JPH06174513A - Emptiness detection circuit of electromagnetic flowmeter - Google Patents

Emptiness detection circuit of electromagnetic flowmeter

Info

Publication number
JPH06174513A
JPH06174513A JP32831092A JP32831092A JPH06174513A JP H06174513 A JPH06174513 A JP H06174513A JP 32831092 A JP32831092 A JP 32831092A JP 32831092 A JP32831092 A JP 32831092A JP H06174513 A JPH06174513 A JP H06174513A
Authority
JP
Japan
Prior art keywords
signal
detection circuit
circuit
empty
flow meter
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
JP32831092A
Other languages
Japanese (ja)
Inventor
Keiichiro Tago
敬一郎 多胡
Keita Okawa
啓太 大川
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP32831092A priority Critical patent/JPH06174513A/en
Publication of JPH06174513A publication Critical patent/JPH06174513A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To enable emptiness to be detected in the case of empty state by providing an emptiness detection circuit between one of a pair of electrodes of the measuring pipe and a ground terminal for liquid-contacting only the electrode without the emptiness detection circuit. CONSTITUTION:AC content of voltage between a ground terminal 5-1 and an electrode 1-2 and that between the ground terminal 1-5 and an electrode 1-3 are fed to an addition circuit 3-1 via a DC capacitor 1-6 and a DC cut capacitor 1-7, respectively, for addition. The addition signal is amplifier by a non-inversion amplifier circuit 3-2, is rectified by a smoothing circuit 3-3 and them smoothed, and is compared with a comparison reference voltage 3-4-6 by a comparator 3-4, thus obtaining an emptiness detection signal 3a which is H in an empty state and L in a full state.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は導電性の流体が磁界内を
通過するとき、その速さに比例した電圧が誘起するとい
うファラデーの法則を用いた電磁流量計の検出器におけ
る測定管内の空状態を検知する回路、特に電磁流量計変
換器から出力される流量信号の精度を維持しつつ空状態
を確実に検出できるようにした電磁流量計空検知回路に
関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an empty space in a measuring tube in a detector of an electromagnetic flow meter using Faraday's law that a voltage proportional to the speed of a conductive fluid is induced when the fluid flows in a magnetic field. BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a circuit for detecting a state, and more particularly to an electromagnetic flow meter empty detection circuit capable of reliably detecting an empty state while maintaining accuracy of a flow rate signal output from an electromagnetic flow meter converter.

【0002】なお以下各図において同一の符号は同一も
しくは相当部分を示す。
In the following figures, the same reference numerals indicate the same or corresponding parts.

【0003】[0003]

【従来の技術】電磁流量計のこの種の空検知回路として
は本出願人の先願になる、特開昭63−006420
号,「電磁流量計の空水検知回路」がある。この先願の
発明は、電磁流量計検出部における測定管内の2つの電
極のうちいずれか一方の電極に発生する電圧中の交流分
の大きさが、接液状態の場合と空水状態の場合とでは大
きく異なるので、前記交流分を増幅した後直流化し、こ
の結果得られる直流電圧を基準電圧と比較することによ
って空水状態検知を行うようにしたものである。
2. Description of the Related Art As an empty detection circuit of this kind for an electromagnetic flow meter, the applicant of the present application has filed a prior application, Japanese Patent Laid-Open No. 63-006420.
No., "Electromagnetic flowmeter empty water detection circuit". According to the invention of this prior application, the magnitude of the alternating current component in the voltage generated at any one of the two electrodes in the measuring tube in the electromagnetic flowmeter detection unit is in the liquid contact state and the empty water state. However, since the AC component is amplified, the AC component is converted into DC, and the DC voltage obtained as a result is compared with a reference voltage to detect the empty water state.

【0004】[0004]

【発明が解決しようとする課題】図3は検出部内の測定
管の空状態と判定すべき接液状態の1例を示す。同図に
おいて1−1は測定管、1−2,1−3は電極、8は測
定流体である。ところで前記先願の空検知回路は、検出
部における測定管1−1内の2つの電極1−2,1−3
のうち一方の電極だけが空検知回路に接続されている。
今、測定流体8が図3のように測定管1−1内に存在し
ていた場合、もし接液されている電極1−2に空検知回
路が接続されていなければ、空検知できないという問題
が起きる。そこで本発明はこの問題を解消できる電磁流
量計の空検知回路を提供することを課題とする。
FIG. 3 shows an example of a liquid contact state which should be judged to be an empty state of the measuring tube in the detector. In the figure, 1-1 is a measuring tube, 1-2 and 1-3 are electrodes, and 8 is a measuring fluid. By the way, the sky detection circuit of the above-mentioned prior application has two electrodes 1-2, 1-3 within the measuring tube 1-1 in the detection section.
Only one of the electrodes is connected to the empty detection circuit.
Now, when the measurement fluid 8 is present in the measurement tube 1-1 as shown in FIG. 3, the empty detection cannot be performed unless the empty detection circuit is connected to the electrode 1-2 which is in contact with the liquid. Occurs. Therefore, it is an object of the present invention to provide an empty detection circuit for an electromagnetic flow meter that can solve this problem.

