JPS5847214A - Square wave exciting electro-magnetic flow meter converter - Google Patents

Square wave exciting electro-magnetic flow meter converter

Info

Publication number
JPS5847214A
JPS5847214A JP14462881A JP14462881A JPS5847214A JP S5847214 A JPS5847214 A JP S5847214A JP 14462881 A JP14462881 A JP 14462881A JP 14462881 A JP14462881 A JP 14462881A JP S5847214 A JPS5847214 A JP S5847214A
Authority
JP
Japan
Prior art keywords
converter
signal
output
circuit
fluid
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.)
Granted
Application number
JP14462881A
Other languages
Japanese (ja)
Other versions
JPS6261892B2 (en
Inventor
Toyofumi Tomita
冨田 豊文
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura Electric Co Ltd
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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP14462881A priority Critical patent/JPS5847214A/en
Publication of JPS5847214A publication Critical patent/JPS5847214A/en
Publication of JPS6261892B2 publication Critical patent/JPS6261892B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/002Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow wherein the flow is in an open channel
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/56Measuring 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
    • G01F1/58Measuring 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
    • G01F1/60Circuits therefor

Landscapes

  • Physics & Mathematics (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Measuring Volume Flow (AREA)

Abstract

PURPOSE:To detect the flow-out of liquid in a detector by providing a three- way selection switch that shuts off an exciting circuit by means of giving a mimic signal that is synchronized with the exciting signal to the exciting circuit and providing a comparator that takes as a standard voltage the output of a converter at the time where there is a fluid. CONSTITUTION:A square wave exciting electro-magnetic flow meter converter consists of a high input impedance differential A/C amplifier 11, later stage amplifier 12 that processes the output by calculation. Further, a mimic signal generating circuit that consists of a switch 14 such as FET that is turned on and off in synchronization with the exciting signal, D/C standard voltage source 13, and resistor 15 for current limitation is provided. Also a 3-circuit select switches 19a-c and a comparator 21 are provided. The standard voltage 20 is established equal to the output value of an amplifier 12 that is obtained by input of a mimic signal when the switches 19a-c are operated and a fluid exists in the measurement pipe 3 and the output impedance of the electrode 4 is at maximum, and it is possible to make a comparator 21 sends a signal that indicates that there is no liquid in the measurement tube 3.

Description

【発明の詳細な説明】 本発明は、電磁流量計に係り、特に方形波励磁電磁流量
計検出器の測定管内の流体の存否を検知する機能を有す
る電磁流量計変換器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electromagnetic flowmeter, and more particularly to an electromagnetic flowmeter converter having a function of detecting the presence or absence of fluid in a measurement pipe of a square wave excitation electromagnetic flowmeter detector.

第1図に電磁流量計検出器(以下検出器という)(1)
と電磁流量計変換器(以下変換器という)(5)とから
なる電磁流量計のブロック図を示す。検出器(1)は励
磁コイル(2)と測定管(3)に設けられ流体に発生す
る起電力を検出する電極(4)とからなり、電極間の電
圧は変換器(5)の高入力インピーダンス差動交流増幅
器(6)で増幅され、通常は後段増幅器(7)で4〜2
0 m A I) Cの統一信号にして出力される。
Figure 1 shows the electromagnetic flowmeter detector (hereinafter referred to as the detector) (1).
The block diagram of the electromagnetic flowmeter which consists of and an electromagnetic flowmeter converter (hereinafter referred to as a converter) (5) is shown. The detector (1) consists of an excitation coil (2) and an electrode (4) installed in the measuring tube (3) to detect the electromotive force generated in the fluid, and the voltage between the electrodes is determined by the high input of the converter (5). It is amplified by an impedance differential AC amplifier (6), and usually 4 to 2
0 m A I) It is output as a unified signal of C.

第2図に入力信号の等価回路を示す。図中、(8)は電
極間に同相で現われる同相雑音電圧源、(9)。
FIG. 2 shows an equivalent circuit of the input signal. In the figure, (8) is a common-mode noise voltage source that appears in the same phase between the electrodes, and (9).

(9′)は流量に比例した信号電圧源であり、抵抗(I
I。
(9') is a signal voltage source proportional to the flow rate, and a resistance (I
I.

