JPS5815120A - Transmitter of electromagnetic flowmeter - Google Patents
Transmitter of electromagnetic flowmeterInfo
- Publication number
- JPS5815120A JPS5815120A JP11360581A JP11360581A JPS5815120A JP S5815120 A JPS5815120 A JP S5815120A JP 11360581 A JP11360581 A JP 11360581A JP 11360581 A JP11360581 A JP 11360581A JP S5815120 A JPS5815120 A JP S5815120A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- conduit
- electrode
- frequency
- flow rate
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/56—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects
- G01F1/58—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects by electromagnetic flowmeters
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Volume Flow (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は電磁流量計発信器に関し、その構造が簡単に表
るとともに信頼性が向上するよう改曳したi)5ある。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electromagnetic flowmeter transmitter, and has been modified to simplify the structure and improve reliability.
第1(2)は従来の電磁流量計発信器の要部を示す。同
図に示すように導管1には一対の測定電極2,2aが装
着されてお)、この測定電極2.2mは端子3,3al
介して図示しない増幅器に接続されている。磁界発生装
置4は、商用周波数の正弦波磁界を発生し、この磁界の
向きが導管lの管軸及び測定電極2.2a間を結ぶ直線
に対し夫々直交するように配設されている。このため測
定電極2,2aより流量に比例した流量信号が送出され
る。更にtXz図に示す等価回路を基に従来技#fを評
言すると、導管1円の流体には、磁界発生装置4の磁界
による流量電圧e@、e@のみならず商用電源に基づく
商用周波数雑音(コモンそ−Pノイズ) eCNも発生
している。したがって測定電極2.2aと流体との間の
接液インピーダンス2及び流体自体の抵抗rを介し、測
定電極2Kに流m′電圧eSと商用周波数雑音Ccj*
が、測定電極2aには流量電圧−csと商用周波数雑音
eCNが夫々生起される。仁のとき測定電極2は、端子
3に接続された高入力インピーダンスのバッファアンプ
5を介し、同相ノイズ除去用の抵抗R1,R2、R3。Part 1 (2) shows the main parts of a conventional electromagnetic flowmeter transmitter. As shown in the figure, a pair of measuring electrodes 2, 2a are attached to the conduit 1), and this measuring electrode 2.2m is attached to the terminals 3, 3al.
It is connected to an amplifier (not shown) via the power supply. The magnetic field generator 4 generates a sinusoidal magnetic field at a commercial frequency, and is arranged so that the direction of the magnetic field is perpendicular to the straight line connecting the tube axis of the conduit l and the measurement electrodes 2.2a. Therefore, a flow rate signal proportional to the flow rate is sent out from the measurement electrodes 2, 2a. Furthermore, evaluating the conventional technique #f based on the equivalent circuit shown in the tXz diagram, the fluid in one circle of the conduit has not only the flow voltage e@, e@ due to the magnetic field of the magnetic field generator 4, but also commercial frequency noise due to the commercial power supply. (Common So-P noise) eCN is also generated. Therefore, through the wetted impedance 2 between the measuring electrode 2.2a and the fluid and the resistance r of the fluid itself, m' voltage eS and commercial frequency noise Ccj* flow to the measuring electrode 2K.
However, a flow voltage -cs and a commercial frequency noise eCN are generated at the measurement electrode 2a. When the measurement electrode 2 is connected to a high input impedance buffer amplifier 5 connected to the terminal 3, the measurement electrode 2 is connected to the resistors R1, R2, and R3 for removing common mode noise.
瓜が接続された差動アyゾロの非反転入力端子に接続さ
れてお夛、同様に測定電極2aはパツ7アアンデ5af
介し差動アンプ6の反転入力端子に接続されている。ま
た差動アンプ6の出力側の端子7,7aには、電磁流量
計発信器からの*iな流量信号を統−電流信号若しくは
−9ルス列信号に変換する変換器(図示省略)が接続さ
れる。このため測定電極2,2aに夫々生起されたrt
t*電圧as 、 −esO差の電圧2eBに対応し友
流量信号が差動アンプ6から変換器に送出されるととも
に、との差動アンプ6に同相ノイズとなって入力される
商用周波数雑音elcNは相殺されて除去される。Similarly, the measurement electrode 2a is connected to the non-inverting input terminal of the differential y-Zoro connected to the electrode 2a.
