JPH0814971A - Electromagnetic flowmeter - Google Patents

Electromagnetic flowmeter

Info

Publication number
JPH0814971A
JPH0814971A JP15370194A JP15370194A JPH0814971A JP H0814971 A JPH0814971 A JP H0814971A JP 15370194 A JP15370194 A JP 15370194A JP 15370194 A JP15370194 A JP 15370194A JP H0814971 A JPH0814971 A JP H0814971A
Authority
JP
Japan
Prior art keywords
electromotive force
inter
fluid
signal electromotive
coil
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP15370194A
Other languages
Japanese (ja)
Inventor
Ichiro Mitsutake
一郎 光武
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Azbil Corp
Original Assignee
Azbil Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Azbil Corp filed Critical Azbil Corp
Priority to JP15370194A priority Critical patent/JPH0814971A/en
Publication of JPH0814971A publication Critical patent/JPH0814971A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To accurately measure the flow rate of a fluid regardless of the temperature change of the fluid by finding a measurement error at a predetermined flow rate from storage tables respectively indicating the relations between previously measured inter-coil voltages and the temperature of the fluid and between the temperature of the fluid and measurement errors. CONSTITUTION:A first storage table indicating the relation between the inter-coil voltage of an exciting coil 2 and the temperature of a fluid to be measured and second storage table indicating the relation between the temperature of the fluid when the flow rate of the fluid is 100% and measurement errors of signal electromotive forces are prepared from measured results and stored in an EEPROM 12. An electromotive force detecting circuit 6 detects the signal electromotive force between electrodes 4a and 4b and a CPU 9 finds measured values based on the electromotive force. At the time of finding the electromotive force, the CPU 9 fetches the inter-coil voltage of the coil 2 and reads out the fluid temperature corresponding to the voltage from the first storage table in the ROM 12 and the measurement error when the flow rate is 100% at the fluid temperature from the second storage table. Then the CPU 9 finds the measured flow rate value of the fluid which is not affected by the temperature change of the fluid by calculating and eliminating the measurement error contained in the signal electromotive force based on the read-out measurement error.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は、各種プロセス系にお
いて導電性を有する流体の流量を測定する電磁流量計に
関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electromagnetic flow meter for measuring the flow rate of electrically conductive fluid in various process systems.

【0002】[0002]

【従来の技術】従来より、この種の電磁流量計において
は、測定管内を流れる流体の流れ方向に対してその磁界
の発生方向を垂直として配置された励磁コイルへ所定周
波数で励磁電流を供給し、励磁コイルの発生磁界と直交
して測定管内に配置された電極間に得られる信号起電力
(流量に比例した信号)を検出し、この検出した信号起
電力に基づいてCPUでの演算処理により計測値を求め
ている。すなわち、励磁コイルへ励磁電流を周期的に供
給し、測定管内に交流磁界を発生させる。これにより、
測定管内に配置された電極間に、流速と磁界との相互作
用により信号起電力が生じる。この信号起電力を信号起
電力検出回路により検出する。そして、この検出される
信号起電力を、周期的に励磁電流の供給が遮断される直
前で保持(サンプリング)し、A/D変換器を介してC
PUへ与える。CPUは、この供与される信号起電力に
基づいて計測値を測定レンジの0〜100%値として求
め、この求めた計測値に応じて出力電流を4〜20mA
の電流範囲で調整する。
2. Description of the Related Art Conventionally, in this type of electromagnetic flowmeter, an exciting current is supplied at a predetermined frequency to an exciting coil arranged such that a magnetic field is generated in a direction perpendicular to a flow direction of a fluid flowing in a measuring tube. , The signal electromotive force (a signal proportional to the flow rate) obtained between the electrodes arranged in the measuring tube at right angles to the magnetic field generated by the exciting coil is detected, and based on the detected signal electromotive force, the CPU performs arithmetic processing. Seeking the measured value. That is, an exciting current is periodically supplied to the exciting coil to generate an alternating magnetic field in the measuring tube. This allows
A signal electromotive force is generated between the electrodes arranged in the measuring tube due to the interaction between the flow velocity and the magnetic field. This signal electromotive force is detected by the signal electromotive force detection circuit. Then, the detected signal electromotive force is held (sampled) immediately before the supply of the exciting current is interrupted periodically, and the signal electromotive force is converted to C via the A / D converter.
Give to PU. The CPU obtains a measured value as a 0-100% value of the measurement range based on the supplied signal electromotive force, and outputs an output current of 4-20 mA according to the obtained measured value.
Adjust within the current range of.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、このよ
うな電磁流量計においては、流体温度が変化すると、励
磁コイルの抵抗値が変わり、励磁波形が変化する。例え
ば、流体温度が20℃である場合の励磁波形が図4
(a)に実線で示すような波形であったとすると、流体
温度が160℃へ変化することによって破線で示すよう
な励磁波形となる。このため、得られる信号起電力も図
4(b)に実線で示すような波形から破線で示すような
波形へ変化し、信号起電力のサンプリング値e20とe
160 との間に差が生じ、この差Δeが計測値に含まれる
誤差成分となる。すなわち、従来においては、流体温度
の変化が、正確な流量測定を阻害していた。
However, in such an electromagnetic flowmeter, when the fluid temperature changes, the resistance value of the exciting coil changes and the exciting waveform changes. For example, the excitation waveform when the fluid temperature is 20 ° C. is shown in FIG.
If the waveform is as shown by the solid line in (a), the excitation waveform will be as shown by the broken line as the fluid temperature changes to 160 ° C. Therefore, the obtained signal electromotive force also changes from the waveform shown by the solid line in FIG. 4B to the waveform shown by the broken line, and the sampling values e 20 and e of the signal electromotive force are changed.
The difference Δe is 160, and this difference Δe becomes an error component included in the measured value. That is, in the past, changes in fluid temperature hindered accurate flow rate measurement.

