JPH09138147A - Electromagnetic flowmeter - Google Patents

Electromagnetic flowmeter

Info

Publication number
JPH09138147A
JPH09138147A JP29717595A JP29717595A JPH09138147A JP H09138147 A JPH09138147 A JP H09138147A JP 29717595 A JP29717595 A JP 29717595A JP 29717595 A JP29717595 A JP 29717595A JP H09138147 A JPH09138147 A JP H09138147A
Authority
JP
Japan
Prior art keywords
magnetic field
fluid
measured
outer core
electromotive force
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
JP29717595A
Other languages
Japanese (ja)
Inventor
Eiji Onaka
英治 大中
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 JP29717595A priority Critical patent/JPH09138147A/en
Publication of JPH09138147A publication Critical patent/JPH09138147A/en
Pending legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To provide an electromagnetic flowmeter wherein excellent workability of positioning/fixing of a lead wire is provided and the lead wire is fixed with sure, by providing a positioning recessed part and hole formed in a magnetic flux feeding-back outer core in parallel, in the circumferential direction of the outer core. SOLUTION: A coil 4 is energized by feeding from a power source, and a magnetic field is generated in the direction orthogonal to the axis of a measuring tube 1, and to-be-measured fluid 2 is moved into the measuring tube in the magnetic field, so that electromotive force is generated based on Faraday's law of electromagnetic induction. At this time, the magnetic field is generated at a right angle to the measuring tube electrically insulated, and, when conductivity of the flowing fluid is not too low, the electromotive force is measured between a pair of electrodes 5. Since the electromotive force is proportional to intensity of the magnetic field, average flow velocity of the fluid, and distance between the electrodes, flow rate can be measured by removing noise from the electromotive force, and converting into the signal corresponding to the fluid with a converter, for outputting.

Description

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

【0001】[0001]

【発明の属する技術分野】この発明は、測定管内を流れ
る被測定流体に対して交差方向に磁界を発生させ、この
磁界を横切る流体の流量に応じて発生する起電力を、上
記測定管の直径上に対向して設けられた少なくとも一対
の電極を通じて検出し、上記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 generates a magnetic field in a direction intersecting with a fluid to be measured flowing in a measuring pipe, and an electromotive force generated according to a flow rate of the fluid traversing the magnetic field is measured as a diameter of the measuring pipe. The present invention relates to an electromagnetic flow meter that measures the flow rate by detecting it through at least a pair of electrodes provided facing each other.

【0002】[0002]

【従来の技術】図6は電磁流量計50の測定原理を示す
構成図であり、図において、51は内面がテフロン等に
よってライニング処理された測定管、52は測定管1内
を流れる導電性液体である被測定流体、53は測定管5
1の外周に設けられたコア、54はそのコア53に巻か
れた磁界発生手段としてのコイル、55は測定管51の
直径上で対向し且つ磁界と交差する位置に設けられた少
なくとも一対の電極、56はその電極55によって検出
された起電力からノイズ等を取り除き、この起電力から
被測定流体52の流量に応じた信号に変換する変換器で
ある。
2. Description of the Related Art FIG. 6 is a block diagram showing the measuring principle of an electromagnetic flowmeter 50. In the figure, 51 is a measuring tube whose inner surface is lined with Teflon or the like, and 52 is a conductive liquid flowing in the measuring tube 1. Is the fluid to be measured, 53 is the measuring tube 5
1, 54 is a coil wound around the core 53 as a magnetic field generating means, and 55 is at least a pair of electrodes provided at positions facing each other on the diameter of the measuring tube 51 and intersecting the magnetic field. 56 are converters that remove noise and the like from the electromotive force detected by the electrode 55 and convert the electromotive force into a signal corresponding to the flow rate of the fluid 52 to be measured.

