JPH044980Y2 - - Google Patents

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Publication number
JPH044980Y2
JPH044980Y2 JP1986064247U JP6424786U JPH044980Y2 JP H044980 Y2 JPH044980 Y2 JP H044980Y2 JP 1986064247 U JP1986064247 U JP 1986064247U JP 6424786 U JP6424786 U JP 6424786U JP H044980 Y2 JPH044980 Y2 JP H044980Y2
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JP
Japan
Prior art keywords
resistor
liquid
voltage
constant current
liquid level
Prior art date
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Expired
Application number
JP1986064247U
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Japanese (ja)
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JPS62176730U (en
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Priority to JP1986064247U priority Critical patent/JPH044980Y2/ja
Publication of JPS62176730U publication Critical patent/JPS62176730U/ja
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  • Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)

Description

【考案の詳細な説明】 〔産業上の利用分野〕 本考案は容器内に充填された液体に抵抗体を浸
漬させ、この抵抗体の抵抗値から液体の液面レベ
ルを測定する液面レベル測定装置に関するもので
ある。
[Detailed description of the invention] [Field of industrial application] The present invention is a liquid level measurement method in which a resistor is immersed in a liquid filled in a container, and the level of the liquid is measured from the resistance value of this resistor. It is related to the device.

〔従来の技術〕[Conventional technology]

従来の抵抗体による液面レベル測定装置は第3
図aに示す構成となつている。図において、容器
1には被測定物である液体2が液面レベルHまで
充填されている。この液体2に抵抗体R1を浸漬
し、これに定電流源I1により一定電流を供給す
る。抵抗体R1は定電流源I1によつて加熱され、抵
抗体R1から発生した熱は抵抗体R1の表面から周
囲に放熱される。このとき放熱度合は液体2の中
への放熱の方が、空気中への放熱に比して大き
い。抵抗体R1は一般に正の温度特性を有してい
る。従つて抵抗体R1が液体2中に浸漬している
部分は加熱による抵抗体の温度上昇が低く、抵抗
値が小さくなる。一方空気中に露出している部分
では温度上昇は大きく抵抗値は大きくなる。よつ
て抵抗値R1の液体2の中に浸漬している部分の
割合が大きくなる程抵抗体R1の全抵抗値は小さ
くなり、抵抗体R1には一定電流が供給されてい
るため、抵抗体R値の両端の端子電圧Vは低くな
る。即ち、第3図bに示すように、端子電圧Vは
液面レベルHの関数となる。そこでこの端子電圧
Vを測定することにより、液面レベルHを検出す
ることができる。
The conventional liquid level measuring device using a resistor is the third type.
The configuration is shown in Figure a. In the figure, a container 1 is filled with a liquid 2, which is an object to be measured, up to a liquid level H. A resistor R1 is immersed in this liquid 2, and a constant current is supplied to it by a constant current source I1 . The resistor R 1 is heated by the constant current source I 1 , and the heat generated from the resistor R 1 is radiated from the surface of the resistor R 1 to the surroundings. At this time, the degree of heat radiation is greater in the liquid 2 than in the air. Resistor R 1 generally has positive temperature characteristics. Therefore, in the portion where the resistor R1 is immersed in the liquid 2, the temperature rise of the resistor due to heating is low, and the resistance value becomes small. On the other hand, in parts exposed to the air, the temperature rise is large and the resistance value becomes large. Therefore, as the proportion of the portion immersed in the liquid 2 with the resistance value R 1 increases, the total resistance value of the resistor R 1 becomes smaller, and since a constant current is supplied to the resistor R 1 , The terminal voltage V across the resistor R value becomes low. That is, as shown in FIG. 3b, the terminal voltage V becomes a function of the liquid level H. Therefore, by measuring this terminal voltage V, the liquid level H can be detected.

