JP3335822B2 - Electromagnetic flow meter - Google Patents

Electromagnetic flow meter

Info

Publication number
JP3335822B2
JP3335822B2 JP29717495A JP29717495A JP3335822B2 JP 3335822 B2 JP3335822 B2 JP 3335822B2 JP 29717495 A JP29717495 A JP 29717495A JP 29717495 A JP29717495 A JP 29717495A JP 3335822 B2 JP3335822 B2 JP 3335822B2
Authority
JP
Japan
Prior art keywords
magnetic field
coil
fluid
magnetic flux
measured
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 - Lifetime
Application number
JP29717495A
Other languages
Japanese (ja)
Other versions
JPH09138146A (en
Inventor
進吾 小松
▲つとむ▼ 後藤
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 JP29717495A priority Critical patent/JP3335822B2/en
Publication of JPH09138146A publication Critical patent/JPH09138146A/en
Application granted granted Critical
Publication of JP3335822B2 publication Critical patent/JP3335822B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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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 relates to a method for generating a magnetic field in a cross direction with respect to a fluid to be measured flowing in a measuring tube, and generating an electromotive force generated in accordance with a flow rate of the fluid traversing the magnetic field with a diameter of the measuring tube. The present invention relates to an electromagnetic flowmeter that detects the above flow rate through at least a pair of electrodes provided to face each other and measures the flow rate.

【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 measurement principle of an electromagnetic flowmeter 50. In the figure, reference numeral 51 denotes a measuring tube whose inner surface is lined with Teflon or the like, and 52 denotes a conductive liquid flowing through the measuring tube 1. Is the fluid to be measured, and 53 is the measuring tube 5
A core 54 provided on the outer periphery of the reference numeral 1 is a coil as a magnetic field generating means wound around the core 53, 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. And 56 are converters for removing noise and the like from the electromotive force detected by the electrode 55 and converting the electromotive force into a signal corresponding to the flow rate of the fluid 52 to be measured.

【0003】図7は従来の電磁流量計のコイル54と、
このコイル54を覆って上記測定管51に固定する磁束
帰還用アウターコア57との関係を示す概要図であり、
コイル54は測定管の外周に沿う円弧状の磁束帰還用ア
ウターコア57により測定管51の表面に押圧固定され
ている。
FIG. 7 shows a coil 54 of a conventional electromagnetic flow meter,
FIG. 4 is a schematic diagram showing a relationship with a magnetic flux feedback outer core 57 that covers the coil 54 and is fixed to the measurement tube 51;
The coil 54 is pressed and fixed to the surface of the measurement tube 51 by an arc-shaped outer core 57 for magnetic flux feedback along the outer circumference of the measurement tube.

【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を励磁すると、コア53
を通じて測定管51の軸線と直交する方向に磁界φが発
生する。この磁界内の測定管51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φが電気的に絶縁された
測定管51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φ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もので、この起
電力を計測することによって流量を測定できる。
Next, the operation will be described. When the coil 54 is excited by power supply from a power source (not shown), the core 53
, A magnetic field φ is generated in a direction orthogonal to the axis of the measuring tube 51. When the fluid 52 to be measured is moved to the measurement tube 51 in the magnetic field, an electromotive force is generated according to Faraday's law of electromagnetic induction. In this case, if the magnetic field φ is generated at right angles to the electrically insulated measurement tube 51 and the electric conductivity of the fluid 52 to be measured is not too low, the electromotive force can be measured between the pair of electrodes 55. The electromotive force is proportional to the strength of the magnetic field φ, the average flow velocity of the fluid 52 to be measured, and the distance between the electrodes. By measuring the electromotive force, 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 − 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 unit are as follows, quantity symbol physical quantity unit B magnetic flux density TD inner diameter of measurement tube mv average axial fluid velocity m / s E electromotive force Vk constant-Q volume flow rate m According to the 3 / s Faraday's law, the magnitude of the electromotive force E is represented by the following equation. E = kBDv (1) The volume flow rate is given by the following equation in the case of a circular measuring tube. Q = (πD 2/4) · v ··· (2) Because of this relationship, equation (1) is expressed by the equation (3). Q = (πD / 4 kB) · E (3) Here, assuming that the magnetic flux density B is constant, the flow rate in the measurement tube can be 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、コイル54は測定管5
1の外周に沿う磁束帰還用アウターコア57の寸法によ
り幅寸法Wが規定されるため、この幅寸法Wを規定寸法
とするためにコイルの巻き数を制限すると性能が落ち
る。一方性能を確保するために巻き数を確保すると、コ
イル自体の長さ(縦方向)が長くなり、その結果、電磁
流量計全体の長さが長くなり、小型化を達成できないと
いう課題があった。
Since the conventional electromagnetic flowmeter is configured as described above, the coil 54 is connected to the measuring tube 5.
Since the width W is defined by the size of the magnetic flux feedback outer core 57 along the outer circumference of 1, the performance decreases when the number of turns of the coil is limited in order to make the width W the specified size. On the other hand, if the number of windings is secured to ensure performance, the length of the coil itself (longitudinal direction) becomes longer, and as a result, the overall length of the electromagnetic flowmeter becomes longer, and there is a problem that miniaturization cannot be achieved. .