【0003】上記電極55に接続し磁束帰還用アウター
コア57の穴57aから取り出したたリード線58は、
図7、図8に示すように、磁束帰還用アウターコア57
の表面に、90°ノイズの発生を回避するようにスズメ
ッキ線59で位置決め固定している。ここで、90°ノ
イズとは、フレミングの右手の法則により生じる起電力
を取り出す際、リード線が図9に示すように磁束に対し
交差するような曲がり配線により生ずるもので、このノ
イズが起電力に重畳すると、正確な起電力ひいては正確
な流量が測定できない。
The lead wire 58 connected to the electrode 55 and taken out from the hole 57a of the magnetic flux feedback outer core 57 is
As shown in FIGS. 7 and 8, the magnetic flux feedback outer core 57.
A tin-plated wire 59 is positioned and fixed on the surface of the so as to avoid generation of 90 ° noise. Here, the 90 ° noise is caused by a curved wiring in which a lead wire crosses a magnetic flux as shown in FIG. 9 when an electromotive force generated by Fleming's right-hand rule is extracted, and this noise is an electromotive force. If it is superposed on, accurate electromotive force and hence accurate flow rate cannot be measured.

【0004】次に動作について説明する。不図示の電源
からの給電によってコイル54を励磁し、測定管51の
軸線と直交する方向に磁界を発生させ、この磁界内の測
定管に被測定流体52を移動させると、ファラデーの電
磁誘導の法則によって起電力を発生する。この場合、磁
界が電気的に絶縁された測定管に直角に生じ、流れてい
る被測定流体52の導電率が低すぎなければ、一対の電
極55間から起電力が測定できる。この起電力は磁界の
強さと被測定流体52の平均流速と電極間距離に比例す
るので、この起電力からノイズを取り除き、この起電力
を変換器56で被測定流体52に応じた信号に変換して
出力することにより、流量を測定できる。
Next, the operation will be described. When the coil 54 is excited by power supply from a power source (not shown), a magnetic field is generated in a direction orthogonal to the axis of the measuring tube 51, and the measured fluid 52 is moved to the measuring tube in this magnetic field. An electromotive force is generated according to the law. In this case, the magnetic field is generated at right angles to the electrically insulated measuring tube, and the electromotive force can be measured between the pair of electrodes 55 unless the electric conductivity of the flowing measured fluid 52 is too low. Since this electromotive force is proportional to the strength of the magnetic field, the average flow velocity of the fluid to be measured 52, and the distance between the electrodes, noise is removed from this electromotive force, and this electromotive force is converted by the converter 56 into a signal corresponding to the fluid to be measured 52. Then, the flow rate can be measured.

【0005】つまり、量記号および単位を次のようにす
ると、 量記号 物理量 単位 B 磁束密度 T D 測定管の内径 m v 平均軸方向流体速度 m/s E 起電力 V k 定数 ー Q 体積流量 m3 /s ファラデーの法則に従って、起電力Eの大きさは、次の
式で示される。 E=kBDv ・・・(1) 体積流量は円管測定管の場合は次の式となる。 Q=(πD2 /4)・v ・・・(2) この関係があるので、式(1)は式(3)のように表さ
れる。 Q=(πD/4kB)・E ・・・(3) ここで、磁束密度Bを一定とすると、測定管内の流量
は、起電力Eを測定することによって求められる。
That is, when the quantity symbol and the unit are as follows, quantity symbol physical quantity unit B magnetic flux density TD inner diameter of measuring tube m v average axial fluid velocity m / s E electromotive force V k constant-Q volume flow rate m According to Faraday's law of 3 / s, the magnitude of the electromotive force E is expressed by the following equation. E = kBDv (1) The volume flow rate is calculated by the following equation in the case of a circular pipe. Q = (πD 2/4) · v ··· (2) Because of this relationship, equation (1) is expressed by the equation (3). Q = (πD / 4kB) · E (3) Here, assuming that the magnetic flux density B is constant, the flow rate in the measuring tube is obtained by measuring the electromotive force E.