(10’)は流体の導電率や電極の大きさで主に決まる
出力インピーダンスをあられしている。
(10') indicates the output impedance, which is mainly determined by the conductivity of the fluid and the size of the electrode.

実際に検出器が設置される場合、流量変化、圧力変化が
激しい配管や設置方法そのものにより検出器内の流体が
抜けてしまうこともしばしばある。検出器内の流体が抜
けると、第2図において、信号電源(9)、(9’)は
ゼロ、出力インピーダンス(IL (10’)i無限大
となる。変換器内の差動交流増幅器(6)は、外来雑音
の影響がないなどの理想的な条件であれば出力値はゼロ
となり、流体がない即ち流量がゼロということが出力さ
れ、特に問題は々い。しかしながら通常は、商用電源や
励磁電源からの影響を受け、差動交流増幅器(6)が飽
和を起したりして変換器の出力値はゼロにならず、流体
が流れていると誤認してしまうという不都合が生じた。
When a detector is actually installed, the fluid inside the detector often leaks due to piping or the installation method itself, which undergoes large changes in flow rate and pressure. When the fluid in the detector is discharged, the signal power supplies (9) and (9') become zero and the output impedance (IL (10') i becomes infinite in Fig. 2.The differential AC amplifier ( 6) is especially problematic because under ideal conditions, such as no influence of external noise, the output value will be zero, indicating that there is no fluid, that is, the flow rate is zero.However, normally, commercial power supply The differential AC amplifier (6) may become saturated due to the influence of the converter and the excitation power supply, resulting in the inconvenience that the output value of the converter does not become zero, leading to the misunderstanding that fluid is flowing. .

そして、このような問題に対し従来は次のような対策が
なされていた。その一つの例は第3図に示すように、差
動交流増幅器(6)の各入力とグランド間を抵抗器(i
ll、 (11’)で結びインピーダンスを低くする方
法である。これにより、流体が抜けても入力部のインピ
ーダンスは大きくならず且つ雑音の影響も受けず出力値
はゼロとなる。この方法の欠点は流体の導電率が変化す
ると、つ壕りインピーダンスが変化すると変換器の出力
値が変動することであり、流体の導電率があ′まり低く
なく且つ変化も少ない場合にしか適用できないことであ
る。
Conventionally, the following countermeasures have been taken against such problems. One example is as shown in Figure 3, where a resistor (i) is connected between each input of the differential AC amplifier (6) and the ground.
ll, (11') to lower the impedance. As a result, even if the fluid escapes, the impedance of the input section does not increase, and the output value becomes zero without being affected by noise. The disadvantage of this method is that when the conductivity of the fluid changes, the output value of the converter changes as the trench impedance changes, so it is only applicable when the conductivity of the fluid is not too low and changes little. It is impossible.

捷た、流体が静止しているのか、無いのかのどちらであ
るかということが変換器の出力だけでは判別できない。
It is not possible to determine whether the fluid is stationary or absent from the output of the converter alone.

他の対像例は、測定管に圧力計を取シ付け、管内の圧力
で流体の抜けたことを検出する方法である。通常、流体
が流れれば圧力を生じるので、圧力の上昇が無く、変換
器の出力が振れれば流体抜けとわかる1、この方法の欠
点は、圧力計等余分な計器を必要とすることである。
Another example is a method in which a pressure gauge is attached to a measuring tube and the leakage of fluid is detected based on the pressure inside the tube. Normally, when fluid flows, pressure is generated, so if there is no pressure rise and the output of the converter fluctuates, you can tell that there is a fluid leak1.The disadvantage of this method is that it requires extra instruments such as a pressure gauge. be.