【0004】本発明はこのような課題を解決するために
なされたもので、その目的とするところは、流体温度の
変化とは無関係に、正確に流量測定を行うことの可能な
電磁流量計を提供することにある。
The present invention has been made to solve the above problems, and an object of the present invention is to provide an electromagnetic flow meter capable of accurately measuring a flow rate regardless of changes in fluid temperature. To provide.

【0005】[0005]

【課題を解決するための手段】このような目的を達成す
るために、その第1発明(請求項1に係る発明)は、上
述した電磁流量計において、励磁コイルのコイル間電圧
を検出するものとし、この検出されるコイル間電圧に基
づいて、流体温度の変化により生じる誤差成分を計測値
から除去するようにしたものである。また、その第2発
明(請求項2に係る発明)は、上述した電磁流量計にお
いて、励磁コイルのコイル間電圧を検出するものとし、
この検出されるコイル間電圧より、第1の記憶テーブル
(コイル間電圧と流体温度との関係を示す記憶テーブ
ル)を参照として流体の温度を求め、この求めた流体温
度より、第2の記憶テーブル(所定流量時における流体
温度と計測誤差との関係を示す記憶テーブル)を参照と
して、その流体温度における所定流量時の計測誤差を求
め、この求めた計測誤差に基づいて流体温度の変化によ
り生じる誤差成分を計測値から除去するようにしたもの
である。また、その第3発明(請求項3に係る発明)
は、上述した電磁流量計において、所定流量時における
第1および第2の流体温度での信号起電力ならびにコイ
ル間電圧を実測して得た定数を記憶しておくものとし、
また励磁コイルのコイル間電圧を検出するものとし、コ
イル間電圧および信号起電力の検出値と記憶されている
定数とから、流体温度の変化により生じる誤差成分の除
去された信号起電力を算出するようにしたものである。
In order to achieve such an object, a first invention thereof (an invention according to claim 1) is to detect the inter-coil voltage of an exciting coil in the electromagnetic flowmeter described above. Then, based on the detected inter-coil voltage, an error component caused by a change in fluid temperature is removed from the measured value. A second invention (an invention according to claim 2) of the electromagnetic flowmeter described above is to detect a voltage between coils of an exciting coil,
From the detected inter-coil voltage, the temperature of the fluid is obtained with reference to the first storage table (the storage table indicating the relationship between the inter-coil voltage and the fluid temperature), and the second storage table is obtained from the obtained fluid temperature. An error caused by a change in the fluid temperature based on the calculated measurement error at the predetermined flow rate at that fluid temperature with reference to (a memory table indicating the relationship between the fluid temperature and the measurement error at the predetermined flow rate) The component is removed from the measured value. The third invention (the invention of claim 3)
In the electromagnetic flowmeter described above, the constants obtained by actually measuring the signal electromotive force and the inter-coil voltage at the first and second fluid temperatures at a predetermined flow rate are stored,
Further, the voltage between the coils of the exciting coil is detected, and the signal electromotive force from which the error component caused by the change in the fluid temperature is removed is calculated from the detected value of the voltage between the coils and the signal electromotive force and the stored constant. It was done like this.