〔考案が解決しようとする問題点〕[Problem that the invention attempts to solve]

しかしながら斯かる従来の装置にあつては、測
定感度を上げるためには、液体2の液面レベルH
の変化に対する抵抗体R1の端子電圧Vの変化を
大きくする必要がある。このため抵抗体R1はニ
ツケル等の抵抗温度係数の大なる金属を用いてい
る。ところが、このような抵抗体は液面レベルの
測定を行なう周囲の温度変化に対しても感度が良
くなり、この温度変化によつて抵抗値が変動して
しまい、液面レベルの測定精度が低下する。
However, in such a conventional device, in order to increase the measurement sensitivity, it is necessary to increase the liquid level H of the liquid 2.
It is necessary to increase the change in the terminal voltage V of the resistor R1 with respect to the change in . For this reason, the resistor R1 is made of a metal with a large resistance temperature coefficient, such as nickel. However, such resistors also become more sensitive to changes in the temperature around which the liquid level is being measured, and the resistance value fluctuates due to these temperature changes, reducing the accuracy of measuring the liquid level. do.

よつて本考案は、上述した従来の問題点に鑑
み、周囲温度の変化によつて液面レベルの測定値
が変動することがないようにした液面レベル測定
装置を提供することを目的としている。
Therefore, in view of the above-mentioned conventional problems, the present invention aims to provide a liquid level measuring device in which the measured value of the liquid level does not fluctuate due to changes in ambient temperature. .

〔問題点を解決するための手段〕[Means for solving problems]

上記目的と達成するため本考案により成された
液面レベル測定装置は、容器内の液体の液面レベ
ルに応じて液体に浸漬されている部分の割合が増
減する測定用の第1の抵抗体と、該第1の抵抗体
と同一形状・寸法、同一の温度特性及び抵抗値を
有し、常時空気中又は前記液体中に全体があるよ
うに配置された温度補償用の第2の抵抗体と、前
記第1の抵抗体にその上端から下端に向かつて一
定電流を流すと共に、前記第2の抵抗体に前記第
1の抵抗体に流す電流と同一の大きさの一定電流
を流す定電流源と、前記第1の抵抗体の両端に発
生する端子電圧と、前記第2の抵抗体の両端に発
生する端子電圧を前記第1の抵抗体の端子電圧よ
り常に小さい電圧又は大きい電圧になるように変
換した電圧との差をとり、液面レベルに応じて連
続的に変化する信号を出力する演算手段とを備え
ることを特徴としている。
In order to achieve the above object, the liquid level measuring device according to the present invention has a first resistor for measurement, which increases or decreases the proportion of the part immersed in the liquid depending on the level of the liquid in the container. and a second resistor for temperature compensation, which has the same shape, dimensions, same temperature characteristics, and resistance value as the first resistor, and is arranged so that the entire body is always in the air or in the liquid. and a constant current that causes a constant current to flow through the first resistor from its upper end to the lower end, and a constant current that has the same magnitude as the current that flows through the second resistor. source, a terminal voltage generated across the first resistor, and a terminal voltage generated across the second resistor to a voltage that is always smaller or larger than the terminal voltage of the first resistor. The present invention is characterized by comprising a calculation means that calculates the difference between the converted voltage and outputs a signal that continuously changes depending on the liquid level.

〔作用〕[Effect]

上記構成において、第1の抵抗体と第2の抵抗
体は同一形状・寸法、同一の温度特性及び抵抗値
を有し、かつこれらの抵抗体には定電流源により
同一の一定電流が流されているので、常時空気中
又は液体中に全体が配設されている温度補償用の
第2の抵抗体の端子電圧は、一定電流の通電よる
温度と周囲空気又は液体の温度とに依存する抵抗
値に対応したものとなるのに対し、液面レベルに
応じて液体に浸漬されている部分の割合が増減す
る測定用の第1の抵抗体の端子電圧は、一定電流
の通電よる温度と周囲空気及び液体の温度の他
に、液体に浸漬した分だけ放熱が進んだ状態での
温度又は液体に浸漬しない分だけ放熱が進んでい
ない状態での温度に依存した抵抗値に対応したも
のとなる。
In the above configuration, the first resistor and the second resistor have the same shape and dimensions, the same temperature characteristics, and the same resistance value, and the same constant current is passed through these resistors by the constant current source. Therefore, the terminal voltage of the second resistor for temperature compensation, which is completely disposed in air or liquid at all times, is a resistance that depends on the temperature due to constant current application and the temperature of the surrounding air or liquid. On the other hand, the terminal voltage of the first resistor for measurement, in which the proportion of the part immersed in the liquid increases or decreases depending on the liquid level, depends on the temperature and ambient temperature due to the application of a constant current. In addition to the temperature of the air and liquid, it corresponds to the resistance value that depends on the temperature when heat radiation has progressed by the amount of immersion in the liquid, or the temperature when heat radiation has not progressed by the amount not immersed in the liquid. .