本発明は、検出器内流体の抜けを、変換器側の工夫によ
り特に測定機器を別に用意することなく、また変換器の
入力インピーダンスを下げるという性能の低下も々く検
知することを目的とする。しかしてこの目的は、励磁信
号に同期してオンオフするスイッチと直流基準電圧源と
抵抗器とを有し変換器への入力信号の模擬信号を発生す
る模擬信号発生回路と、この回路の出力信号を前記変換
器の一方の入力へ接続するとともに変換器の他方の入力
をグランドへ接続し且つ励磁回路を遮断する3回路切替
スイッチと、この切替スイッチを作動させたとき前記変
換器の出力電圧を、測定管内に流体が存在し1対の電極
の出力インピーダンスが最高値のときに前記模擬信号を
入力して得られた変換器の出力値に等しく定められた基
準電圧と比較し、この基準電圧を超えたとき測定管内に
流体が存在しないことを示す信号を出力するコンパレー
タとを具備するようにし、前記3回路切替スイッチによ
り流量測定動作と測定管内流体の存否検出動作とが切換
えられるようにしたことにより達成された。
The purpose of the present invention is to easily detect the leakage of fluid in the detector without preparing a separate measuring device by using a device on the converter side, and also to easily detect a drop in performance by lowering the input impedance of the converter. . However, the purpose of the lever is to provide a simulation signal generation circuit that has a switch that turns on and off in synchronization with an excitation signal, a DC reference voltage source, and a resistor, and generates a simulation signal of the input signal to the converter, and an output signal of this circuit. a three-circuit selector switch that connects the converter to one input of the converter, connects the other input of the converter to ground, and interrupts the excitation circuit; and when the selector switch is activated, the output voltage of the converter changes. , when there is a fluid in the measurement tube and the output impedance of the pair of electrodes is at its highest value, the simulated signal is input and the output value of the converter is compared with a reference voltage determined to be equal to the output value of the converter. and a comparator that outputs a signal indicating that there is no fluid in the measuring pipe when the flow rate exceeds 1, and the three-circuit changeover switch can switch between a flow rate measurement operation and an operation for detecting the presence or absence of fluid in the measuring pipe. This was achieved by

以下、本発明の実施例を図面を参照して説明する。第4
図に本発明一実施例の方形波励磁電磁流量計変換器の構
成を示す。方形波励磁電磁流量計変換器は高入力インピ
ーダンス差動交流増幅器(Ll)とその出力を演算処理
する後段増幅器t121.励磁回路(laから構成され
るのは従来通りである。この電磁流量計変換器に下記の
各要素を付設する。励磁信号に同期してオンオフする通
常FET等の半導体で構成されるスイッチa4)、直流
基準電圧源(13)、オンオフされる基準電圧を所定の
電流値に制限する抵抗器QE9からなシミ磁流置針変換
器への入力信号の模擬信号を発生する模擬信号発生回路
を設ける。
Embodiments of the present invention will be described below with reference to the drawings. Fourth
The figure shows the configuration of a square wave excitation electromagnetic flowmeter converter according to an embodiment of the present invention. The square wave excitation electromagnetic flow meter converter includes a high input impedance differential AC amplifier (Ll) and a post-stage amplifier t121. The excitation circuit (la) is the same as before.The following elements are attached to this electromagnetic flowmeter converter.Switch a4, which is usually made of a semiconductor such as an FET, which turns on and off in synchronization with the excitation signal) , a DC reference voltage source (13), and a simulated signal generation circuit that generates a simulated signal of the input signal to the stain magnetic current pointer converter, which includes a resistor QE9 that limits the reference voltage that is turned on and off to a predetermined current value.

まだ、この模擬信号発生回路の出力信号を変換器の一方
の入力へ接続するスイッチ(19b)、変換器の他方の
入力をグランドへ接続するスイッチ(19a )、励磁
回路08)の出力を遮断するスイッチ(19c)からな
る3回路切替スイッチQlを設ける。さらに変換器の後
段増幅器(lりの出力を基準電圧−と比較するコンパレ
ータC11)を設ける。
Still, the switch (19b) that connects the output signal of this simulated signal generation circuit to one input of the converter, the switch (19a) that connects the other input of the converter to the ground, and the output of the excitation circuit 08) are cut off. A three-circuit changeover switch Ql consisting of a switch (19c) is provided. Further, a downstream amplifier (a comparator C11 for comparing the output of the second one with a reference voltage -) is provided after the converter.