【0006】[0006]

【作用】したがってこの発明によれば、その第1発明で
は、励磁コイルのコイル間電圧に基づいて、すなわち流
体温度の変化を反映するコイル間電圧に基づいて、流体
温度の変化により生じる誤差成分が計測値から除去され
る。また、その第2発明では、励磁コイルのコイル間電
圧より第1の記憶テーブルを参照として流体の温度が求
められ、この求められた流体温度より第2の記憶テーブ
ルを参照としてその流体温度における所定流量時の計測
誤差が求められ、この求められた計測誤差に基づいて流
体温度の変化により生じる誤差成分が計測値から除去さ
れる。また、その第3発明では、コイル間電圧および信
号起電力の検出値と記憶されている定数とから、流体温
度の変化により生じる誤差成分の除去された信号起電力
が算出され、この結果として流体温度の変化により生じ
る誤差成分が計測値から除去される。
Therefore, according to the first aspect of the present invention, the error component caused by the change in the fluid temperature is generated based on the inter-coil voltage of the exciting coil, that is, the inter-coil voltage that reflects the change in the fluid temperature. Removed from measurement. In the second aspect of the invention, the temperature of the fluid is obtained from the inter-coil voltage of the exciting coil with reference to the first storage table, and the predetermined fluid temperature is obtained with reference to the second storage table from the obtained fluid temperature. The measurement error at the time of the flow rate is obtained, and the error component caused by the change of the fluid temperature is removed from the measurement value based on the obtained measurement error. In the third aspect of the invention, the signal electromotive force from which the error component caused by the change in fluid temperature is removed is calculated from the detected values of the inter-coil voltage and the signal electromotive force and the stored constants, and as a result, the fluid electromotive force is calculated. The error component caused by the temperature change is removed from the measured value.

【0007】[0007]

【実施例】【Example】

〔実施例1〕以下、本発明を実施例に基づき詳細に説明
する。図1はこの発明の一実施例を示す電磁流量計の要
部を示すブロック回路構成図である。同図において、1
は測定管、2は測定管1内を流れる流体の流れ方向に対
してその磁界の発生方向を垂直として配置された励磁コ
イル、3は励磁コイル2へ矩形波状の励磁電流IEXを周
期的に供給する励磁回路、4a,4bは励磁コイル2の
発生磁界と直交して測定管1内に配置された検出電極、
5は接地電極、6は電極4a,4b間に得られる信号起
電力を検出する信号起電力検出回路、7はこの信号起電
力検出回路6の検出する信号起電力をサンプルホールド
するサンプルホールド回路、8はA/D変換器、9はC
PU、10はD/A変換器、11は励磁コイル2のコイ
ル間電圧を検出しこの検出電圧をディジタル値に変換し
てCPU9へ与えるA/D変換器、12はEEPROM
である。
Example 1 The present invention will be described in detail below based on examples. FIG. 1 is a block circuit configuration diagram showing a main part of an electromagnetic flowmeter showing an embodiment of the present invention. In the figure, 1
Is a measuring tube, 2 is an exciting coil arranged such that the direction of its magnetic field is perpendicular to the flow direction of the fluid flowing in the measuring tube 3, and 3 is a rectangular wave exciting current I EX to the exciting coil 2 periodically. The exciting circuits 4a and 4b to be supplied are detection electrodes arranged in the measuring tube 1 at right angles to the magnetic field generated by the exciting coil 2.
Reference numeral 5 is a ground electrode, 6 is a signal electromotive force detection circuit that detects a signal electromotive force obtained between the electrodes 4a and 4b, 7 is a sample hold circuit that samples and holds the signal electromotive force detected by the signal electromotive force detection circuit 6, 8 is an A / D converter, 9 is C
PU, 10 is a D / A converter, 11 is an A / D converter for detecting the voltage between the coils of the exciting coil 2 and converting the detected voltage to a digital value and giving it to the CPU 9, 12 is an EEPROM
Is.

【0008】この電磁流量計100はケーブルL1,L
2を介して直流電源(D.C.24V)200と接続されて
いる。励磁回路3は励磁電圧回路3−1と定電流回路3
−2とを備えてなる。定電流回路3−2にはCPU9か
らの指令によりそのスイッチング動作が制御される励磁
電流スイッチング回路が含まれている。EEPROM1
2には、励磁コイル2のコイル間電圧と測定すべき流体
の温度との関係を示す第1の記憶テーブル(図2(a)
参照)、および、100%流量時における流体温度と信
号起電力の計測誤差との関係を示す第2の記憶テーブル
(図2(b)参照)が格納されている。これらの記憶テ
ーブルは実測結果に基づいて予め求められたものであ
る。
This electromagnetic flowmeter 100 has cables L1 and L.
It is connected to the DC power supply (DC 24V) 200 via the line 2. The excitation circuit 3 includes an excitation voltage circuit 3-1 and a constant current circuit 3
-2 and. The constant current circuit 3-2 includes an exciting current switching circuit whose switching operation is controlled by a command from the CPU 9. EEPROM 1
2 shows a first storage table (FIG. 2A) showing the relationship between the inter-coil voltage of the exciting coil 2 and the temperature of the fluid to be measured.
2) and a second storage table (see FIG. 2B) showing the relationship between the fluid temperature and the measurement error of the signal electromotive force at a flow rate of 100%. These storage tables are obtained in advance based on actual measurement results.