【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、全体形状を小さくしつつコイルの
巻き数を増やし、磁束を十分発生させ、性能向上を図る
ことのできる電磁流量計を得ることを目的とする。
SUMMARY OF THE INVENTION The present invention has been made to solve the above-described problems, and an electromagnetic flowmeter capable of increasing the number of windings of a coil while reducing the overall shape, sufficiently generating magnetic flux, and improving performance. The purpose is to obtain.

【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
電極とを備え、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該磁界発生手段との
干渉逃げ部の機能を持つと共に前記電極と結線された内
部のリード線の配線状態を外部から確認可能な窓部の機
能を併せ持つ穴とを設けたものである。
According to the present invention, there is provided an electromagnetic flowmeter, comprising: a magnetic field generating means for generating a magnetic field perpendicular to a fluid to be measured in a measuring pipe; 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 outer core for magnetic flux feedback fixed to the measuring tube covering the magnetic field generating means. It has a function of an escape part for the magnetic field generating means and is connected to the electrode.
Window machine that allows externally checking the wiring status of the lead wires
It is provided with a hole having both functions .

【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は図1のIII−III線に沿
う横断平面図である。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5の収容室9−2等を有する。
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 a first embodiment of the present invention, FIG. 2 is a partially cutaway side view, and FIG. 3 is a cross-sectional plane taken along line III-III in FIG. FIG. In the figure, 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 periphery of the measuring tube 1, 4 is a magnetic field generating means wound around the core 3 5, at least one pair of electrodes provided at positions facing each other on the diameter of the measuring tube 1 and intersecting the magnetic field; 6, a lead wire connected to the electrode 5; An outer core for magnetic flux feedback fixed to 1, 8 is an inner core interposed between the coil 4 and the measuring tube 1 to generate a magnetic field in parallel in the diameter range of the measuring tube 1, 9 is a coil 4, and a magnetic flux feedback Is a case that covers the periphery of the outer core 7 and the inner core 8 and is fixed to the measuring tube 1 by welding.
1, an accommodation room 9-2 for the electrode 5 and the like.

【0010】上記磁束帰還用アウターコア7には、図4
に示すようにコイル4の表面両側部に対向する部分に該
コイルの干渉逃げ部としての穴7a,7bが設けられて
おり、コイル4の表面を測定管1に押圧した状態で該測
定管にねじ10で取り付けられている。
The outer core 7 for magnetic flux feedback has a structure shown in FIG.
As shown in FIG. 3, holes 7a and 7b as interference escape portions of the coil 4 are provided at portions facing both sides of the surface of the coil 4, and the surface of the coil 4 is pressed against the measurement tube 1 in a state where the coil 4 is pressed against the measurement tube 1. It is attached with screws 10.

【0011】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 tube 1 has an inner surface and an end surface having corrosion resistance,
A lining treatment 11 for abrasion resistance is applied, and a liquid contact ring 12 for making a detection portion in the case 9 and a measurement fluid the same potential is attached to an end surface thereof. As a material of the lining treatment 11, for example, fluororesin, chloroprene rubber, polyurethane rubber, ceramics, or the like is used. 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.

【0012】上記電極5は、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、17は測定管1の電
極収容室9−2の入口にねじ込んだ蓋体である。
The electrode 5 is measured while the flange 5b of the electrode rod 5a is in contact with the receiving seat 11a formed by the running process, and the coil spring 13 which is in contact with the other surface of the flange 5b is pressed. The cap 14 is screwed and fixed in the electrode mounting hole 1b of the tube 1. 15 is the electrode rod 3
Reference numeral 17 denotes a screw for attaching the lead wire 6 to a, and 17 denotes a lid screwed into the entrance of the electrode accommodating chamber 9-2 of the measuring tube 1.