上記のように構成された本発明一実施例の電磁流量計変
換器は、3回路切替スイッチ員が図示の状態にある場合
即ち通常の流量測定動作においては、全〈従来通シの方
形波励磁電磁流量計変換器として働くことは明らかであ
る。第5図には、励磁回路a印で作られる励磁信号(2
りを(a)図に、高インピーダンス差動交流増幅器0]
)の内入力に現われる検出器Q7)の出力信号(ハ)を
(b)図に示す。(b)図に示した斜線部分の波高値を
サンプリングし流量信号として出力するのが一般的であ
る。
In the electromagnetic flowmeter converter according to the embodiment of the present invention configured as described above, when the three-circuit changeover switch member is in the state shown in the figure, that is, in normal flow rate measurement operation, all <conventional square wave excitation> It is clear that it works as an electromagnetic flowmeter transducer. Figure 5 shows the excitation signal (2
Figure (a) shows the high impedance differential AC amplifier 0]
) The output signal (c) of the detector Q7) appearing at the input is shown in figure (b). (b) It is common to sample the wave height value of the shaded area shown in the figure and output it as a flow rate signal.

検出器の測定管内の流体の抜けを検出するため3回路切
替スイッチQ卸を切替えた場合には、差動交流増幅器α
υの入力の一端はスイッチ(19a)によジグランドに
落ち、他端はスイッチ(19b)により抵抗器aつに接
続され、励磁回路0均の出力はスイッチ(19c)によ
シ遮断され、そのだめ励磁コイル(2)は励磁されず、
検出器07)内の電極(3)に流量信号は発生しない。
When the 3-circuit selector switch Q is switched to detect the leakage of fluid in the measuring tube of the detector, the differential AC amplifier α
One end of the input of υ is connected to ground by the switch (19a), the other end is connected to one resistor by the switch (19b), and the output of the excitation circuit 0 is cut off by the switch (19c). No excitation coil (2) is not excited,
No flow signal is generated at the electrode (3) in the detector 07).

このときの差動交流増幅器αl)の入力間の電圧波形(
24)を第5図(c)に示す。第5図(C1は第4図に
おける差動交流増幅器(11)の上側入力を基準として
表わしだものであわ、下側入力には負電圧の方形波電圧
が加わる。しかしながら差動交流増幅器αηが交流増幅
器であるため出力は第5図(d)に示した波形(2■が
加わった場合と等価である。この入力波形の波高値は、 7、V、Ro/  R,、十R8−(1,)となる。こ
こでvlは基準電圧源Q鴎の電圧、Roは第2図に示し
た出力インピーダンスθL(10’)の直列合成抵抗値
、R1は抵抗器(1つの抵抗値である。励磁周波数は1
0H2以下と低く、電圧値も安定した領域なので、容量
分等は考えず抵抗器のみと出力インピーダンスを考えて
よい。
At this time, the voltage waveform (
24) is shown in FIG. 5(c). Fig. 5 (C1 is expressed based on the upper input of the differential AC amplifier (11) in Fig. 4. A negative square wave voltage is applied to the lower input. However, the differential AC amplifier αη Since it is an AC amplifier, the output is equivalent to the waveform shown in Figure 5(d) (2■ is added. The peak value of this input waveform is 7, V, Ro/R,, 10R8-( 1, ).Here, vl is the voltage of the reference voltage source Q, Ro is the series combined resistance value of the output impedance θL (10') shown in Fig. 2, and R1 is the resistor (one resistance value). .Excitation frequency is 1
Since the voltage is low, below 0H2, and the voltage value is stable, you can consider only the resistor and output impedance without considering the capacitance.

電磁流量計変換器の出力は、入力波形の波高値に比例す
るから、3回路切替スイッチ翰を切替えた場合の出力値
は(1)式よシ、基準電圧■、に比例1〜、R,> 1
(、oならR6にも比例する。また、(1)式は■1や
R,の値を適当に選ぶことにより変換器の増幅度を変え
なくても流量信号と同じような出力値が得られることを
示している。
The output of an electromagnetic flowmeter converter is proportional to the peak value of the input waveform, so when the three-circuit selector switch is switched, the output value is proportional to the reference voltage 1 to R, according to equation (1). > 1
(If , o, then it is also proportional to R6. Also, equation (1) shows that ■ By appropriately selecting the values of 1 and R, an output value similar to the flow rate signal can be obtained without changing the amplification degree of the converter. This indicates that the

そこで、検出器の測定管内に流体が存在する場合のR8
の最高値を予め求めておき、vl r R4を適当に定
数にして模擬信号発生回路の出力を一定のゲインを持っ
た変換器に入力したときの変換器の出力値を求める。そ
して、この出力値を電圧値とし、これをコンパレータC
υの基準電圧−とする。
Therefore, when there is fluid in the measuring tube of the detector, R8
The highest value of is determined in advance, and the output value of the converter is determined when the output of the simulated signal generation circuit is inputted to a converter having a constant gain with vl r R4 set to an appropriate constant. Then, this output value is set as a voltage value, and this is set as a voltage value by the comparator C.
Let the reference voltage of υ be −.