【0005】[0005]

【課題を解決するための手段】前記の課題を解決するた
めに、請求項1の空検知回路は、電磁流量計の検出器
(検出部1の測定管1−1など)における一対の電極
(1−2,1−3など)とアース(アース端子1−5な
ど)との間に発生する各電圧のうちの交流分の和を抽出
してこの和に応じた加算交流信号を出力する交流分加算
抽出手段(加算回路3−1,非反転増幅回路3−2な
ど)と、該加算交流信号を直流信号に変換する直流化手
段(平滑回路3−3など)と、前記直流信号を基準信号
(比較基準電圧3−4−6など)と比較して比較結果に
応じた信号を出力する比較手段(コンパレータ3−4な
ど)とを備え、前記比較手段の出力信号(空検知信号3
aなど)にもとづき前記検出器における空状態を検知す
るようにする。
In order to solve the above-mentioned problems, the empty detection circuit according to claim 1 has a pair of electrodes in a detector of an electromagnetic flow meter (such as the measuring tube 1-1 of the detection section 1). AC that outputs the addition AC signal corresponding to this sum by extracting the sum of the AC components of the respective voltages generated between (1-2, 1-3, etc.) and the ground (ground terminal 1-5, etc.) Minute addition extraction means (adding circuit 3-1, non-inverting amplifier circuit 3-2, etc.), DC conversion means (smoothing circuit 3-3, etc.) for converting the added AC signal into a DC signal, and the DC signal as a reference And a comparison means (comparator 3-4 etc.) for comparing the signal (comparison reference voltage 3-4-6 etc.) and outputting a signal according to the comparison result, and the output signal of the comparison means (empty detection signal 3
(a) or the like) is used to detect an empty state in the detector.

【0006】また請求項2の空検知回路では、請求項1
に記載の空検知回路において、前記直流信号は少なくと
も第1の可変抵抗器(3−2−3など)により増幅度が
可変設定される増幅手段(非反転増幅回路3−2など)
を経て得られるものであるようにする。また請求項3の
空検知回路では、請求項1または請求項2に記載の空検
知回路において、前記基準信号は第2の可変抵抗器(3
−4−5など)により可変設定されるものであるように
する。
According to a second aspect of the empty detection circuit of the present invention,
In the empty detection circuit described in (1), the DC signal has an amplification degree variably set by at least a first variable resistor (3-2-3, etc.) (non-inverting amplification circuit 3-2, etc.).
Be obtained through. Further, in the sky detection circuit according to claim 3, in the sky detection circuit according to claim 1 or 2, the reference signal is the second variable resistor (3
-4-5, etc.).

【0007】[0007]

【作用】本発明では、測定管内の1対の電極とアースと
の間に発生する各交流信号の和を抽出することにより、
前記の問題を解消する。ここで抽出される交流信号は主
として商用周波のノイズであるが、これは測定管の口径
や配管への接地状態によって、その大きさが異なる。従
って増幅率を可変にして最適な増幅度を容易に得るよう
にする。しかし回路定数の制約等により増幅度の可変範
囲に制約を受ける場合もある。その場合には、コンパレ
ータの比較基準電圧を可変にして同等の効果を得る。
In the present invention, by extracting the sum of the AC signals generated between the pair of electrodes in the measuring tube and the ground,
The above problems are solved. The AC signal extracted here is mainly commercial frequency noise, but its magnitude varies depending on the diameter of the measuring pipe and the grounding state of the pipe. Therefore, the amplification factor is made variable to easily obtain the optimum amplification degree. However, there are cases where the variable range of the amplification degree is restricted due to restrictions on circuit constants. In that case, the comparison reference voltage of the comparator is made variable to obtain the same effect.