【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、このコイル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1に取り付ける。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5の収容室9−2において、測定管1に電極5を
取り付けるとともに、コイル4、電極5の各リード線4
a,6をケース9の取出し室9−3から取出す。
Next, a method of assembling the electromagnetic flow meter including the above-described components will be described. First, a coil 4 having an axially symmetrical core 3 on the outer peripheral surface of the measuring tube 1, and a 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. Then, measuring tube 1
Is inserted into the case 9 through the accommodation hole 9-1 and the joints (both ends) of the case 9 and the measuring tube 1 are welded. And case 9
The electrode 5 is attached to the measuring tube 1 in the accommodating chamber 9-2 of the electrode 5, and the coil 4 and each lead wire 4
a, 6 are taken out of the take-out chamber 9-3 of the case 9.

【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 flow meter having the above-described structure is connected and fixed to the right and left sides of the measuring pipe 1 so as to match the pipes 18a and 18b. The connecting method includes a flange connection method, a flange sandwiching method, a sanitary connection method, and the like. 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) to generate a magnetic field in a direction perpendicular to the axis of the measuring tube 1, and the fluid 2 to be measured is moved to the measuring tube in the magnetic field, the Faraday electromagnetic induction An electromotive force is generated according to the law. In this case, if a magnetic field is generated at right angles to the electrically insulated measuring tube and the conductivity of the flowing liquid is not too low, the electromotive force can be measured from between the pair of electrodes 5. Since the 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 the electromotive force, and the electromotive force is converted into a signal corresponding to the fluid by the converter 56 as shown in FIG. By converting and outputting, the flow rate can be measured.

【0016】以上のように、この実施の形態1によれ
ば、コイルを覆って該コイルを測定管1に固定する磁束
帰還用アウターコア7に、前記コイル4との穴7a,7
bを設けたので、ケース9の大きさを小さくして、磁束
帰還用アウターコア7の円弧が小さくなっても、コイル
4の両側部は穴7a,7bから外部に突出し、何ら寸法
規制を受けないので、コイル4の取り付けに支障を生ず
ることがなく、コイル4の巻き数を増して、磁束を十分
発生させ、性能向上を図ることができる効果が得られ
る。
As described above, according to the first embodiment, the holes 7a, 7 with the coil 4 are provided in the outer core 7 for magnetic flux feedback which covers the coil and fixes the coil to the measuring tube 1.
Since the case b is provided, even if the size of the case 9 is reduced and the arc of the magnetic flux return outer core 7 is reduced, both side portions of the coil 4 protrude to the outside from the holes 7a and 7b and are subject to any size restrictions. Since there is no problem, there is no problem in mounting the coil 4, and the number of turns of the coil 4 can be increased to generate sufficient magnetic flux, thereby improving the performance.

【0017】また、穴7a,7bを窓部とすることによ
り、電極5に接続されたリード線6の引き出し状態を外
部より見ることができる。その結果、図5に示すように
リード線6が磁束に対し交差するような曲がり配線によ
る90°ノイズの信号への重畳を確実に回避することが
できる。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、ノイズが重畳
し、正確な起電力ひいては正確な流量が測定できないこ
とである。
Further, by using the holes 7a and 7b as windows, it is possible to externally see the lead-out state of the lead wire 6 connected to the electrode 5. As a result, as shown in FIG. 5, it is possible to reliably avoid the superposition of the 90 ° noise on the signal by the bent wiring in which the lead wire 6 crosses the magnetic flux. Here, 90 ° noise refers to the fact that when extracting an electromotive force generated by the Fleming's right-hand rule, noise is superimposed, and an accurate electromotive force and thus an accurate flow rate cannot be measured.

【0018】[0018]