このように設定、構成された本発明一実施例の電磁流量
計変換器において、通常流量測定動作から3回路切替ス
イッチQ9)Icより測定管内流体存否検知動作に切替
えた場合、変換器の出力電圧値が基準電圧(20)を超
えたときは前丙己のR8が所定最高値より大なるときで
あり、つまシ、測定管内に流体が存在しない場合であシ
、このときのコンパレータ01+の出力により検出器内
流体抜けを知ることができる。
In the electromagnetic flowmeter converter of the embodiment of the present invention set and configured as described above, when switching from the normal flow rate measurement operation to the operation for detecting the presence or absence of fluid in the measurement pipe using the 3-circuit changeover switch Q9) Ic, the output voltage of the converter When the value exceeds the reference voltage (20), it means that the previous R8 is larger than the predetermined maximum value, and if there is no fluid in the measuring tube, the output of comparator 01+ at this time. This allows you to know if there is fluid leakage in the detector.

以上の説明から明らかなように、本発明による電磁流量
−制変換器では、検出器内の流体存否検知のために、特
に変換器のゲインを変えるなどの変更を必要とせず、ま
た変換器に若干の電気部品を追加付設するのみで他の圧
力計などの測定計器やそれを接続するケーブル等も必要
としないで、検出器内の流体の存否を知ることができる
。また、流量測定動作時には従来の変換器と全く同等に
働くので、変換器入力インピーダンス低下に伴う性能低
下がない。第4図の実施例では3回路切替スイッチを用
いたが、これはリレーでも全く問題ないし、変換器のゲ
イン変更もないので遠隔操作で検出器内流体の存否検知
も容易である。
As is clear from the above explanation, the electromagnetic flow control converter according to the present invention does not require any changes such as changing the gain of the converter in order to detect the presence or absence of fluid in the detector, and does not require any change in the gain of the converter. The presence or absence of fluid in the detector can be determined by simply adding a few additional electrical parts and without requiring other measurement instruments such as pressure gauges or cables to connect them. Furthermore, since it works exactly the same as a conventional converter during flow measurement operation, there is no performance deterioration due to a reduction in converter input impedance. In the embodiment shown in FIG. 4, a three-circuit changeover switch is used, but a relay can also be used, and since there is no need to change the gain of the converter, it is easy to detect the presence or absence of fluid in the detector by remote control.

次に、第6図に本発明の別の実施例を示す。この実施例
のものけ、励磁信号を分周器QOで分周j〜、その分周
した励磁信号によりパルス発生器■ηから、例えば正信
号が入った時のみ流体の存否検知に必要な時間だけリレ
ー(ハ)をオンさせるようなワンショットパルスを発生
させる。そして、ワンショットパルスが発生[7ている
間リレーceをオンさせ、流体検知動作を行ない、流量
信号はトラックホールド回路−により流体検知動作直前
の値を出力するようにしたものである。
Next, FIG. 6 shows another embodiment of the present invention. In this embodiment, the excitation signal is frequency-divided by the frequency divider QO, and the frequency-divided excitation signal is used to generate the time required to detect the presence or absence of fluid only when a positive signal is received from the pulse generator ■η. Generates a one-shot pulse that turns on the relay (c). Then, while the one-shot pulse is generated [7], the relay ce is turned on to perform the fluid detection operation, and the flow rate signal is outputted from the track hold circuit at the value immediately before the fluid detection operation.

第4図の実施例では、遠隔操作は可能でも人為的に信号
を与えなければ流体検知動作は行なわなかったが、第6
図の実施例では流体検知を自動で行なうことができる。
In the embodiment shown in Fig. 4, even though remote control was possible, fluid detection operation was not performed unless a signal was given manually.
In the illustrated embodiment, fluid sensing can be performed automatically.