【0008】[0008]

【実施例】以下図1および図2に基づいて本発明の実施
例を説明する。図2は本発明の一実施例としての電磁流
量計の全体構成図である。同図において、5はこの電磁
流量計全体を制御するマイクロコンピュータ、1−1は
図3で述べた測定流体8が流れる電磁流量計の測定管、
1−5は測定管1−1に設けたアース端子、1−2,1
−3は電極、1−6,1−7は直流分カット用のコンデ
ンサで、1は上記各部と励磁コイル1−4および図外の
コアとからなる電磁流量計の検出部である。
Embodiments of the present invention will be described below with reference to FIGS. FIG. 2 is an overall configuration diagram of an electromagnetic flowmeter as an embodiment of the present invention. In the figure, 5 is a microcomputer for controlling the entire electromagnetic flow meter, 1-1 is a measuring tube of the electromagnetic flow meter through which the measuring fluid 8 described in FIG. 3 flows,
1-5 is a ground terminal provided on the measuring tube 1-1, 1-2, 1
Reference numeral -3 is an electrode, 1-6 and 1-7 are capacitors for cutting a direct current component, and 1 is a detector of an electromagnetic flowmeter including the above-mentioned parts, an exciting coil 1-4 and a core not shown.

【0009】2はコンデンサ1−6,1−7を介し2つ
の電極1−2,1−3間に現れる電圧信号の増幅を行う
と共に、この増幅信号に所定の処理を行って測定管1−
1を通過する測定流体8の流量に応じた流量信号2aを
マイクロコンピュータ5に出力する増幅・信号変換回路
である。また3は夫々コンデンサ1−6,1−7を介
し、電極1−2,1−3とアース端子1−5との間に表
れる電圧信号を入力して後述のように測定管1−1内が
空状態であるか接液状態(満水状態)であるかを示す空
検出信号3aを出力する空検知回路であり、本発明の主
体となるものである。
Numeral 2 amplifies the voltage signal appearing between the two electrodes 1-2 and 1-3 via the capacitors 1-6 and 1-7, and performs a predetermined process on the amplified signal to make a measurement tube 1-.
1 is an amplification / signal conversion circuit that outputs a flow rate signal 2a corresponding to the flow rate of the measurement fluid 8 passing through 1 to the microcomputer 5. In addition, 3 inputs the voltage signal appearing between the electrodes 1-2 and 1-3 and the earth terminal 1-5 via the capacitors 1-6 and 1-7, respectively, and the inside of the measuring tube 1-1 is described later. Is an empty detection circuit that outputs an empty detection signal 3a indicating whether it is an empty state or a liquid contact state (full water state), and is the main subject of the present invention.

【0010】なお4はAC電源7から次に述べるタイミ
ングパルス発生回路6を介し、この電源7に同期した所
定レベル、所定時間幅の交番電流パルスを作り、励磁コ
イル1−4を付勢する励磁回路であり、上記タイミング
パルス発生回路6はAC電源7の電圧を入力し、マイク
ロコンピュータ5から指定された時間幅のタイミングパ
ルスを生成して励磁回路4に与える役割を持つ。
Reference numeral 4 is an AC power source 7 which, via a timing pulse generating circuit 6 described below, generates an alternating current pulse of a predetermined level and a predetermined time width in synchronization with the power source 7, and excites the exciting coils 1-4. The timing pulse generation circuit 6 has a role of inputting the voltage of the AC power supply 7 to generate a timing pulse of a time width designated by the microcomputer 5 and giving it to the excitation circuit 4.