【発明の効果】以上のように、請求項1記載の発明によ
れば、コイルを覆って該コイルを測定管に固定する磁束
帰還用アウターコアに、前記コイルとの干渉逃げ部の機
能を持つと共に前記電極と結線された内部のリード線の
配線状態を外部から確認可能な窓部の機能を併せ持つ穴
を設けて構成したので、磁束帰還用アウターコアの円
弧寸法が小さくなっても、コイル4の両側部は干渉逃げ
部から外部に突出し何ら寸法規制を受けない。従って、
コイルの巻き数を増しても該コイルの取り付けに支障を
生ずることがなく、磁束を十分に発生させ、性能向上を
図ることができるとともに、リード線の配線状態を外部
より見ることができるため、リード線の曲がり配線によ
る90°ノイズの信号への重畳を確実に回避できるとと
もにリード線の配線自体も容易であるという効果があ
る。
As is evident from the foregoing description, according to the first aspect of the invention, the outer core flux feedback over the coil to fix the coil to the measuring tube, the machine interference relief portion of said coil
Of the internal lead wire connected to the electrode
A hole that also has a window function that allows you to check the wiring status from the outside
Since it is configured by providing the door, even if the arc dimension of the outer core for flux return is reduced, both side portions of the coil 4 is not subject to any dimensional restriction protruding outward from the interference relief portion. Therefore,
Even if the number of turns of the coil is increased, there is no problem in mounting the coil, sufficient magnetic flux can be generated, performance can be improved, and the wiring state of the lead wire can be seen from the outside. There is an effect that the superposition of 90 ° noise on the signal due to the bent wiring of the lead wire can be reliably avoided and the wiring of the lead wire itself is easy.

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

【図1】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である。
FIG. 1 is a partially cutaway front view showing an electromagnetic flow meter according to Embodiment 1 of the present invention.

【図2】その電磁流量計を示す一部を切断した側面図で
ある。
FIG. 2 is a partially cut-away side view showing the electromagnetic flow meter.

【図3】図2のIII−III線に沿う横断平面図であ
る。
FIG. 3 is a cross-sectional plan view taken along the line III-III of FIG. 2;

【図4】磁束帰還用アウターコアとコイルとの関係を示
す側面図である。
FIG. 4 is a side view showing a relationship between a magnetic flux feedback outer core and a coil.

【図5】測定管に対するリード線の取り出し状態を示す
斜視図である。
FIG. 5 is a perspective view showing a state in which a lead wire is taken out of a measurement tube.

【図6】電磁流量計の原理を説明する図である。FIG. 6 is a diagram illustrating the principle of an electromagnetic flow meter.

【図7】従来の電磁流量計の磁束帰還用アウターコアと
コイルとの関係を示す側面図である。
FIG. 7 is a side view showing a relationship between a magnetic flux feedback outer core and a coil of a conventional electromagnetic flowmeter.

【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 7 磁束帰還用アウターコア 7a,7b 穴(干渉逃げ部) DESCRIPTION OF SYMBOLS 1 Measuring pipe 2 Fluid to be measured 4 Coil (magnetic field generating means) 5 Electrode 7 Outer core for magnetic flux feedback 7a, 7b Hole (interference relief part)

───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.7,DB名) G01F 1/58 ──────────────────────────────────────────────────続 き Continued on front page (58) Field surveyed (Int.Cl. 7 , DB name) G01F 1/58

Claims (1)

(57)【特許請求の範囲】(57) [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
ーコアとを備えた電磁流量計において、前記磁束帰還用
アウターコアに前記磁界発生手段との干渉逃げ部の機能
を持つと共に前記電極と結線された内部のリード線の配
線状態を外部から確認可能な窓部の機能を併せ持つ穴と
を備え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 passes, a magnetic field generating means for generating a magnetic field orthogonal to the fluid to be measured in the measuring pipe, and an electromotive force generated in the fluid to be measured by the action of the magnetic field. In an electromagnetic flowmeter including at least a pair of electrodes provided to face each other on the diameter of the measurement tube so as to measure, and an outer core for magnetic flux feedback fixed to the measurement tube covering the magnetic field generating means, A function of an interference relief portion between the magnetic flux generating outer core and the magnetic flux feedback outer core
And the internal lead wires connected to the electrodes.
An electromagnetic flowmeter comprising: a hole having a function of a window part capable of confirming a line state from the outside .
JP29717495A 1995-11-15 1995-11-15 Electromagnetic flow meter Expired - Lifetime JP3335822B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29717495A JP3335822B2 (en) 1995-11-15 1995-11-15 Electromagnetic flow meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29717495A JP3335822B2 (en) 1995-11-15 1995-11-15 Electromagnetic flow meter

Publications (2)

Publication Number Publication Date
JPH09138146A JPH09138146A (en) 1997-05-27
JP3335822B2 true JP3335822B2 (en) 2002-10-21

Family

ID=17843142

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29717495A Expired - Lifetime JP3335822B2 (en) 1995-11-15 1995-11-15 Electromagnetic flow meter

Country Status (1)

Country Link
JP (1) JP3335822B2 (en)

Also Published As

Publication number Publication date
JPH09138146A (en) 1997-05-27

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