そして、第6図の実施例では励磁信号を分周して検知間
隔を決めているので、特にタイマなど必要なく、また流
量信号もホールド回路を用いて流体検知し2ている間に
発生する誤差をなるべく少なくしている。
In the embodiment shown in Fig. 6, the detection interval is determined by dividing the frequency of the excitation signal, so there is no need for a timer, and the flow rate signal also uses a hold circuit to detect the fluid. I try to keep it as low as possible.

以上詳述したように本発明によれば、電磁流量計検出器
内の流体抜けを特に測定機器を別に用意することなく、
また変換器の入力インピーダンスを下げるという性能の
低下もなく、流量測定動作から任意に切替えて検知でき
る方形波励磁電磁流量計変換器を提供することができる
As detailed above, according to the present invention, fluid leakage in an electromagnetic flowmeter detector can be detected without preparing a separate measurement device.
Further, it is possible to provide a square wave excitation electromagnetic flowmeter converter that can perform detection by arbitrarily switching from flow rate measurement operation without degrading performance due to lowering the input impedance of the converter.

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

第1図は電磁流量計の検出器と変換器からなる構成を示
すブロック図、第2図は変換器への入力信号の等価回路
を示す図、第3図は検出器内流体抜は発生時の誤動作防
止対策の従来例を示す電気的接続図、第4図は本発明一
実施例の方形波励磁電磁流量計変換器の構成を示すブロ
ック図、第5図(a)、(b)、(c)、(diはそれ
ぞれ第4図における励磁信号、差動交流増幅器の肉入力
に現われる検出器の出力信号、流体検知動作時における
差動交流増幅器の入力間の電圧波形、第5図(C)と等
価な入力波形を示すタイムチャート、第6図は本発明の
別の実施例の方形波励磁電磁流量計変換器の構成を示す
ブロック図である。 2・・・励磁コイル   3・・・測定管4・・・電極
10,10′・・・出力インピーダンス11・・・高入
力インピーダンス差動交流増幅器12・・・後段増幅器
  13・・・直流基準電圧源14・・・スイッチ  
 15・・・抵抗器17・・・検出器    18・・
・励磁回路19・・・3回路切替スイッチ 20・・・
基準電圧21・・・コンパレータ  26・・・分周器
27・・・ハルス発生器28・・・リレー29・・・ト
ラックホールド回路 代理人 弁理士 井 上 −男
Figure 1 is a block diagram showing the configuration of the electromagnetic flowmeter's detector and converter, Figure 2 is a diagram showing the equivalent circuit of the input signal to the converter, and Figure 3 shows fluid leakage in the detector when it occurs. 4 is a block diagram showing the configuration of a square wave excitation electromagnetic flowmeter converter according to an embodiment of the present invention; FIGS. 5(a), (b), (c), (di are the excitation signal in Figure 4, the output signal of the detector appearing at the input of the differential AC amplifier, the voltage waveform between the inputs of the differential AC amplifier during fluid detection operation, and Figure 5 ( FIG. 6 is a block diagram showing the configuration of a square wave excitation electromagnetic flowmeter converter according to another embodiment of the present invention. 2. Excitation coil 3. - Measuring tube 4... Electrodes 10, 10'... Output impedance 11... High input impedance differential AC amplifier 12... Post-stage amplifier 13... DC reference voltage source 14... Switch
15...Resistor 17...Detector 18...
・Excitation circuit 19...3 circuit changeover switch 20...
Reference voltage 21... Comparator 26... Frequency divider 27... Hals generator 28... Relay 29... Track hold circuit agent Patent attorney Inoue - Male

Claims (1)