【0011】図1は図2の空検知回路3の詳細構成を示
す。この検知回路3は大きくは加算回路3−1,非反転
増幅回路3−2,平滑回路3−3,コンパレータ3−4
から構成されている。測定管1−1の両電極1−2,1
−3とアース端子1−5との間に生じる電圧は、夫々コ
ンデンサ1−6,1−7を経て、抵抗器3−1−3,3
−1−4、オペアンプ3−1−5、抵抗器3−1−6,
3−1−7からなる加算回路3−1に入り、加算され
る。この加算回路3−1によって抽出された交流信号
は、オペアンプ3−2−1,抵抗器3−2−2,可変抵
抗器3−2−3からなる非反転増幅回路3−2によって
増幅される。この増幅回路3−2の増幅度は、可変抵抗
器3−2−3を用いることにより可変にすることができ
る。これは、測定管1−1の内径によって電極1−2,
1−3とアース端子1−5間の抽出されるノイズ電圧の
大きさが異なるので、その大きさに適した増幅度を得る
ためである。次に、この非反転増幅回路3−2によって
増幅された信号は、整流器3−3−1とコンデンサ3−
3−2,抵抗3−3−3から成る平滑回路3−3によっ
て直流信号に変換される。この直流信号はオペアンプ3
−4−1等からなるコンパレータ3−4で比較基準電圧
3−4−6と比較され、HighまたはLowのレベル
の空検出信号3aとして出力され、マイクロコンピュー
タ5に送られる。
FIG. 1 shows a detailed structure of the sky detection circuit 3 of FIG. The detection circuit 3 is roughly composed of an adder circuit 3-1, a non-inverting amplifier circuit 3-2, a smoothing circuit 3-3, and a comparator 3-4.
It consists of Both electrodes 1-2 and 1 of the measuring tube 1-1
-3 and the voltage generated between the earth terminal 1-5 pass through the capacitors 1-6 and 1-7, respectively, and the resistors 3-1-3 and 3-3.
-1-4, operational amplifier 3-1-5, resistor 3-1-6,
The addition circuit 3-1 composed of 3-1-7 is added and added. The AC signal extracted by the adder circuit 3-1 is amplified by the non-inverting amplifier circuit 3-2 including the operational amplifier 3-2-1, the resistor 3-2-2, and the variable resistor 3-2-3. . The amplification degree of the amplifier circuit 3-2 can be made variable by using the variable resistor 3-2-3. This is because the inner diameter of the measuring tube 1-1 causes the electrodes 1-2,
This is because the magnitude of the noise voltage extracted between 1-3 and the ground terminal 1-5 is different, so that the amplification degree suitable for the magnitude is obtained. Next, the signal amplified by the non-inverting amplifier circuit 3-2 is rectified by a rectifier 3-3-1 and a capacitor 3-.
It is converted into a DC signal by a smoothing circuit 3-3 composed of 3-2 and resistors 3-3-3. This DC signal is the operational amplifier 3
It is compared with the comparison reference voltage 3-4-6 by the comparator 3-4 composed of 4-1 and the like, and is output as the sky detection signal 3a at the High or Low level and sent to the microcomputer 5.

【0012】この空検出信号3aは、Highレベルの
ときを空状態、Lowレベルのときを接液(満水)状態
として識別される。またコンパレータ3−4で使われて
いる比較基準電圧3−4−6は、抵抗器3−4−2と可
変抵抗器3−4−5との比で与えられ、この比は被検出
信号の増幅度によって決められる。つまり、測定管内が
測定流体で満たされているときの平滑回路3−3の出力
圧値VL と空状態のときの同電圧値VH が以下に記す
(1)式のような関係になるように比較基準電圧
(VS )3−4−6を設定すればよい。
The sky detection signal 3a is identified as an empty state when it is at a high level and a liquid contact (full water) state when it is at a low level. The comparison reference voltage 3-4-6 used in the comparator 3-4 is given by the ratio of the resistor 3-4-2 and the variable resistor 3-4-5, and this ratio is Determined by the degree of amplification. In other words, the voltage value V H is a relationship as that following referred (1) when the output pressure value V L and the empty state of the smoothing circuit 3-3 when the measuring tube is filled with the measurement fluid the comparison reference voltage (V S) 3-4-6 may be set as.

【0013】[0013]

【数1】VL <VS <VH …………(1)[Equation 1] V L <V S <V H ………… (1)

【0014】[0014]

【発明の効果】本発明によれば、測定管1−1内の1対
の電極1−2,1−3とアース端子1−5との間に発生
する各交流信号の和を加算回路3−1により抽出して空
状態を検知するようにしたので、測定流体8が図3のよ
うに測定管1−1に存在しても確実に空状態を検知でき
る。
According to the present invention, the summing circuit 3 adds the sum of the AC signals generated between the pair of electrodes 1-2 and 1-3 in the measuring tube 1-1 and the ground terminal 1-5. Since the empty state is detected by extracting with -1, the empty state can be surely detected even if the measuring fluid 8 exists in the measuring pipe 1-1 as shown in FIG.

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

【図1】本発明の一実施例としての空検知回路の構成を
示す回路図
FIG. 1 is a circuit diagram showing a configuration of a sky detection circuit as an embodiment of the present invention.

【図2】同じく電磁流量計の全体構成を示すブロック回
路図
FIG. 2 is a block circuit diagram showing the overall configuration of the same electromagnetic flowmeter.

【図3】従来の空検知回路では誤動作を生ずる接液状態
を示す図
FIG. 3 is a diagram showing a liquid contact state in which a conventional empty detection circuit causes a malfunction.