The inverting input terminal of the differential amplifier 6 is connected to the inverting input terminal of the differential amplifier 6 through the inverting input terminal. In addition, a converter (not shown) that converts the *i flow rate signal from the electromagnetic flowmeter transmitter into a unified current signal or -9 pulse train signal is connected to the output side terminals 7 and 7a of the differential amplifier 6. be done. Therefore, the rt generated in the measurement electrodes 2 and 2a, respectively.
A flow rate signal corresponding to the voltage 2eB of the difference between t* voltage as and -esO is sent from the differential amplifier 6 to the converter, and the commercial frequency noise elcN is input as common mode noise to the differential amplifier 6. are canceled out and removed.
ところでかかる従来技術モは、2本の測定電極2,2a
を導管1に装着したため、この装着部を介して流体が漏
れる鉋率が高いばかりでなく、流体のシールがなされる
ように測定電極2.2aを導管lに装着するという複雑
なシール構造を2箇所に備えなければならなかった。By the way, in the conventional technique, two measurement electrodes 2, 2a are used.
is attached to the conduit 1, which not only increases the chance of fluid leaking through this attachment part, but also requires a complicated sealing structure in which the measurement electrode 2.2a is attached to the conduit 1 to ensure a fluid seal. I had to prepare in place.
本発明に、上記従来技術に鑑み、シール漏れの確率が低
く構造が簡雛であるとともに信頼性の高い電磁流量計発
信器を提供することを目的とする。かかる目的を達成す
る本発明の構成は、流体が流通する導管と直交するよう
に商用周波数と異なる周波数の磁界全発生する磁界発生
装置と、前記導管に装着された1本の測定電極とを有し
、前記流体及び磁界により測定電極と基準電位点間に生
起された流量信号を得ることを特徴とする。In view of the above prior art, it is an object of the present invention to provide an electromagnetic flowmeter transmitter that has a low probability of seal leakage, has a simple structure, and is highly reliable. The configuration of the present invention that achieves this object includes a magnetic field generating device that generates a magnetic field at a frequency different from the commercial frequency so as to be orthogonal to a conduit through which fluid flows, and one measurement electrode attached to the conduit. and obtaining a flow signal generated between the measurement electrode and a reference potential point by the fluid and the magnetic field.
以下本発明の冥施Nを図面に基づき詳細に説明すゐ。な
お従来技術と同一部分には同一番号を付し重複する説明
は省略する。Below, the ritual N of the present invention will be explained in detail based on the drawings. Note that parts that are the same as those in the prior art are given the same numbers and redundant explanations will be omitted.
第3図は本発明の実施例の等価回路を示す。FIG. 3 shows an equivalent circuit of an embodiment of the present invention.
同図に示すように磁界発生装置8は1周波数が商用周波
数の百の矩形波磁界を発生しており。As shown in the figure, the magnetic field generating device 8 generates a rectangular wave magnetic field with one frequency being a commercial frequency.
この矩形波磁界が導管1と直交するように配設されてい
る。また導管IKは1本の測定電極2が装着されており
、この測定電極2は差動アンプ6の非反転入力端子に接
続されている。このとき差動アンプ60反転入力端子は
起電力の生じない場所で接液されている。つまりこの差
動アンプ6に、これに入力される電圧に対応した信号を
送出するのみでノイズを除去する機能に有していない。This rectangular wave magnetic field is arranged so as to be orthogonal to the conduit 1. Further, one measuring electrode 2 is attached to the conduit IK, and this measuring electrode 2 is connected to the non-inverting input terminal of the differential amplifier 6. At this time, the inverting input terminal of the differential amplifier 60 is in contact with the liquid at a location where no electromotive force is generated. In other words, the differential amplifier 6 only sends out a signal corresponding to the voltage input thereto, but does not have the function of removing noise.
