブリツジ辺に任意の1辺に接続し、この
辺と隣接するブリツジ辺に接続される調整用の並
列抵抗の抵抗値を予め所望範囲の抵抗値に設定す
ることができ、調整用並列抵抗値を調整の容易な
値に選択することが可能となり、小型且つ微調整
容易なブリツジ回路を得ることが可能となる。 As explained above, according to the present invention, in a bridge circuit that performs zero point adjustment and zero point movement temperature compensation by connecting a series resistor and a parallel resistor for adjustment to a resistance element of a full bridge circuit, the bias parallel resistor is connected in advance to the bridge circuit. The resistance value of the parallel resistor for adjustment connected to any one side of the side and connected to this side and the adjacent bridge side can be set in advance to a resistance value within a desired range. It becomes possible to easily select a value, and it becomes possible to obtain a bridge circuit that is small and easy to finely adjust.
更に、本発明においては、抵抗値の小さい固定
抵抗と一般に入手しやすい標準的な抵抗値を有す
る可変抵抗の並列接続からなる零点微調整回路を
接続することによつて、零点調整を高精度に且つ
簡単な回路構成で得ることが可能となる利点を有
する。 Furthermore, in the present invention, zero point adjustment can be made with high precision by connecting a zero point fine adjustment circuit consisting of a parallel connection of a fixed resistor with a small resistance value and a variable resistor with a standard resistance value that is easily available. Moreover, it has the advantage that it can be obtained with a simple circuit configuration.
以上のように、本発明によれば、小型且つ高精
度なブリツジ回路を安価に提供することができ、
広範囲の測定器に適応し得るブリツジ回路を得る
ことが可能となる。 As described above, according to the present invention, a small and highly accurate bridge circuit can be provided at low cost.
It becomes possible to obtain a bridge circuit that can be applied to a wide range of measuring instruments.
第1図は従来の調整抵抗が付加されたブリツジ
回路を示す回路図、第2図は従来のブリツジ回路
を圧力変換器として用いた場合の温度特性図、第
3図は本発明にかかるブリツジ回路の好適な第1
実施例を示す回路図、第4図は第3図のブリツジ
回路を圧力変換器として構成した実施例を示す斜
視図、第5図は第4図の要部断面図、第6図は本
発明にかかるブリツジ回路の好適な第2実施例を
示す回路図、第7図は本発明にかかるブリツジ回
路の好適な第3実施例を示す回路図である。
10…ブリツジ回路、12,14,16,18
…抵抗素子、40,42…電源端子、44…電
源、46,48…出力端子、54…直列抵抗、5
6…バイアス用並列抵抗、58…調整用並列抵
抗、60…固定抵抗、62…可変抵抗、64…ス
パン調整抵抗。
Fig. 1 is a circuit diagram showing a conventional bridge circuit with an adjustment resistor added, Fig. 2 is a temperature characteristic diagram when the conventional bridge circuit is used as a pressure transducer, and Fig. 3 is a bridge circuit according to the present invention. preferred first
A circuit diagram showing an embodiment, FIG. 4 is a perspective view showing an embodiment in which the bridge circuit of FIG. 3 is configured as a pressure transducer, FIG. 5 is a sectional view of the main part of FIG. 4, and FIG. FIG. 7 is a circuit diagram showing a second preferred embodiment of the bridge circuit according to the present invention, and FIG. 7 is a circuit diagram showing a third preferred embodiment of the bridge circuit according to the present invention. 10... Bridge circuit, 12, 14, 16, 18
...Resistance element, 40, 42...Power supply terminal, 44...Power supply, 46, 48...Output terminal, 54...Series resistance, 5
6...Parallel resistance for bias, 58...Parallel resistance for adjustment, 60...Fixed resistance, 62...Variable resistance, 64...Span adjustment resistance.