【符号の説明】[Explanation of symbols]

1 検出部 1−1 測定管 1−2 電極 1−3 電極 1−4 励磁コイル 1−5 アース端子 1−6 直流カットコンデンサ 1−7 直流カットコンデンサ 2 増幅・信号変換回路 2a 流量信号 3 空検知回路 3a 空検出信号 3−1 加算回路 3−2 非反転増幅回路 3−2−3 可変抵抗器 3−3 平滑回路 3−4 コンパレータ 3−4−5 可変抵抗器 3−4−6 比較基準電圧 4 励磁回路 5 マイクロコンピュータ 6 タイミングパルス発生回路 7 AC電源 1 Detection Unit 1-1 Measuring Tube 1-2 Electrode 1-3 Electrode 1-4 Excitation Coil 1-5 Earth Terminal 1-6 DC Cut Capacitor 1-7 DC Cut Capacitor 2 Amplification / Signal Conversion Circuit 2a Flow Signal 3 Empty Detection Circuit 3a Empty detection signal 3-1 Adder circuit 3-2 Non-inverting amplifier circuit 3-2-3 Variable resistor 3-3 Smoothing circuit 3-4 Comparator 3-4-5 Variable resistor 3-4-6 Comparison reference voltage 4 Excitation circuit 5 Microcomputer 6 Timing pulse generation circuit 7 AC power supply

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】電磁流量計の検出器における一対の電極と
アースとの間に発生する各電圧のうちの交流分の和を抽
出してこの和に応じた加算交流信号を出力する交流分加
算抽出手段と、 該加算交流信号を直流信号に変換する直流化手段と、 前記直流信号を基準信号と比較して比較結果に応じた信
号を出力する比較手段とを備え、 前記比較手段の出力信号にもとづき前記検出器における
空状態を検知することを特徴とする電磁流量計の空検知
回路。
1. An AC component addition for extracting a sum of AC components of respective voltages generated between a pair of electrodes and a ground in a detector of an electromagnetic flow meter and outputting an addition AC signal according to the sum. An output signal of the comparison means, which comprises an extraction means, a DC conversion means for converting the added AC signal into a DC signal, and a comparison means for comparing the DC signal with a reference signal and outputting a signal according to a comparison result, An empty detection circuit for an electromagnetic flow meter, which detects an empty state in the detector based on the above.
【請求項2】請求項1に記載の空検知回路において、 前記直流信号は少なくとも第1の可変抵抗器により増幅
度が可変設定される増幅手段を経て得られるものである
ことを特徴とする電磁流量計の空検知回路。
2. The electromagnetic wave detection circuit according to claim 1, wherein the DC signal is obtained through at least an amplifying means whose amplification degree is variably set by a first variable resistor. Flow meter empty detection circuit.
【請求項3】請求項1または請求項2に記載の空検知回
路において、 前記基準信号は第2の可変抵抗器により可変設定される
ものであることを特徴とする電磁流量計の空検知回路。
3. The empty detection circuit according to claim 1 or 2, wherein the reference signal is variably set by a second variable resistor. .
JP32831092A 1992-12-09 1992-12-09 Emptiness detection circuit of electromagnetic flowmeter Pending JPH06174513A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32831092A JPH06174513A (en) 1992-12-09 1992-12-09 Emptiness detection circuit of electromagnetic flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32831092A JPH06174513A (en) 1992-12-09 1992-12-09 Emptiness detection circuit of electromagnetic flowmeter

Publications (1)

Publication Number Publication Date
JPH06174513A true JPH06174513A (en) 1994-06-24

Family

ID=18208809

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32831092A Pending JPH06174513A (en) 1992-12-09 1992-12-09 Emptiness detection circuit of electromagnetic flowmeter

Country Status (1)

Country Link
JP (1) JPH06174513A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010004193A (en) * 2008-06-19 2010-01-07 Mitsumi Electric Co Ltd Semiconductor integrated circuit device and offset cancel setting system
EP2259028A2 (en) 2009-05-28 2010-12-08 Yokogawa Electric Corporation Electromagnetic Flow Meter
JP2011209231A (en) * 2010-03-30 2011-10-20 Yamatake Corp Electromagnetic flowmeter

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010004193A (en) * 2008-06-19 2010-01-07 Mitsumi Electric Co Ltd Semiconductor integrated circuit device and offset cancel setting system
EP2259028A2 (en) 2009-05-28 2010-12-08 Yokogawa Electric Corporation Electromagnetic Flow Meter
US8433527B2 (en) 2009-05-28 2013-04-30 Yokogawa Electric Corporation Electromagnetic flow meter
JP2011209231A (en) * 2010-03-30 2011-10-20 Yamatake Corp Electromagnetic flowmeter

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