従つて、演算回路が第1の抵抗体の端子電圧
と、第2の抵抗体の端子電圧を変換した電圧との
差をとつて出力する液体の液面レベルに応じた大
きさの信号は、温度変化による成分を含まない真
に液面レベルのみに応じて変化するものとなる。
Therefore, the signal that is output by the arithmetic circuit by calculating the difference between the terminal voltage of the first resistor and the voltage obtained by converting the terminal voltage of the second resistor, which corresponds to the level of the liquid, is as follows. It does not include components caused by temperature changes, and changes only according to the liquid level.

特に、第1の抵抗体と第2の抵抗体が同一形
状・寸法、同一の温度特性及び抵抗値を有し、か
つこれらに同一の一定電流を流すようにしている
ので、両抵抗体の端子電圧に基づいて簡単に周囲
温度の変動に対する補償を行うことができる。
In particular, since the first resistor and the second resistor have the same shape and dimensions, the same temperature characteristics, and the same resistance value, and the same constant current is passed through them, the terminals of both resistors are Compensation for ambient temperature fluctuations can be easily performed on the basis of voltage.

〔実施例〕〔Example〕

以下本考案の実施例を図と共に説明する。 Embodiments of the present invention will be described below with reference to the drawings.

第1図において、液体2には液面レベル測定用
抵抗体R1が浸漬され端子aより定電流I1が供給さ
れる。またこの抵抗体R1と同一形状・寸法の温
度補償用抵抗体R2が液体2の液面レベルに垂直
な面に対して抵抗体R1と対称位置に配置する。
この抵抗体R2は抵抗体R1と同一の正の温度特性
及び抵抗値を有し、定電流源I2から端子bを介し
て定電流源I1と同一電流値の定電流が供給されて
いる。また抵抗体R2は液体2に浸漬されずに常
時空気中に曝されている。第1図の構成において
は、抵抗体R1,R2を保護チユーブ3に装填し、
抵抗体R1の保護チユーブ3内には下面に孔を設
けて液体2を導入すると共に、抵抗体R2の保護
チユーブ3は下面を密閉して液体2が導入されな
いようにしている。尚、各抵抗体R1,R2の他方
の端子c,dは夫々接地される。抵抗体R1のa
点に得られる端子電圧V1は差動増幅器(演算回
路)OPの正相入力に供給され、抵抗体R2のb点
に得られる端子電圧V20は抵抗R3,R4により分圧
され、その分圧電圧V21が差動増幅器OPの逆相
入力に供給される。
In FIG. 1, a resistor R1 for measuring the liquid level is immersed in a liquid 2, and a constant current I1 is supplied from a terminal a. Further, a temperature compensating resistor R 2 having the same shape and dimensions as the resistor R 1 is arranged at a position symmetrical to the resistor R 1 with respect to a plane perpendicular to the level of the liquid 2 .
This resistor R2 has the same positive temperature characteristics and resistance value as the resistor R1 , and a constant current having the same current value as the constant current source I1 is supplied from the constant current source I2 through the terminal b. ing. Further, the resistor R 2 is not immersed in the liquid 2 but is constantly exposed to the air. In the configuration shown in FIG. 1, resistors R 1 and R 2 are loaded into the protective tube 3,
A hole is provided in the lower surface of the protective tube 3 of the resistor R 1 to introduce the liquid 2, and the lower surface of the protective tube 3 of the resistor R 2 is sealed to prevent the liquid 2 from being introduced. Note that the other terminals c and d of each resistor R 1 and R 2 are grounded, respectively. a of resistor R1
The terminal voltage V 1 obtained at point B is supplied to the positive phase input of the differential amplifier (arithmetic circuit) OP, and the terminal voltage V 20 obtained at point b of resistor R 2 is divided by resistors R 3 and R 4 . , the divided voltage V 21 is supplied to the negative phase input of the differential amplifier OP.