【0009】この電磁流量計100において、励磁回路
3は、励磁コイル2へ励磁電流IEX(4mA)を周期的
に供給し、測定管1内に交流磁界を発生させる。これに
より、電極4a,4b間に流速と磁界との相互作用によ
り信号起電力が生じ、これが信号起電力検出回路6によ
り検出される。この検出される信号起電力は、周期的に
励磁電流の供給が中断される直前でサンプルホールド回
路7にて保持され、この保持された信号起電力がA/D
変換器8へ与えられディジタル値に変換されて、CPU
9に取り込まれる。CPU9は、このA/D変換器8か
らの信号起電力に基づき計測値を測定レンジの0〜10
0%値として求め、この求めた計測値をD/A変換器1
0へ与え、ケーブルL1,L2に流れる電流Iout を、
上記求めた計測値に応じて4〜20mAの電流範囲で調
整する
In this electromagnetic flowmeter 100, the exciting circuit 3 periodically supplies an exciting current I EX (4 mA) to the exciting coil 2 to generate an alternating magnetic field in the measuring tube 1. As a result, a signal electromotive force is generated between the electrodes 4a and 4b due to the interaction between the flow velocity and the magnetic field, and this is detected by the signal electromotive force detection circuit 6. The detected signal electromotive force is held in the sample hold circuit 7 immediately before the supply of the exciting current is interrupted periodically, and the held signal electromotive force is A / D.
It is given to the converter 8 and converted into a digital value, and the CPU
Taken in 9. The CPU 9 measures the measured value based on the signal electromotive force from the A / D converter 8 in the measurement range of 0 to 10
Obtained as 0% value, and the obtained measured value is D / A converter 1
0, and the current I out flowing through the cables L1 and L2 is
Adjust in the current range of 4 to 20 mA according to the measured value obtained above.

【0010】ここで、CPU9は、信号起電力に基づい
て計測値を求めるに際し、次のようにして温度補正を行
う。すなわち、CPU9は、周期的に励磁電流IEXの供
給が中断される直前の励磁コイル2のコイル間電圧Ex
をA/D変換器11を介して取り込む。そして、この取
り込んだコイル間電圧Ex に対応する流体温度Tx を、
EEPROM12に格納されている第1の記憶テーブル
から読み出す。そして、この読み出した流体温度Tx
の100%流量時における計測誤差Nx(100)を、EEP
ROM12に格納されている第2の記憶テーブルから読
み出す。そして、この読み出した計測誤差Nx(100)に基
づき、信号起電力の検出値ex(y)に含まれている計測誤
差Nx(y)を算出し、この計測誤差Nx(y)を検出値ex(y)
から除去する。そして、この計測誤差Nx(y)の除去され
た信号起電力ex(y)’より、流体温度の変化により生じ
る誤差成分の除去された値として計測値Qx(y)’を求め
る。これにより、流体温度の変化とは無関係に、正確に
流量測定を行うことができる。
Here, when the CPU 9 obtains the measured value based on the signal electromotive force, the temperature is corrected as follows. That is, the CPU 9 causes the inter-coil voltage E x of the exciting coil 2 immediately before the supply of the exciting current I EX is periodically interrupted.
Are taken in via the A / D converter 11. Then, the fluid temperature T x corresponding to the captured inter-coil voltage E x is
The data is read from the first storage table stored in the EEPROM 12. Then, the measurement error N x (100) at the time of 100% flow rate at the read fluid temperature T x is calculated as EEP
It is read from the second storage table stored in the ROM 12. On the basis of the read measurement error N x (100), calculates the signal electromotive force detection value e x (y) in the included measurement error N x (y), the measurement error N x (y) Detected value e x (y)
To remove from. Then, from the signal electromotive force ex (y) 'from which this measurement error Nx (y) has been removed, a measurement value Qx (y) ' is obtained as a value from which an error component caused by a change in fluid temperature has been removed. Thereby, the flow rate can be accurately measured regardless of the change in the fluid temperature.

【0011】〔実施例2〕なお、上述した実施例では、
EEPROM12に格納した記憶テーブルを参照として
信号起電力ex(y)’を得るようにしたが、下記(1)式
に示すような計算式を用いるようにしてもよい。すなわ
ち、この計算式を用いれば、コイル間電圧Ex および信
号起電力の検出値ex(y)を代入するのみで、流体温度の
変化により生じる誤差成分の除去された信号起電力e
x(y)’を得ることができる。これにより、実施例1で用
いたような記憶テーブルが不要となり、メモリ容量を節
約することができる。
[Embodiment 2] In the embodiment described above,
Although the signal electromotive force ex (y) 'is obtained by referring to the storage table stored in the EEPROM 12, a calculation formula as shown in the following formula (1) may be used. That is, if this calculation formula is used, the signal electromotive force e from which the error component caused by the change of the fluid temperature has been removed is simply substituted by the inter-coil voltage E x and the detected value e x (y) of the signal electromotive force.
You can get x (y) '. As a result, the storage table used in the first embodiment becomes unnecessary, and the memory capacity can be saved.