Claims (1)
が変化する抵抗素子が接続され、相対する一対の
電源端子間に電源を接続し、他の一対の出力端子
から出力電圧を取出すブリツジ回路において、 前記ブリツジ回路の任意の1辺にその辺の抵抗
素子より十分に大きな抵抗値を有するバイアス用
並列抵抗を予め接続し、 このバイアス用並列抵抗の接続されたブリツジ
辺と隣接するブリツジ辺に調整用の並列抵抗を接
続し、 更に他のブリツジ辺に調整用の直列抵抗を接続
し、 前記バイアス用並列抵抗、調整用並列抵抗及び
直列抵抗を温度変化に対して実質的に抵抗変化を
生じない抵抗素子から形成し、 バイアス用並列抵抗を予め接続しておくことに
よつてその後に接続する調整用の並列抵抗値を前
記バイアス用並列抵抗と同程度の抵抗値範囲に設
定し、 調整用の直列抵抗及び並列抵抗によつてブリツ
ジ回路の零点調整及び零点移動温度補償を行うこ
とを特徴とするブリツジ回路。 2 特許請求の範囲1記載の装置において、ブリ
ツジ回路の一方の出力端子に固定抵抗と可変抵抗
との並列回路からなる零点微調整回路を接続し、
前記可変抵抗の中間端子からブリツジ出力を取り
出し、可変抵抗の調整によつて零点出力の微調整
を行うことを特徴とするブリツジ回路。 3 特許請求の範囲1,2のいずれかに記載の回
路において、ブリツジ回路の出力端子間にスパン
調整抵抗を接続したことを特徴とするブリツジ回
路。[Claims] 1. A resistance element whose resistance value changes according to a change in physical quantity is connected to each of the four sides, and a power supply is connected between a pair of opposing power supply terminals, and an output voltage is output from the other pair of output terminals. In the bridge circuit from which the output is taken out, a bias parallel resistor having a sufficiently larger resistance value than the resistance element on that side is connected in advance to any one side of the bridge circuit, and the bridge side adjacent to the bridge side to which this parallel bias resistor is connected is connected in advance. A parallel resistor for adjustment is connected to the side of the bridge that is to be adjusted, and a series resistor for adjustment is connected to the other bridge side, so that the bias parallel resistance, parallel adjustment resistance, and series resistance are substantially controlled against temperature changes. It is formed from a resistance element that does not cause a resistance change, and by connecting a bias parallel resistance in advance, the value of the adjustment parallel resistance connected afterwards is set to the same resistance value range as the bias parallel resistance. A bridge circuit characterized in that the zero point adjustment and zero point movement temperature compensation of the bridge circuit are performed using a series resistor and a parallel resistor for adjustment. 2. In the device according to claim 1, a zero point fine adjustment circuit consisting of a parallel circuit of a fixed resistor and a variable resistor is connected to one output terminal of the bridge circuit,
A bridge circuit characterized in that a bridge output is taken out from an intermediate terminal of the variable resistor, and the zero point output is finely adjusted by adjusting the variable resistor. 3. A bridge circuit according to claim 1 or 2, characterized in that a span adjustment resistor is connected between the output terminals of the bridge circuit.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4310880A JPS56140204A (en) | 1980-04-02 | 1980-04-02 | Bridge circuit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4310880A JPS56140204A (en) | 1980-04-02 | 1980-04-02 | Bridge circuit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56140204A JPS56140204A (en) | 1981-11-02 |
| JPH0248865B2 true JPH0248865B2 (en) | 1990-10-26 |
Family
ID=12654632
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4310880A Granted JPS56140204A (en) | 1980-04-02 | 1980-04-02 | Bridge circuit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56140204A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4927587B2 (en) * | 2007-02-16 | 2012-05-09 | マスプロ電工株式会社 | antenna |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS554846B2 (en) * | 1972-06-30 | 1980-02-01 |
-
1980
- 1980-04-02 JP JP4310880A patent/JPS56140204A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56140204A (en) | 1981-11-02 |
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