このため矩形波磁界により発生した流量電圧e8のみな
らず、商用電源に起因して発生する商用周波数雑音ec
xや矩形波磁界の時間的変化(矩形波磁界の立上シ時や
立下)時における変化)に起因して発生する電磁誘導雑
音eiNも差曽アンプ6に入力される結果、このアンプ
6の出力である流量信号には商用周波数雑音ecN及び
電磁誘導雑音eiNを含んだものとなる。したがって、
端子7,7aに接続される変換器(図示省略)には、雑
音が含まれた流量信号が入力される。ところが、電磁流
量計発信器が本実施例の如く、低周波励振型である場合
変換器において、矩形波磁界(励振磁界)が安定した時
点で且つタイミングを商用周波数雑音に同期させて信号
全サンプリングする構造になっている結果、商用周波数
雑音ecl(及び電磁誘導雑音eiNを除去し、流量信
号のみを取り出し得、正確な流量測定が出来る。Therefore, not only the flow voltage e8 generated by the rectangular wave magnetic field but also the commercial frequency noise ec generated due to the commercial power supply
Electromagnetic induction noise eiN generated due to x and temporal changes in the rectangular wave magnetic field (changes at the time of rise and fall of the rectangular wave magnetic field) is also input to the differential amplifier 6, and as a result, this amplifier 6 The flow rate signal that is the output includes commercial frequency noise ecN and electromagnetic induction noise eiN. therefore,
A flow signal containing noise is input to a converter (not shown) connected to the terminals 7 and 7a. However, when the electromagnetic flowmeter oscillator is of a low frequency excitation type as in this embodiment, the converter performs all signal sampling at the point when the rectangular wave magnetic field (excitation magnetic field) is stabilized and the timing is synchronized with the commercial frequency noise. As a result, commercial frequency noise ecl (and electromagnetic induction noise eiN) can be removed, only the flow rate signal can be extracted, and accurate flow rate measurement can be performed.
ここで本実施例によ〕実際に流量を測定した測定結果を
第4図及び第5図に示す。第4図は規定の流量を100
〔チ〕としたフロー1ノート(FLOW RATE)に
対する本実施例に係る電磁流量計発信器の出力誤差(q
6 rate)を示し。The results of actual flow rate measurements according to this embodiment are shown in FIGS. 4 and 5. Figure 4 shows the specified flow rate as 100
Output error (q
6 rate).
この特性から出力誤差は±0.6 (” % rate
)以内であることがわかる。また第5図に70−1/
−ト< FLOW RATE)に対する出力表示(0
UTPUT )を示し、この特性からも極めて誤差の少
ないことがわかる。From this characteristic, the output error is ±0.6 ("% rate
). Also shown in Figure 5 is 70-1/
- Output display (0
UTPUT), and it can be seen from this characteristic that the error is extremely small.
なお上記実施例でに磁界発生装置8にて低周波の矩形波
磁界を発生せしめたが、測定のために発生せしめられる
磁界としては、その周波数が商用周波数と異なっていれ
ば充分である。っ壕り商用周波数と異なる周波数の磁界
を採用すれば変換器によって流量信号のみを取り出し得
るのである。また、差動アンプ6の反転入力端子の接液
は、第10図に示すように、流体と電気的導通のある接
続された相手配管でとってもよりし、第11図に示すよ
うに、電磁流量計発信器の7ランジ端面に付属した接液
フランジ10でとってもよい、また、流体が接地してい
る場合には第12図に示すように、差動アンゾロの反転
入力電子は、接地してよい。また測定電極2は第1図に
示すような点電極に限らず、第6図及び第7図に示すよ
うに導管1の内周面に臨む線状をなす線電極や、第8図
に示すように導管1の内周面に臨む面状をなす面電極や
、更には第9図に示すように導管1のライニング材lb
中に埋設される容量検出形電極であってもよい。In the above embodiment, the magnetic field generator 8 generates a low frequency rectangular wave magnetic field, but it is sufficient for the magnetic field to be generated for measurement as long as the frequency is different from the commercial frequency. By using a magnetic field with a frequency different from the trench commercial frequency, it is possible to extract only the flow rate signal using a converter. In addition, as shown in FIG. 10, the inverting input terminal of the differential amplifier 6 is in contact with liquid through a connected mating pipe that has electrical continuity with the fluid, and as shown in FIG. 11, the electromagnetic flow rate This may be done with the liquid contact flange 10 attached to the end face of the 7-lange of the meter transmitter.Also, if the fluid is grounded, the inverting input electron of the differential anzoro may be grounded as shown in Figure 12. . Furthermore, the measurement electrode 2 is not limited to a point electrode as shown in FIG. 1, but may also be a linear electrode facing the inner peripheral surface of the conduit 1 as shown in FIGS. 6 and 7, or a wire electrode as shown in FIG. As shown in FIG.