斯かる構成において、定電流が供給される測定
用抵抗体R1の各液面レベルH1,H2に対する端子
電圧は、第2図に示す液面レベル特性及び周囲温
度特性のようになる。つまり、周囲温度TがT1
からT2の如く上昇するに従つて端子電圧V1が大
きくなる。これは抵抗体R1の抵抗値が正の温度
特性を有し露出する部分の空気の温度、及び液体
2の温度により変化するためである。
In such a configuration, the terminal voltages of the measuring resistor R 1 to which a constant current is supplied for each liquid level H 1 and H 2 are as shown in the liquid level characteristics and ambient temperature characteristics shown in FIG. In other words, the ambient temperature T is T 1
As the voltage increases from T 2 to T 2 , the terminal voltage V 1 increases. This is because the resistance value of the resistor R 1 has a positive temperature characteristic and changes depending on the temperature of the air in the exposed portion and the temperature of the liquid 2 .

一方、常時空気中に配置している補償用の抵抗
体R2も抵抗体R1と同一の電流値の一定電流が供
給されており、しかも両者は同一形状・寸法の抵
抗体であるから、その端子電圧V20の周囲温度に
対する変化は、測定用抵抗体R1の液面レベルH
=0、即ち抵抗体R1が液体2に浸漬されていな
い場合の端子電圧V1と同一の温度変化となる。
つまり抵抗体R1,R2における周囲温度が同じで
あれば、同一の端子電圧となる。
On the other hand, the compensating resistor R2 , which is always placed in the air, is also supplied with a constant current of the same current value as the resistor R1 , and since both resistors have the same shape and dimensions, The change in the terminal voltage V20 with respect to the ambient temperature is the liquid level H of the measuring resistor R1 .
= 0, that is, the temperature change is the same as the terminal voltage V 1 when the resistor R 1 is not immersed in the liquid 2.
In other words, if the ambient temperatures at the resistors R 1 and R 2 are the same, the terminal voltages will be the same.

従つて、補償用抵抗体R2の端子電圧V20を抵抗
R3,R4で分圧した電圧V21が、常に測定用抵抗体
R1の端子電圧V1より低い値となるように設定す
れば、電圧V21は周囲温度にのみ依存する特性を
有しているから、差動増幅器OPにより端子電圧
V1と電圧V21との差をとれば、第2図に示すよう
に、その出力電圧V0は周囲温度には依存せずに、
液面レベルHに対してのみの関数となり温度補償
が図れる。よつて液面レベルHが一定であれば、
周囲温度が変化しても差動増幅器OPの出力電圧
V0は変化しないので、正確な液面レベルを測定
することができる。
Therefore, the terminal voltage V 20 of the compensation resistor R 2 is
The voltage V 21 divided by R 3 and R 4 is always applied to the measurement resistor.
If it is set to a value lower than the terminal voltage V 1 of R 1 , the voltage V 21 has a characteristic that depends only on the ambient temperature, so the terminal voltage will be reduced by the differential amplifier OP.
If we take the difference between V 1 and voltage V 21 , the output voltage V 0 is independent of the ambient temperature, as shown in Figure 2.
It becomes a function only for the liquid level H, and temperature compensation can be achieved. Therefore, if the liquid level H is constant,
Differential amplifier OP output voltage even when ambient temperature changes
Since V 0 does not change, it is possible to accurately measure the liquid level.

尚、上記実施例では温度補償用の抵抗体R2
常時空気中に露出するように構成したが、常時そ
の全体を液体2に浸漬するようにして温度補償用
の電圧を得るように構成してもよい。
In the above embodiment, the resistor R 2 for temperature compensation was constructed so as to be exposed in the air at all times, but it was constructed so that the entire resistor R 2 was always immersed in the liquid 2 to obtain the voltage for temperature compensation. You can.

また、電圧V21の設定として常に電圧V1より低
い値となるように設定したが電圧V1より常に高
い値となるように設定してもよい。
Further, although the voltage V 21 is set to always have a value lower than the voltage V 1 , it may be set to always have a value higher than the voltage V 1 .

更に、演算回路として、測定用抵抗体R1の端
子電圧V1を所定の基準レベルで反転させ、この
反転電圧と補償用抵抗体R2の端子電圧V20から得
られる補償用電圧V21とを加算するように構成し
てもよい。
Furthermore, as an arithmetic circuit, the terminal voltage V 1 of the measuring resistor R 1 is inverted at a predetermined reference level, and the compensation voltage V 21 obtained from this inverted voltage and the terminal voltage V 20 of the compensation resistor R 2 is calculated. It may be configured to add .

