JPS6111611Y2 - - Google Patents

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Publication number
JPS6111611Y2
JPS6111611Y2 JP3911280U JP3911280U JPS6111611Y2 JP S6111611 Y2 JPS6111611 Y2 JP S6111611Y2 JP 3911280 U JP3911280 U JP 3911280U JP 3911280 U JP3911280 U JP 3911280U JP S6111611 Y2 JPS6111611 Y2 JP S6111611Y2
Authority
JP
Japan
Prior art keywords
fluid
pipe
switch
signal generator
noise
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
Application number
JP3911280U
Other languages
Japanese (ja)
Other versions
JPS56142320U (en
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 filed Critical
Priority to JP3911280U priority Critical patent/JPS6111611Y2/ja
Publication of JPS56142320U publication Critical patent/JPS56142320U/ja
Application granted granted Critical
Publication of JPS6111611Y2 publication Critical patent/JPS6111611Y2/ja
Expired legal-status Critical Current

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Description

【考案の詳細な説明】 本考案は配管内に挿入して流体の流量を測定す
る挿入式電磁流量計に関する。
[Detailed Description of the Invention] The present invention relates to an insertion type electromagnetic flowmeter that is inserted into piping to measure the flow rate of fluid.

管内流体の流量を測定する挿入式電磁流量計の
ノイズとしては次の3つが挙げられる。
The following three types of noise can be cited as noise in an insertion-type electromagnetic flowmeter that measures the flow rate of fluid in a pipe.

a 磁界を形成するための励磁電源に正弦波交流
を用いたことによる電磁誘導ノイズ b 励磁コイルに電圧を印加することで電極に誘
導される静電誘導ノイズ c 電極と流体間の電気化学現象に基づく電気化
学ノイズ これらのノイズは管内流体の種類または電磁流
量計の設置環境によつて大きく異るために、流量
計の新設または変更の度毎に零点調節を余儀なく
される。したがつて流体が移動中の管内に流量計
を挿入するとともに管内流体の移動を一時的に止
めることによつて正確な零点調節が行なわれてい
た。周知の如く挿入式電磁流量計は流体を移送中
の既設配管への設置が極めて容易であることが特
長であるにも拘わらず管内流体の移動を中断しな
ければ正確な零点調節ができないという点でその
特長を十分に活かしきれず、例えば、不断水で取
付工事を要請された場合には多少の零点のずれは
止むを得ないものとして調整せざるを得なかつ
た。
a Electromagnetic induction noise caused by using a sine wave alternating current as the excitation power source to form a magnetic field b Electrostatic induction noise induced in the electrode by applying voltage to the excitation coil c Electrochemical phenomena between the electrode and the fluid Electrochemical noise based on electrochemical noise Because these noises vary greatly depending on the type of fluid in the pipe or the installation environment of the electromagnetic flowmeter, zero point adjustment is required every time a flowmeter is installed or replaced. Therefore, accurate zero point adjustment has been performed by inserting a flow meter into a pipe during which fluid is moving and temporarily stopping the movement of the fluid within the pipe. As is well known, insertion-type electromagnetic flowmeters have the advantage of being extremely easy to install into existing piping while fluid is being transferred; however, accurate zero point adjustment cannot be made without interrupting the movement of fluid within the pipes. Therefore, the features could not be fully utilized, and for example, when installation work was required due to a water outage, some deviation of the zero point had to be adjusted as it was unavoidable.

本考案は上記の点に鑑みてなされたもので、各
種ノイズの影響を除去するとともに管内流体の移
動を中断することなく零点調節を行い得る挿入式
電磁流量計の提供を目的とする。
The present invention has been made in view of the above points, and aims to provide an insertion type electromagnetic flowmeter that can eliminate the influence of various noises and perform zero point adjustment without interrupting the movement of fluid in the pipe.

以下、添付図面を参照して本考案の一実施例に
ついて説明する。
Hereinafter, one embodiment of the present invention will be described with reference to the accompanying drawings.