【0012】 ex(y)’=A・ex(y)/(A+Ex ・B) ・・・(1) なお、この(1)式において、AおよびBは、A=(E
160 −E25)・e25(1 00)、B=e160(100)−e25(100)
で表される定数である。ここで、E25は流体温度が25
℃の時のコイル間電圧の実測値、E160 は流体温度が1
60℃の時のコイル間電圧の実測値、e25(100)は流体
温度25℃での100%流量時の信号起電力の実測値、
160(100)は流体温度160℃での100%流量時の信
号起電力の実測値である。すなわち、上記定数Aおよび
Bは、E25,E160 ,e25(100)およびe160(100)を実
測して得た定数であり、これらの定数はEEPROM1
2に記憶させておく。
Ex (y) '= A · ex (y) / (A + Ex · B) (1) In this equation (1), A and B are A = (E
160 -E 25) · e 25 ( 1 00), B = e 160 (100) -e 25 (100)
Is a constant represented by. Here, E 25 has a fluid temperature of 25
Actual measured value of coil voltage at ℃, E 160 is fluid temperature 1
The measured value of the voltage between the coils at 60 ° C., e 25 (100) is the measured value of the signal electromotive force at a fluid temperature of 25 ° C. and a 100% flow rate,
e 160 (100) is a measured value of the signal electromotive force at a fluid temperature of 160 ° C. and a flow rate of 100%. That is, the constants A and B are constants obtained by actually measuring E 25 , E 160 , e 25 (100) and e 160 (100) , and these constants are the EEPROM 1
Remember in 2.

【0013】上記(1)式は次のようにして導き出した
ものである。今、流体温度がx℃であり、信号起電力が
x(y)として得られたとする(図3参照)。この信号起
電力ex(y)には流体温度の変化により生じる誤差成分が
含まれている。この誤差成分の除去された信号起電力を
x(y)’とする。ここで、流体温度がx℃の100%流
量時の信号起電力をex(100)とすれば、この信号起電力
x(100)は下記(2)式により表される。 ex(100)=e25(100)+(e160(100)−e25(100))・Ex /(E160 −E25) ・・・(2)
The above equation (1) is derived as follows. Now, assume that the fluid temperature is x ° C. and the signal electromotive force is obtained as e x (y) (see FIG. 3). This signal electromotive force ex (y) contains an error component caused by a change in fluid temperature. The signal electromotive force from which this error component is removed is defined as e x (y) '. Here, if the signal electromotive force at a 100% flow rate at a fluid temperature of x ° C. is ex (100) , this signal electromotive force ex (100) is expressed by the following equation (2). e x (100) = e 25 (100) + (e 160 (100) -e 25 (100)) · E x / (E 160 -E 25) ··· (2)

【0014】また、求めるべき信号起電力ex(y)’は、
下記(3)式により表される。 ex(y)’=ex(y)−(ex(100)−e25(100))・ex(y)/ex(100) ・・・( 3) この(3)式を変形すると、 ex(y)−ex(y)’=(ex(100)−e25(100))・ex(y)/ex(100)=(ex(100 ) ・ex(y)−e25(100)・ex(y))/ex(100)=ex(y)−e25(100)・ex(y)/ex (100) となり、 ex(y)’=e25(100)・ex(y)/ex(100) ・・・(4) となる。
The signal electromotive force e x (y) 'to be obtained is
It is expressed by the following equation (3). ex (y) '= ex (y) -(ex (100) -e25 (100) ). ex (y) / ex (100) ... (3) When transformed, ext (y) -ex (y) '= (ex (100) -e25 (100) ). Ex (y) / ex (100) = (ex (100 ) .e x (y) −e 25 (100) · ex x (y) ) / ex x (100) = ex x (y) −e 25 (100) · ex x (y) / ex x (100) , and e x (y) '= e25 (100) * ex (y) / ex (100) ... (4).