【0006】[0006]

【発明が解決しようとする課題】従来の電磁流量計は以
上のように構成されているので、電極55に接続したリ
ード線58は、90°ノイズを除去するために、磁束帰
還用アウターコア57の表面にスズメッキ線59で位置
決め固定されている。この結果、その取り付けを確実に
行うことが困難であると共に位置決め固定の作業性が悪
いという課題があった。
Since the conventional electromagnetic flowmeter is constructed as described above, the lead wire 58 connected to the electrode 55 has a magnetic flux feedback outer core 57 for removing 90 ° noise. The tin-plated wire 59 is positioned and fixed on the surface of the. As a result, there is a problem that it is difficult to surely perform the attachment and the workability of positioning and fixing is poor.

【0007】この発明は上記のような課題を解決するた
めになされたもので、リード線の位置決め固定の作業性
がよく、リード線を確実に固定することのできる電磁流
量計を得ることを目的とする。
The present invention has been made in order to solve the above problems, and an object thereof is to obtain an electromagnetic flow meter which has good workability in positioning and fixing lead wires and which can securely fix the lead wires. And

【0008】[0008]

【課題を解決するための手段】請求項1記載の発明に係
る電磁流量計は、被測定流体に直交する磁界を測定管内
に発生させる磁界発生手段と、前記磁界の作用により前
記被測定流体中に発生した起電力を測定するように前記
測定管の直径上で対向して設けられた少なくとも一対の
電極と、前記磁界発生手段を覆って前記測定管に固定す
る磁束帰還用アウターコアに設けた前記電極組み付け用
の第1の穴の穴縁に形成した位置決め凹部と、前記電極
に接続したリード線を前記凹部から前記磁束帰還用アウ
ターコアの内側に導入した後再び外側に取り出すように
該磁束帰還用アウターコアに形成された第2の穴とを備
え、前記位置決め凹部と第2の穴とは前記磁束帰還用ア
ウターコアの円周方向に並設したものである。
According to a first aspect of the present invention, there is provided an electromagnetic flowmeter which comprises a magnetic field generating means for generating a magnetic field orthogonal to a fluid to be measured in a measuring pipe, and an action of the magnetic field in the fluid to be measured. At least a pair of electrodes provided to face each other on the diameter of the measuring tube so as to measure the electromotive force generated in the magnetic flux feedback outer core fixed to the measuring tube to cover the magnetic field generating means. The positioning recess formed in the hole edge of the first hole for assembling the electrode and the lead wire connected to the electrode are introduced into the inside of the magnetic flux feedback outer core from the recess and then the magnetic flux is taken out again. A second hole is formed in the return outer core, and the positioning recess and the second hole are arranged side by side in the circumferential direction of the magnetic flux return outer core.

【0009】[0009]