〔考案の効果〕[Effect of idea]

以上のように本考案によれば、被測定物である
液体の液面レベルを測定するに際して、周囲温度
の変化に影響を受けることがなく、液面レベルの
測定精度を向上させることができる。
As described above, according to the present invention, when measuring the liquid level of a liquid to be measured, it is possible to improve the accuracy of measuring the liquid level without being affected by changes in ambient temperature.

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

第1図は本考案に係る液面レベル測定装置の実
施例を示す図、第2図は第1図装置における検出
電圧及び抵抗体の端子電圧の液面レベル特性、及
び温度特性を示す図、第3図a,bは従来の液面
レベル測定装置、及びその検出電圧の液面レベル
特性をそれぞれ示す図である。 R1……液面レベル測定用抵抗体、R2……温度
補償用抵抗体、I1,I2……定電流源、OP……差動
増幅器、2……液体。
FIG. 1 is a diagram showing an embodiment of the liquid level measuring device according to the present invention, FIG. 2 is a diagram showing the liquid level characteristics and temperature characteristics of the detection voltage and terminal voltage of the resistor in the device shown in FIG. FIGS. 3a and 3b are diagrams showing a conventional liquid level measuring device and the liquid level characteristics of its detection voltage, respectively. R1 ...Resistor for liquid level measurement, R2 ...Resistor for temperature compensation, I1 , I2 ...Constant current source, OP...Differential amplifier, 2...Liquid.

Claims (1)

【実用新案登録請求の範囲】 容器内の液体の液面レベルに応じて液体に浸漬
されている部分の割合が増減する測定用の第1の
抵抗体と、 該第1の抵抗体と同一形状・寸法、同一の温度
特性及び抵抗値を有し、常時空気中又は前記液体
中に全体があるように配置された温度補償用の第
2の抵抗体と、 前記第1の抵抗体にその上端から下端に向かつ
て一定電流を流すと共に、前記第2の抵抗体に前
記第1の抵抗体に流す電流と同一の大きさの一定
電流を流す定電流源と、 前記第1の抵抗体の両端に発生する端子電圧
と、前記第2の抵抗体の両端に発生する端子電圧
を前記第1の抵抗体の端子電圧より常に小さい電
圧又は大きい電圧になるように変換した電圧との
差をとり、液面レベルに応じて連続的に変化する
信号を出力する演算手段とを備える ことを特徴とする液面レベル測定装置。
[Claims for Utility Model Registration] A first resistor for measurement whose proportion of the portion immersed in the liquid increases or decreases depending on the level of the liquid in the container, and a shape identical to the first resistor. - A second resistor for temperature compensation, which has the same dimensions, the same temperature characteristics, and the same resistance value, and is arranged so that the entire body is always in the air or in the liquid, and its upper end is connected to the first resistor. a constant current source that flows a constant current from the to the lower end toward the lower end, and that flows a constant current that is the same magnitude as the current that flows through the first resistor through the second resistor, and both ends of the first resistor. and a voltage obtained by converting the terminal voltage generated across the second resistor to a voltage that is always smaller or larger than the terminal voltage of the first resistor, 1. A liquid level measuring device comprising: arithmetic means for outputting a signal that continuously changes according to the liquid level.
JP1986064247U 1986-04-30 1986-04-30 Expired JPH044980Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1986064247U JPH044980Y2 (en) 1986-04-30 1986-04-30

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1986064247U JPH044980Y2 (en) 1986-04-30 1986-04-30

Publications (2)

Publication Number Publication Date
JPS62176730U JPS62176730U (en) 1987-11-10
JPH044980Y2 true JPH044980Y2 (en) 1992-02-13

Family

ID=30900231

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1986064247U Expired JPH044980Y2 (en) 1986-04-30 1986-04-30

Country Status (1)

Country Link
JP (1) JPH044980Y2 (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE2841889B2 (en) * 1978-09-26 1980-09-25 Siemens Ag, 1000 Berlin Und 8000 Muenchen Device for continuous measurement of the filling level in a container at least partially filled with liquid
JPS5774622A (en) * 1980-10-29 1982-05-10 Mitsubishi Atom Power Ind Inc High temperature liquid level meter

Also Published As

Publication number Publication date
JPS62176730U (en) 1987-11-10

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