図は本考案による挿入式電磁流量計の構成を示
す電気回路図で、流体を移送中の配管1の内部に
電磁流量計の検出部2を挿し込んだもので、その
検出内部には磁場を形成するための励磁コイル3
が納められており、さらに検出部の両外側面には
それぞれ電極4が設けられ管内流体と接してい
る。これらの励磁コイル3および電極4はともに
変換器5に接続されるが、その中電極4の出力は
変換器5内の演算回路6に加えられ管内流体の流
量を算出するために必要な演算を行つた後、零点
調節用の可変抵抗8を通して変換器外の表示計器
10によつて表示されるように講じられており、
一方、励磁コイル3は変換器5内のスイツチ7を
介して方形波電流を供給する信号発生器9の出力
端に結ばれ励磁電流の供給を受けている。ここで
スイツチ7は信号発生器9のアース側に設けられ
る。
The figure is an electric circuit diagram showing the configuration of the insertion-type electromagnetic flowmeter according to the present invention, in which the detection part 2 of the electromagnetic flowmeter is inserted inside the pipe 1 that is transferring fluid, and a magnetic field is applied inside the detection part 2. Excitation coil 3 for forming
Further, electrodes 4 are provided on both outer surfaces of the detection section and are in contact with the fluid within the tube. Both of these exciting coils 3 and electrodes 4 are connected to a converter 5, and the output of the electrodes 4 is applied to an arithmetic circuit 6 in the converter 5 to perform the arithmetic operations necessary to calculate the flow rate of the fluid in the pipe. After the change is made, it is arranged to be displayed by a display instrument 10 outside the converter through a variable resistor 8 for zero point adjustment,
On the other hand, the excitation coil 3 is connected via a switch 7 in the converter 5 to the output end of a signal generator 9 which supplies a square wave current, and is supplied with an excitation current. Here, the switch 7 is provided on the ground side of the signal generator 9.

上記の如く構成された本考案による挿入式電磁
流量計の作用を以下に説明する。
The operation of the insertion type electromagnetic flowmeter according to the present invention constructed as described above will be explained below.

先ず、信号発生器9を発振させ、動作に必要な
方形波電圧を演算回路6に供給すると共に、スイ
ツチ7を閉成して流量検出に必要な方形波電流を
励磁コイル3に加える。この方形波電流は分極を
生じない範囲の適切な周期を持つておれば、その
極性が交互に変化しても、あるいは、極性の変化
しない直流を間歇的に加えるもののどちらでもよ
い。いずれにしても演算回路6は、励磁コイル3
からスイツチ7を通して信号発生器9に流れ込む
電流波形の立上がりから所定時間を経過して電流
値が十分に安定した時点で、電極4,4間に発生
する電圧信号をサンプリングし、例えば、増幅し
て表示計器10に加える。このとき、励磁コイル
3は方形波電流によつて励磁される、前述の電磁
誘導ノイズを除去することができる。
First, the signal generator 9 is oscillated to supply a square wave voltage necessary for operation to the arithmetic circuit 6, and the switch 7 is closed to apply a square wave current necessary for flow rate detection to the excitation coil 3. As long as this square wave current has an appropriate period within a range that does not cause polarization, the polarity may alternately change, or a direct current with no change in polarity may be applied intermittently. In any case, the arithmetic circuit 6
When the current value becomes sufficiently stable after a predetermined period of time has elapsed from the rise of the current waveform that flows into the signal generator 9 through the switch 7, the voltage signal generated between the electrodes 4, 4 is sampled and, for example, amplified. Add to display instrument 10. At this time, the excitation coil 3 is excited by the square wave current and can remove the above-mentioned electromagnetic induction noise.

次に、信号発生器9を発振させ、演算回路6に
電流を供給し、スイツチ7を開放した場合には励
磁コイル3に電流が供給されることはないから磁
界は発生しない。しかし、励磁コイルはスイツチ
7が挿入されない側のラインで信号発生器9と結
ばれるので、流量測定時と同様な電圧が印加され
ることとなり電極4に対して静電誘導ノイズを発
ぜしめる。一方、電極4,4間には当初から電気
化学ノイズが発生している。すなわち、信号発生
器9を発振させたままでスイツチ7を開放した場
合には、流体に対して磁界が作用することはな
く、したがつて、流体の流量信号を含まない静電
誘導ノイズと電気化学ノイズの和が演算回路6の
出力となる。そこで、可変抵抗器8を調節して表
示計器10の指示値を零にすれば、前述のノイズ
値を補正した零点調節が行なわれる。
Next, when the signal generator 9 is caused to oscillate and current is supplied to the arithmetic circuit 6, and the switch 7 is opened, no current is supplied to the excitation coil 3, so no magnetic field is generated. However, since the excitation coil is connected to the signal generator 9 through the line on the side where the switch 7 is not inserted, the same voltage as when measuring the flow rate is applied, causing electrostatic induction noise to the electrode 4. On the other hand, electrochemical noise has been generated between the electrodes 4 from the beginning. That is, if the switch 7 is opened while the signal generator 9 continues to oscillate, the magnetic field will not act on the fluid, and therefore electrostatic induction noise and electrochemical noise that does not include the fluid flow rate signal will be generated. The sum of the noises becomes the output of the arithmetic circuit 6. Therefore, by adjusting the variable resistor 8 to make the indicated value of the display meter 10 zero, the zero point adjustment is performed with the above-mentioned noise value corrected.