【発明の実施の形態】以下、この発明の実施の一形態を
説明する。 実施の形態1.図1はこの発明の実施の形態1による電
磁流量計を示す一部を切断した正面図、図2はその一部
を切断した側面図、図3は電極取り付け部の正面図であ
り、図において、1は測定管、2は測定管1内を流れる
導電性液体である被測定流体、3は測定管1の外周に設
けられたコア、4はそのコア3に巻かれた磁界発生手段
としてのコイル、5は測定管1の直径上で対向し且つ磁
界と交差する位置に設けられた少なくとも一対の電極、
6は電極5に接続したリード線、7はコイル4を覆って
上記測定管1に固定する磁束帰還用アウターコア、8は
測定管1の直径範囲において磁界を平行に発生させるた
めにコイル4と測定管1との間に介在させたインナーコ
ア、9はコイル4、磁束帰還用アウターコア7、インナ
ーコア8の周囲を覆い、測定管1に溶接により固定する
ケースであり、測定管1の収容穴9−1、電極収容室9
−2等を有している。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the present invention will be described below. Embodiment 1 FIG. 1 is a partially cutaway front view showing an electromagnetic flowmeter according to Embodiment 1 of the present invention, FIG. 2 is a partially cutaway side view thereof, and FIG. 3 is a front view of an electrode mounting portion. Reference numeral 1 is a measuring tube, 2 is a fluid to be measured which is a conductive liquid flowing in the measuring tube 1, 3 is a core provided on the outer circumference of the measuring tube 1, and 4 is a magnetic field generating means wound around the core 3. Coil 5 is at least a pair of electrodes provided at positions facing each other on the diameter of measuring tube 1 and intersecting the magnetic field,
Reference numeral 6 is a lead wire connected to the electrode 5, 7 is an outer core for magnetic flux feedback which covers the coil 4 and is fixed to the measuring tube 1, and 8 is a coil 4 for generating a magnetic field in parallel in the diameter range of the measuring tube 1. An inner core interposed between the measuring tube 1 and 9 is a case that covers the coil 4, the magnetic flux feedback outer core 7 and the inner core 8 and is fixed to the measuring tube 1 by welding. Hole 9-1, electrode storage chamber 9
-2 and so on.

【0010】上記測定管1は内面および端面に耐食性、
耐摩耗性のためのライニング処理11を施してあり、そ
の端面にはケース9内の検出部と測定流体とを同電位に
する接液リング12が取り付けられている。このライニ
ング処理11の材料としては、例えばふっ素樹脂、クロ
ロプレンゴム、ポリウレタンゴム、セラミックス等を用
いる。また、接液リング12の材料としては、例えばス
テンレス鋼、白金・インジウム、タンタル、チタン、ハ
ステロイB、ハステロイC、モネル、導電性ふっ素樹脂
等を用いる。
The measuring pipe 1 has corrosion resistance on the inner surface and the end surface,
A lining treatment 11 for abrasion resistance is applied, and a liquid contact ring 12 that makes the detection portion in the case 9 and the measurement fluid have the same potential is attached to the end surface thereof. As a material for the lining treatment 11, for example, fluorine resin, chloroprene rubber, polyurethane rubber, ceramics or the like is used. Further, as the material of the liquid contact ring 12, for example, stainless steel, platinum / indium, tantalum, titanium, Hastelloy B, Hastelloy C, Monel, conductive fluororesin or the like is used.

【0011】上記電極5は、磁束帰還用アウターコアの
電極組み付け穴から挿入して、ランニング処理により形
成された受け座11aに電極棒5aの鍔座5bを当接さ
せ、この鍔座5bの他面に当接させたコイルスプリング
13を押圧しながら測定管1の電極取り付け穴1bにキ
ャップ14をねじ込んで固定している。15は電極棒3
aにリード線6を取り付けるねじ、16は測定管1の電
極収容室4cの入口にねじ込んだ蓋体である。
The electrode 5 is inserted through the electrode assembling hole of the magnetic flux feedback outer core, and the collar seat 5b of the electrode rod 5a is brought into contact with the receiving seat 11a formed by the running process. The cap 14 is screwed and fixed in the electrode mounting hole 1b of the measuring tube 1 while pressing the coil spring 13 that is brought into contact with the surface. 15 is an electrode rod 3
Reference numeral 16 is a screw for attaching the lead wire 6 to a, and 16 is a lid body screwed into the inlet of the electrode housing chamber 4c of the measuring tube 1.