【0015】この(4)式のex(100)に(2)式を代入
すると、 ex(y)’=(E160 −E25)・e25(100)・ex(y)/{(E160 −E25)・e2 5(100) +Ex ・(e160(100)−e25(100))} ・・・(5) となり、A=(E160 −E25)・e25(100)、B=e
160(100)−e25(100)とすれば、上記(1)式が得られ
る。この(1)式の導出は、流体温度がx℃である場合
の100%流量時の信号起電力ex(100)に含まれる計測
誤差を求め、100%流量時の信号起電力ex(100)と信
号起電力の検出値ex(y)との比からその検出値ex(y)
含まれる計測誤差を求め、この求めた計測誤差を検出値
x(y)から除去してやろうという考えに基づいている。
Substituting the equation (2) into the equation (4), e x (100) , e x (y) '= (E 160 -E 25 ) · e 25 (100) · e x (y) / {(E 160 -E 25) · e 2 5 (100) + E x · (e 160 (100) -e 25 (100))} ··· (5) next, A = (E 160 -E 25 ) · e 25 (100) , B = e
If 160 (100) −e 25 (100) , the above formula (1) can be obtained. The equation (1) is derived by obtaining the measurement error included in the signal electromotive force e x (100) at 100% flow rate when the fluid temperature is x ° C., and calculating the signal electromotive force e x ( at 100% flow rate e x ( 100) and the detected value e x (y) of the signal electromotive force, the measurement error included in the detected value e x (y) is obtained, and the obtained measurement error is removed from the detected value e x (y). It is based on the idea of deafening.

【0016】なお、上述した実施例1,2では、信号起
電力ex(y)から流体温度の変化により生じる誤差成分を
除去することによって、結果的に計測値Qx(y)に含まれ
る流体温度の変化により生じる誤差成分を排除するもの
としたが、計測値Qx(y)より直接その誤差成分を除去す
るものとしてもよい。すなわち、実施例1では第2の記
憶テーブルに格納する計測誤差を計測値の計測誤差とす
ることにより、また実施例2では信号起電力ex を計測
値Qx に置き換えて考えることにより、計測値Qx(y)
り直接その誤差成分を除去することが可能となる。
In the first and second embodiments described above, the error component generated due to the change in the fluid temperature is removed from the signal electromotive force e x (y), so that the result is included in the measured value Q x (y). Although the error component caused by the change in the fluid temperature is eliminated, the error component may be directly removed from the measured value Q x (y) . That is, in the first embodiment, the measurement error stored in the second storage table is used as the measurement error of the measurement value, and in the second embodiment, the signal electromotive force e x is replaced with the measurement value Q x for consideration. It is possible to directly remove the error component from the value Q x (y) .

【0017】[0017]

【発明の効果】以上説明したことから明らかなように本
発明によれば、その第1発明では、励磁コイルのコイル
間電圧に基づいて、すなわち流体温度の変化を反映する
コイル間電圧に基づいて、流体温度の変化により生じる
誤差成分が計測値から除去されるものとなり、またその
第2発明では、励磁コイルのコイル間電圧より第1の記
憶テーブルを参照として流体の温度が求められ、この求
められた流体温度より第2の記憶テーブルを参照として
その流体温度における所定流量時の計測誤差が求めら
れ、この求められた計測誤差に基づいて流体温度の変化
により生じる誤差成分が計測値から除去されるものとな
り、またその第3発明では、コイル間電圧および信号起
電力の検出値と記憶されている定数とから、流体温度の
変化により生じる誤差成分の除去された信号起電力が算
出され、この結果として流体温度の変化により生じる誤
差成分が計測値から除去されるものとなり、流体温度の
変化とは無関係に、正確に流量測定を行うことが可能と
なる。
As is apparent from the above description, according to the present invention, in the first invention, it is based on the inter-coil voltage of the exciting coil, that is, based on the inter-coil voltage reflecting the change in fluid temperature. , The error component caused by the change of the fluid temperature is removed from the measured value, and in the second invention, the temperature of the fluid is obtained by referring to the first memory table from the inter-coil voltage of the exciting coil. A measurement error at a predetermined flow rate at the fluid temperature is obtained from the obtained fluid temperature with reference to the second storage table, and an error component caused by a change in the fluid temperature is removed from the measurement value based on the obtained measurement error. In the third aspect of the invention, the error caused by the change in fluid temperature is detected from the detected values of the voltage between the coils and the signal electromotive force and the stored constants. The signal electromotive force with the component removed is calculated, and as a result, the error component caused by the change in fluid temperature is removed from the measured value, and accurate flow rate measurement can be performed regardless of the change in fluid temperature. It will be possible.

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

【図1】 本発明の一実施例を示す電磁流量計の要部を
示すブロック回路構成図である。
FIG. 1 is a block circuit configuration diagram showing a main part of an electromagnetic flow meter showing an embodiment of the present invention.

【図2】 この電磁流量計のEEPROMに格納された
第1および第2の記憶テーブルを例示する図である。
FIG. 2 is a diagram exemplifying first and second storage tables stored in an EEPROM of this electromagnetic flow meter.

【図3】 (1)式の導出過程の説明に用いる信号起電
力の波形を例示する図である。
FIG. 3 is a diagram exemplifying a waveform of a signal electromotive force used for explaining a derivation process of equation (1).