かかる零点調節を行つた後、スイツチ7を閉成
することで管内流体の正しい流量値が表示計器1
0に表示される。
After performing such zero point adjustment, by closing the switch 7, the correct flow rate value of the fluid in the pipe will be displayed on the meter 1.
Displayed as 0.

以上の説明によつて明らかな如く、本考案の挿
入式電磁流量計によれば、方形波電流を使用して
いるので高い電磁誘導ノイズを除去し得るととも
に、管内流体の移動を中断することなく零点調節
を極めて容易に行うことができる。
As is clear from the above explanation, the insertion-type electromagnetic flowmeter of the present invention uses square wave current, so high electromagnetic induction noise can be removed, and the flow of fluid in the pipe is not interrupted. Zero point adjustment can be performed extremely easily.

また、信号発生器9を発振させスイツチ7を開
放した状態で可換抵抗器8の零点調節を全く行な
わない場合には静電誘導ノイズと電気化学ノイズ
との和が表示計10に表わされるので、これらの
ノイズレベルを間接的に測定することができると
同時に、ノイズ発生原因を追求する手段として用
いることも可能である。
Furthermore, if the zero point adjustment of the variable resistor 8 is not performed at all with the signal generator 9 oscillating and the switch 7 open, the sum of electrostatic induction noise and electrochemical noise will be displayed on the display meter 10. , these noise levels can be measured indirectly, and at the same time, it can also be used as a means to investigate the cause of noise generation.

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

図は本考案による挿入式電磁流量計の構成を示
す電気回路図である。 1……配管、2……検出部、3……励磁コイ
ル、4……電極、5……変換器、6……演算回
路、7……スイツチ、8……可変抵抗、9……信
号発生器、10……表示計器。
The figure is an electrical circuit diagram showing the configuration of an insertion type electromagnetic flowmeter according to the present invention. 1... Piping, 2... Detection unit, 3... Excitation coil, 4... Electrode, 5... Converter, 6... Arithmetic circuit, 7... Switch, 8... Variable resistance, 9... Signal generation Instrument, 10...display instrument.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 配管内に電極および励磁コイルを挿入して配管
内の被測定流体の流量を求める電磁流量計におい
て、励磁コイルに方形波電流を供給する信号発生
器と、前記コイルおよび信号発生器間のアース側
ラインに設けられるスイツチとを具え、前記スイ
ツチを開放して指示計の零点調節を行うことを特
徴とする挿入式電磁流量計。
In an electromagnetic flowmeter that measures the flow rate of a fluid to be measured in a pipe by inserting an electrode and an excitation coil into the pipe, a signal generator that supplies a square wave current to the excitation coil, and a ground side between the coil and the signal generator. 1. An insertion-type electromagnetic flowmeter comprising: a switch provided in a line, the switch being opened to adjust the zero point of an indicator.
JP3911280U 1980-03-25 1980-03-25 Expired JPS6111611Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3911280U JPS6111611Y2 (en) 1980-03-25 1980-03-25

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3911280U JPS6111611Y2 (en) 1980-03-25 1980-03-25

Publications (2)

Publication Number Publication Date
JPS56142320U JPS56142320U (en) 1981-10-27
JPS6111611Y2 true JPS6111611Y2 (en) 1986-04-12

Family

ID=29634584

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3911280U Expired JPS6111611Y2 (en) 1980-03-25 1980-03-25

Country Status (1)

Country Link
JP (1) JPS6111611Y2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2017044694A (en) * 2015-08-26 2017-03-02 テックロス カンパニー リミテッド Electromagnetic flow meter

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE10118003A1 (en) * 2001-04-10 2002-10-24 Krohne Messtechnik Kg Magnetic-inductive flowmeter and magnetic-inductive flowmeter

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2017044694A (en) * 2015-08-26 2017-03-02 テックロス カンパニー リミテッド Electromagnetic flow meter

Also Published As

Publication number Publication date
JPS56142320U (en) 1981-10-27

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