【0012】図4は磁束帰還用アウターコア7の正面
図、図5は図4のV−V線に沿う縦断面図であり、電極
組み付け用の第1の穴7−1の穴縁に形成した位置決め
凹部7−1aと、電極5に接続したリード線6を前記凹
部7−1aから磁束帰還用アウターコア7の内側に導入
した後再び外側に取り出すように第2の穴7−2が形成
され、その位置決め凹部7−1aと第2の穴7−2とは
前記磁束帰還用アウターコア7の円周方向に並設されて
いる。
FIG. 4 is a front view of the magnetic flux feedback outer core 7, and FIG. 5 is a vertical sectional view taken along the line VV of FIG. 4, which is formed at the edge of the first hole 7-1 for electrode assembly. A second hole 7-2 is formed so that the positioning recess 7-1a and the lead wire 6 connected to the electrode 5 are introduced from the recess 7-1a to the inside of the magnetic flux feedback outer core 7 and then taken out again. The positioning recess 7-1a and the second hole 7-2 are arranged side by side in the circumferential direction of the magnetic flux feedback outer core 7.

【0013】次に上記の各構成部品からなる電磁流量計
の組み付け方について説明する。まず、測定管1の外周
面に軸対称にコア3を有するコイル4を設け、電極5の
リード線6を磁束帰還用アウターコア7の位置決め凹部
7−1aから該磁束帰還用アウターコアの内側に導入し
た後、穴7−2から外側に取出した後、上記コイル4を
測定管1の外面に押圧固定するように磁束帰還用アウタ
ーコア7を該測定管に取付ける。その後、測定管1を収
容穴9−1からケース9に挿入してケース9と測定管1
の接合部(両端部)を溶着する。そして、ケース9の電
極収容室9−2において、測定管1に電極5を取り付け
上記リード線6を接続するとともに、コイル4のリード
線4a、電極5のリード線6をケース9の取出し室9−
3より取出す。
Next, a method of assembling the electromagnetic flowmeter composed of the above-mentioned components will be described. First, a coil 4 having an axially symmetrical core 3 is provided on the outer peripheral surface of the measuring tube 1, and the lead wire 6 of the electrode 5 is placed from the positioning recess 7-1a of the magnetic flux feedback outer core 7 to the inside of the magnetic flux feedback outer core. After being introduced, the magnetic flux feedback outer core 7 is attached to the measuring tube 1 so that the coil 4 is pressed and fixed to the outer surface of the measuring tube 1 after being taken out from the hole 7-2. After that, the measuring tube 1 is inserted into the case 9 from the accommodation hole 9-1 and the case 9 and the measuring tube 1 are inserted.
Weld the joints (both ends). Then, in the electrode accommodating chamber 9-2 of the case 9, the electrode 5 is attached to the measuring tube 1 and the lead wire 6 is connected, and the lead wire 4a of the coil 4 and the lead wire 6 of the electrode 5 are connected to the take-out chamber 9 of the case 9. −
Take out from 3.

【0014】上記構成の電磁流量計は、測定管1の左右
に配管18a,18bに合致させて接続固定するもの
で、この接続の仕方には、フランジ接続方式、フランジ
挟み込み方式、サニタリ接続方式、ねじ接続方式の種々
の方式がある。
The electromagnetic flowmeter having the above-described structure is connected and fixed to the left and right sides of the measuring pipe 1 so as to match the pipes 18a and 18b. The connection method is a flange connection method, a flange sandwiching method, a sanitary connection method, There are various types of screw connection methods.

【0015】次に動作について説明する。不図示の電源
からの給電によってコイル4を励磁し、測定管1の軸線
と直交する方向に磁界を発生させ、この磁界内の測定管
に被測定流体2を移動させると、ファラデーの電磁誘導
の法則によって起電力を発生する。この場合、磁界が電
気的に絶縁された測定管に直角に生じ、流れている液体
の導電率が低すぎなければ、一対の電極5間から起電力
が測定できる。この起電力は磁界の強さと流体の平均流
速と電極間距離に比例するので、この起電力からノイズ
を取り除き、この起電力を前記図6に示すように変換器
56で流体に応じた信号に変換して出力することによ
り、流量を測定できる。
Next, the operation will be described. When the coil 4 is excited by power supply from a power source (not shown), a magnetic field is generated in a direction orthogonal to the axis of the measuring tube 1, and the fluid to be measured 2 is moved to the measuring tube in this magnetic field. An electromotive force is generated according to the law. In this case, a magnetic field is generated at right angles to the electrically insulated measuring tube, and if the conductivity of the flowing liquid is not too low, the electromotive force can be measured between the pair of electrodes 5. Since this electromotive force is proportional to the strength of the magnetic field, the average flow velocity of the fluid, and the distance between the electrodes, noise is removed from this electromotive force, and this electromotive force is converted into a signal corresponding to the fluid by the converter 56 as shown in FIG. The flow rate can be measured by converting and outputting.