【特許請求の範囲】[Claims] 測定管の管軸に垂直に励磁コイルにより所定周期で一定
の磁界を加え測定管内を流れる導電性流体に発生する電
圧を電極によシ取り出し、極性が反転する前の磁界が安
定した時点における電圧をサンプリングし信号増幅して
流量信号として出力する方形波励磁電磁流量計変換器に
おいて、励磁信号に同期してオンオフするスイッチと、
前記変換器への入力信号の模擬信号を発生する模擬信号
発生回路と、この回路の出力信号を前記変換器の一方の
入力へ接続するとともに変換器の他方の入力をグランド
へ接続し且つ励磁回路の出力を遮断する3回路切替スイ
ッチと、この切替スイッチを作動させたときの前記変換
器の出力電圧を前記測定管内に流体が存在し前記電極の
出力インピーダンスが最高値のときに前記模擬信号を入
力して得られた前記変換器の出力値に等しく定められた
基準電圧と比較!〜この電圧を超えたとき測定管内に流
体が存在しないことを示す信号を出力するコンパレータ
とを具備したことを特徴とする方形波励磁電磁流量計変
換器。
A constant magnetic field is applied at a predetermined period by an excitation coil perpendicular to the tube axis of the measuring tube, and the voltage generated in the conductive fluid flowing inside the measuring tube is extracted by an electrode.The voltage at the point when the magnetic field stabilizes before the polarity reverses. In a square wave excitation electromagnetic flowmeter converter that samples and amplifies the signal and outputs it as a flow signal, there is a switch that turns on and off in synchronization with the excitation signal,
a simulation signal generation circuit that generates a simulation signal of the input signal to the converter; an excitation circuit that connects the output signal of this circuit to one input of the converter and connects the other input of the converter to ground; a three-circuit changeover switch that cuts off the output of the converter; and a three-circuit changeover switch that cuts off the output of the converter when the changeover switch is activated, and a simulated signal that changes the output voltage of the converter when fluid is present in the measurement tube and the output impedance of the electrode is at its highest value. Compare with a reference voltage set equal to the output value of the converter obtained by inputting it! ~ A comparator that outputs a signal indicating that no fluid is present in the measuring tube when this voltage is exceeded.
JP14462881A 1981-09-16 1981-09-16 Square wave exciting electro-magnetic flow meter converter Granted JPS5847214A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14462881A JPS5847214A (en) 1981-09-16 1981-09-16 Square wave exciting electro-magnetic flow meter converter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14462881A JPS5847214A (en) 1981-09-16 1981-09-16 Square wave exciting electro-magnetic flow meter converter

Publications (2)

Publication Number Publication Date
JPS5847214A true JPS5847214A (en) 1983-03-18
JPS6261892B2 JPS6261892B2 (en) 1987-12-23

Family

ID=15366455

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14462881A Granted JPS5847214A (en) 1981-09-16 1981-09-16 Square wave exciting electro-magnetic flow meter converter

Country Status (1)

Country Link
JP (1) JPS5847214A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58153325U (en) * 1982-04-02 1983-10-13 株式会社山武 electromagnetic flow meter
US5325724A (en) * 1991-11-22 1994-07-05 Fischer & Porter Gmbh Apparatus for measuring the flowrate of a fluid
WO1995006857A1 (en) * 1993-09-02 1995-03-09 Rosemount Inc. Magnetic flowmeter with empty pipe detector
DE102014116505B3 (en) * 2014-11-12 2016-03-31 Finetek Co., Ltd. Electromagnetic flowmeter with variable frequency conductivity detection function for a liquid in a pipe
DE102014114443A1 (en) * 2014-10-06 2016-04-07 Finetek Co., Ltd Electromagnetic flowmeter with voltage amplitude conductivity sampling function for a liquid in a pipe

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58153325U (en) * 1982-04-02 1983-10-13 株式会社山武 electromagnetic flow meter
US5325724A (en) * 1991-11-22 1994-07-05 Fischer & Porter Gmbh Apparatus for measuring the flowrate of a fluid
WO1995006857A1 (en) * 1993-09-02 1995-03-09 Rosemount Inc. Magnetic flowmeter with empty pipe detector
US5426984A (en) * 1993-09-02 1995-06-27 Rosemount Inc. Magnetic flowmeter with empty pipe detector
DE102014114443A1 (en) * 2014-10-06 2016-04-07 Finetek Co., Ltd Electromagnetic flowmeter with voltage amplitude conductivity sampling function for a liquid in a pipe
DE102014114443B4 (en) * 2014-10-06 2019-07-11 Finetek Co., Ltd Electromagnetic flowmeter with voltage amplitude conductivity sampling function for a liquid in a pipe
DE102014116505B3 (en) * 2014-11-12 2016-03-31 Finetek Co., Ltd. Electromagnetic flowmeter with variable frequency conductivity detection function for a liquid in a pipe

Also Published As

Publication number Publication date
JPS6261892B2 (en) 1987-12-23

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