【図4】 流体温度の変化により生じる励磁波形および
信号起電力の波形の変化を例示する図である。
FIG. 4 is a diagram illustrating changes in an excitation waveform and a signal electromotive force waveform caused by a change in fluid temperature.

【符号の説明】[Explanation of symbols]

1…測定管、2…励磁コイル、3…励磁回路、4a,4
b…検出電極、5…接地電極、6…信号起電力検出回
路、7…サンプルホールド回路、8…A/D変換器、9
…CPU、10…D/A変換器、11…A/D変換器、
12…EEPROM。
1 ... Measuring tube, 2 ... Excitation coil, 3 ... Excitation circuit, 4a, 4
b ... Detection electrode, 5 ... Ground electrode, 6 ... Signal electromotive force detection circuit, 7 ... Sample hold circuit, 8 ... A / D converter, 9
... CPU, 10 ... D / A converter, 11 ... A / D converter,
12 ... EEPROM.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 測定管内を流れる流体の流れ方向に対し
てその磁界の発生方向を垂直として配置された励磁コイ
ルへ所定周波数で励磁電流を供給する励磁電流供給手段
と、前記励磁コイルの発生磁界と直交して前記測定管内
に配置された電極間に得られる信号起電力を検出する信
号起電力検出手段と、この信号起電力検出手段の検出す
る信号起電力に基づいて計測値を求める計測値演算手段
とを備えた電磁流量計において、 前記励磁コイルのコイル間電圧を検出するコイル間電圧
検出手段と、 このコイル間電圧検出手段の検出するコイル間電圧に基
づいて前記計測値演算手段により求められる計測値から
流体温度の変化により生じる誤差成分を除去する温度補
正手段とを備えたことを特徴とする電磁流量計。
1. Exciting current supplying means for supplying an exciting current at a predetermined frequency to an exciting coil arranged such that a magnetic field is generated in a direction perpendicular to a flow direction of a fluid flowing in a measuring tube, and a magnetic field generated by the exciting coil. A signal electromotive force detecting means for detecting a signal electromotive force obtained between electrodes arranged in the measuring tube orthogonally to the measurement tube, and a measured value for obtaining a measured value based on the signal electromotive force detected by the signal electromotive force detecting means. In an electromagnetic flowmeter provided with a calculating means, an inter-coil voltage detecting means for detecting the inter-coil voltage of the exciting coil, and the measured value calculating means based on the inter-coil voltage detected by the inter-coil voltage detecting means An electromagnetic flowmeter, comprising: a temperature correction unit that removes an error component caused by a change in fluid temperature from the measured value.
【請求項2】 測定管内を流れる流体の流れ方向に対し
てその磁界の発生方向を垂直として配置された励磁コイ
ルへ所定周波数で励磁電流を供給する励磁電流供給手段
と、前記励磁コイルの発生磁界と直交して前記測定管内
に配置された電極間に得られる信号起電力を検出する信
号起電力検出手段と、この信号起電力検出手段の検出す
る信号起電力に基づいて計測値を求める計測値演算手段
とを備えた電磁流量計において、 前記励磁コイルのコイル間電圧を検出するコイル間電圧
検出手段と、 このコイル間電圧検出手段の検出するコイル間電圧よ
り、コイル間電圧と流体温度との関係を示す第1の記憶
テーブルを参照として、前記流体の温度を求める流体温
度導出手段と、 この流体温度導出手段の求めた流体温度より、所定流量
時における流体温度と計測誤差との関係を示す第2の記
憶テーブルを参照として、その流体温度における所定流
量時の計測誤差を求める計測誤差導出手段と、 この計測誤差導出手段の求めた計測誤差に基づいて前記
計測値演算手段により求められる計測値から流体温度の
変化により生じる誤差成分を除去する温度補正手段とを
備えたことを特徴とする電磁流量計。
2. An exciting current supplying means for supplying an exciting current at a predetermined frequency to an exciting coil arranged such that a magnetic field is generated in a direction perpendicular to a flow direction of a fluid flowing in the measuring tube, and a magnetic field generated by the exciting coil. A signal electromotive force detecting means for detecting a signal electromotive force obtained between electrodes arranged in the measuring tube orthogonally to the measurement tube, and a measured value for obtaining a measured value based on the signal electromotive force detected by the signal electromotive force detecting means. In an electromagnetic flowmeter provided with a calculating means, an inter-coil voltage detecting means for detecting an inter-coil voltage of the exciting coil, and an inter-coil voltage and a fluid temperature are detected from the inter-coil voltage detected by the inter-coil voltage detecting means. With reference to the first storage table showing the relationship, a fluid temperature derivation means for obtaining the temperature of the fluid and a flow at a predetermined flow rate based on the fluid temperature obtained by the fluid temperature derivation means. Based on the measurement error deriving means for obtaining the measurement error at the predetermined flow rate at the fluid temperature and the measurement error obtained by the measurement error deriving means with reference to the second storage table showing the relationship between the body temperature and the measurement error. An electromagnetic flowmeter, comprising: a temperature correction unit that removes an error component caused by a change in fluid temperature from the measurement value obtained by the measurement value calculation unit.
【請求項3】 測定管内を流れる流体の流れ方向に対し
てその磁界の発生方向を垂直として配置された励磁コイ
ルへ所定周波数で励磁電流を供給する励磁電流供給手段
と、前記励磁コイルの発生磁界と直交して前記測定管内
に配置された電極間に得られる信号起電力を検出する信
号起電力検出手段と、この信号起電力検出手段の検出す
る信号起電力に基づいて計測値を求める計測値演算手段
とを備えた電磁流量計において、 前記励磁コイルのコイル間電圧を検出するコイル間電圧
検出手段と、 所定流量時における第1および第2の流体温度での信号
起電力ならびにコイル間電圧を実測して得た定数を記憶
する記憶手段と、 この記憶手段の記憶する定数と前記コイル間電圧検出手
段の検出するコイル間電圧と前記信号起電力検出手段の
検出する信号起電力とから流体温度の変化により生じる
誤差成分の除去された信号起電力を算出する温度補正手
段とを備えたことを特徴とする電磁流量計。
3. Exciting current supply means for supplying an exciting current at a predetermined frequency to an exciting coil arranged such that the direction of the magnetic field is perpendicular to the flow direction of the fluid flowing in the measuring tube, and the magnetic field generated by the exciting coil. A signal electromotive force detecting means for detecting a signal electromotive force obtained between electrodes arranged in the measuring tube orthogonally to the measurement tube, and a measured value for obtaining a measured value based on the signal electromotive force detected by the signal electromotive force detecting means. In an electromagnetic flowmeter provided with a calculating means, an inter-coil voltage detecting means for detecting an inter-coil voltage of the exciting coil, a signal electromotive force and a inter-coil voltage at a first and a second fluid temperature at a predetermined flow rate, Storage means for storing constants obtained by actual measurement, constants stored in the storage means, inter-coil voltage detected by the inter-coil voltage detection means, and detection by the signal electromotive force detection means An electromagnetic flowmeter, comprising: a temperature correction unit that calculates a signal electromotive force from which an error component caused by a change in fluid temperature is removed from the signal electromotive force.
JP15370194A 1994-07-05 1994-07-05 Electromagnetic flowmeter Pending JPH0814971A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15370194A JPH0814971A (en) 1994-07-05 1994-07-05 Electromagnetic flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15370194A JPH0814971A (en) 1994-07-05 1994-07-05 Electromagnetic flowmeter