【0016】以上のように、この実施の形態1によれ
ば、電極5に接続したリード線6を電極組み付け用の第
1の穴7−1の穴縁に形成した位置決め凹部7−1aか
ら磁束帰還用アウターコア7の内側に導入した後再び第
2の穴7−2から外側に取り出すもので、かつその位置
決め凹部7−1aと第2の穴7−2とは前記磁束帰還用
アウターコアの円周方向に並設されていることにより、
リード線6の固定と位置決めが同時に行われ、その作業
が簡単容易であり、しかもリード線6の固定が確実に行
われるという効果が得られる。
As described above, according to the first embodiment, the magnetic flux is generated from the positioning recess 7-1a formed at the edge of the first hole 7-1 for assembling the electrode with the lead wire 6 connected to the electrode 5. After being introduced inside the return outer core 7, it is taken out again from the second hole 7-2, and the positioning recess 7-1a and the second hole 7-2 are the same as those of the magnetic flux return outer core. By being arranged side by side in the circumferential direction,
The fixing and positioning of the lead wire 6 are performed at the same time, and the work is simple and easy, and further, the lead wire 6 is reliably fixed.

【0017】[0017]

【発明の効果】以上のように、請求項1記載の発明によ
れば、電極に接続したリード線を電極組み付け用の第1
の穴の穴縁に形成した位置決め凹部から磁束帰還用アウ
ターコアの内側に導入した後再び第2の穴から外側に取
り出し、その位置決め凹部と第2の穴とは前記磁束帰還
用アウターコアの円周方向に並設して構成したので、リ
ード線の固定と位置決めが同時に行われ、その作業が簡
単容易であり、しかもリード線は磁束と平行に配設され
ので、90°ノイズの発生を確実に防止することができ
るととも固定が確実に行われる。そして、電磁流量計の
長期使用に伴う測定流体の脈動によって生じる振動によ
ってリード線の破断が凹部のエッジ部に限定されるた
め、メンテナンス時にリード線の破断を確認しやすい等
の効果がある。
As described above, according to the first aspect of the present invention, the lead wire connected to the electrode is used as the first electrode for assembling the electrode.
After being introduced into the inside of the magnetic flux feedback outer core from the positioning recess formed in the hole edge of the hole, the positioning recess and the second hole are taken out again from the second hole, and the positioning recess and the second hole are circles of the magnetic flux feedback outer core. Since they are arranged side by side in the circumferential direction, the fixing and positioning of the lead wire can be performed at the same time, the work is easy and easy, and the lead wire is arranged in parallel with the magnetic flux, so that 90 ° noise is surely generated. It can be prevented and the fixing is surely performed. Further, since the breakage of the lead wire is limited to the edge portion of the recess due to the vibration caused by the pulsation of the measured fluid due to the long-term use of the electromagnetic flow meter, it is easy to confirm the breakage of the lead wire during maintenance.

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

【図1】この発明の実施の一形態による電磁流量計を示
す一部を切断した正面図である。
FIG. 1 is a partially cutaway front view showing an electromagnetic flowmeter according to an embodiment of the present invention.

【図2】その電磁流量計の一部を切断した右側面図であ
る。
FIG. 2 is a right side view in which a part of the electromagnetic flow meter is cut away.

【図3】電極取り付け部の正面図である。FIG. 3 is a front view of an electrode mounting portion.