It may also be a capacitive sensing electrode embedded therein.
なお第91i!!中の符号で9はノ・ウジングを示す。Furthermore, the 91st i! ! The code in the middle, 9, indicates No-Using.
以上実施例とともに具体的に説明したように本発明によ
れば、導管に装着する測定電極を1本としたため、構造
が簡単になるとともに製造が容易になりコストが低減す
るばかシでなく。As specifically explained above in conjunction with the embodiments, according to the present invention, only one measuring electrode is attached to the conduit, which simplifies the structure, facilitates manufacturing, and reduces costs.
測定電極の装着部分におけるシール漏れの確率が低下し
信頼性が向上する。更に商用周波数と異なる周波数の磁
界により励振したため、電磁流量計発信器に変換器を接
続することにより流量に対応した流量信号のみを取シ出
せ、正確な流量測定ができる。The probability of seal leakage at the part where the measurement electrode is attached is reduced and reliability is improved. Furthermore, since the electromagnetic flowmeter was excited by a magnetic field with a frequency different from the commercial frequency, by connecting a converter to the electromagnetic flowmeter oscillator, only the flow rate signal corresponding to the flow rate can be extracted, allowing accurate flow rate measurement.
第1図に従来の電磁流量計発信器の要部を示す斜視図、
第2図はその等価回路を示す回路図第3図は本発明の実
施例の等価回路を示す回路図、第4図は本実施例のフロ
ーレート−出力誤差特性を示す特性図、第5図はそのフ
ローレート−出力表示特性を示す特性図、第6図ないし
第9図は本実施例に用いる測定電極の他の例を図面甲、
1は導管、
2.2aは測定電極、
4.8は磁界発生装置である。
特許出願人
株式会社 北辰電機製作所
代理人
弁理士 元方 士 部(他1名)
第3図
表
示
第4図
第5図Fig. 1 is a perspective view showing the main parts of a conventional electromagnetic flowmeter transmitter.
FIG. 2 is a circuit diagram showing the equivalent circuit. FIG. 3 is a circuit diagram showing the equivalent circuit of the embodiment of the present invention. FIG. 4 is a characteristic diagram showing the flow rate-output error characteristic of this embodiment. 1 is a characteristic diagram showing its flow rate-output display characteristics, and FIGS. 6 to 9 show other examples of measurement electrodes used in this example. 1 is a conduit, 2.2a is a measurement electrode, 4.8 is a magnetic field generator. Patent Applicant Hokushin Electric Manufacturing Co., Ltd. Representative Patent Attorney Mr. Motogata (and 1 other person) Figure 3 Display Figure 4 Figure 5
Claims (1)
る周波数の磁界を発生する磁界発生装置と、前記導管に
装着された1本の測定電極とt−iし、前記流体及び磁
界により測定電極と基準電位点間に生起された流量信号
を得ることを特徴とする電磁流量計発信器。A magnetic field generating device that generates a magnetic field with a frequency different from the commercial frequency so as to be orthogonal to a conduit through which a fluid flows, and a measuring electrode attached to the conduit, and a measuring electrode and a measuring electrode attached to the conduit. An electromagnetic flowmeter transmitter characterized in that it obtains a flow rate signal generated between reference potential points.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11360581A JPS5815120A (en) | 1981-07-22 | 1981-07-22 | Transmitter of electromagnetic flowmeter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11360581A JPS5815120A (en) | 1981-07-22 | 1981-07-22 | Transmitter of electromagnetic flowmeter |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5815120A true JPS5815120A (en) | 1983-01-28 |
Family
ID=14616446
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11360581A Pending JPS5815120A (en) | 1981-07-22 | 1981-07-22 | Transmitter of electromagnetic flowmeter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5815120A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6356800B2 (en) * | 1984-08-03 | 1988-11-09 | Asahi Chemical Ind | |
US5932454A (en) * | 1996-12-20 | 1999-08-03 | Daicel Chemical Industries, Ltd. | Method of producing carboxylic acids |
-
1981
- 1981-07-22 JP JP11360581A patent/JPS5815120A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6356800B2 (en) * | 1984-08-03 | 1988-11-09 | Asahi Chemical Ind | |
US5932454A (en) * | 1996-12-20 | 1999-08-03 | Daicel Chemical Industries, Ltd. | Method of producing carboxylic acids |
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