Publications (1)

Publication Number Publication Date
JPH0814971A true JPH0814971A (en) 1996-01-19

Family

ID=15568231

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15370194A Pending JPH0814971A (en) 1994-07-05 1994-07-05 Electromagnetic flowmeter

Country Status (1)

Country Link
JP (1) JPH0814971A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1387148A2 (en) * 2002-08-02 2004-02-04 ABB PATENT GmbH Method for operating an inductive flow measuring arrangement,as well as flow measuring arrangement
DE102004019189B3 (en) * 2004-04-16 2005-08-18 Krohne Ag Magnetic-inductive throughflow measurement method involves selecting second temperature measurement point so second temperature depends on medium's temperature or/and ambient temperature differently than first temperature
WO2010129240A1 (en) * 2009-05-04 2010-11-11 Rosemount Inc. Magnetic flowmeter for measuring flow

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1387148A2 (en) * 2002-08-02 2004-02-04 ABB PATENT GmbH Method for operating an inductive flow measuring arrangement,as well as flow measuring arrangement
EP1387148A3 (en) * 2002-08-02 2007-06-20 ABB PATENT GmbH Method for operating an inductive flow measuring arrangement,as well as flow measuring arrangement
DE102004019189B3 (en) * 2004-04-16 2005-08-18 Krohne Ag Magnetic-inductive throughflow measurement method involves selecting second temperature measurement point so second temperature depends on medium's temperature or/and ambient temperature differently than first temperature
EP1586870A1 (en) * 2004-04-16 2005-10-19 Krohne AG Method for magnetic-inductive measurement of fluid flow and magnetic-inductive flowmeter
WO2010129240A1 (en) * 2009-05-04 2010-11-11 Rosemount Inc. Magnetic flowmeter for measuring flow
US7963173B2 (en) 2009-05-04 2011-06-21 Rosemount Inc. Magnetic flowmeter for measuring flow
CN102365530A (en) * 2009-05-04 2012-02-29 罗斯蒙德公司 Magnetic flowmeter for measuring flow

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