【図4】リード線を取り付けた磁束帰還用アウターコア
の正面図である。
FIG. 4 is a front view of a magnetic flux feedback outer core to which a lead wire is attached.

【図5】図4のV−V線に沿う縦断面図である。FIG. 5 is a longitudinal sectional view taken along the line VV of FIG. 4;

【図6】電磁流量計の測定原理を説明する概略構成図で
ある。
FIG. 6 is a schematic configuration diagram illustrating a measurement principle of an electromagnetic flow meter.

【図7】従来の電磁流量計におけるリード線を取り付け
た磁束帰還用アウターコアの正面図である。
FIG. 7 is a front view of a magnetic flux feedback outer core to which a lead wire is attached in a conventional electromagnetic flowmeter.

【図8】図7のXIII−XIII線に沿う縦断面図で
ある。
8 is a vertical cross-sectional view taken along the line XIII-XIII in FIG.

【図9】90°ノイズの説明図である。FIG. 9 is an explanatory diagram of 90 ° noise.

【符号の説明】[Explanation of symbols]

1 測定管 2 被測定流体 4 コイル(磁界発生手段) 5 電極 6 リード線 7 磁束帰還用アウターコア 7−1 第1の穴 7−1a 凹部 7−2 第2の穴 1 Measuring Tube 2 Fluid to be Measured 4 Coil (Magnetic Field Generating Means) 5 Electrode 6 Lead Wire 7 Outer Core for Flux Return 7-1 First Hole 7-1a Recess 7-2 Second Hole

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 被測定流体を通す測定管と、前記被測定
流体に直交する磁界を前記測定管内に発生させる磁界発
生手段と、前記磁界作用により前記被測定流体中に発生
した起電力を測定するように前記測定管の直径上で対向
して設けられた少なくとも一対の電極と、前記磁界発生
手段を覆って前記測定管に固定する磁束帰還用アウター
コアと、前記磁束帰還用アウターコアに設けた前記電極
組み付け用の第1の穴の穴縁に形成した位置決め凹部
と、前記電極に接続したリード線を前記凹部から前記磁
束帰還用アウターコアの内側に導入した後再び外側に取
り出すように該磁束帰還用アウターコアに形成された第
2の穴とを備え、前記位置決め凹部と第2の穴とは前記
磁束帰還用アウターコアの円周方向に並設したことを特
徴とする電磁流量計。
1. A measuring pipe through which a fluid to be measured is passed, a magnetic field generating means for generating a magnetic field perpendicular to the fluid to be measured in the measuring pipe, and an electromotive force generated in the fluid to be measured by the magnetic field action is measured. As described above, at least a pair of electrodes provided to face each other on the diameter of the measurement tube, a magnetic flux feedback outer core that covers the magnetic field generating means and is fixed to the measurement tube, and a magnetic flux feedback outer core are provided. The positioning recess formed in the hole edge of the first hole for assembling the electrode and the lead wire connected to the electrode are introduced from the recess to the inside of the magnetic flux feedback outer core and then taken out again to the outside. An electromagnetic flowmeter, comprising: a second hole formed in the magnetic flux returning outer core, wherein the positioning recess and the second hole are arranged side by side in the circumferential direction of the magnetic flux returning outer core.
JP29717595A 1995-11-15 1995-11-15 Electromagnetic flowmeter Pending JPH09138147A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29717595A JPH09138147A (en) 1995-11-15 1995-11-15 Electromagnetic flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29717595A JPH09138147A (en) 1995-11-15 1995-11-15 Electromagnetic flowmeter

Publications (1)

Publication Number Publication Date
JPH09138147A true JPH09138147A (en) 1997-05-27

Family

ID=17843156

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29717595A Pending JPH09138147A (en) 1995-11-15 1995-11-15 Electromagnetic flowmeter

Country Status (1)

Country Link
JP (1) JPH09138147A (en)

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