JPH09138148A - Electromagnetic flowmeter - Google Patents

Electromagnetic flowmeter

Info

Publication number
JPH09138148A
JPH09138148A JP29717695A JP29717695A JPH09138148A JP H09138148 A JPH09138148 A JP H09138148A JP 29717695 A JP29717695 A JP 29717695A JP 29717695 A JP29717695 A JP 29717695A JP H09138148 A JPH09138148 A JP H09138148A
Authority
JP
Japan
Prior art keywords
magnetic field
core
measuring tube
measured
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.)
Pending
Application number
JP29717695A
Other languages
Japanese (ja)
Inventor
Eiji Onaka
英治 大中
Atsushi Nemoto
敦之 根本
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 JP29717695A priority Critical patent/JPH09138148A/en
Publication of JPH09138148A publication Critical patent/JPH09138148A/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To provide a light electromagnetic flowmeter of low cost by generating an uniform magnetic field at a right angle to the axis of a measuring tube, while the size of a core is limited by the size of a coil. SOLUTION: A coil 4 is energized by feeding from a power source, so that, by a core 3 and an inner core 8, a magnetic field is generated in the direction orthogonal to the axis of a measuring tube 1. When to-be-measured fluid 2 is moved into the measuring tube 1 in the magnetic field, 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 part of electrodes 5. A core mounting flat surface part of a magnetic field generating means is provided to the central part of inner core for constitution, so that, by fixing the core to the flat surface part, the core can be assigned in parallel to the axis of the measurement tube, so that, the magnetic field orthogonal to the axis is uniformly generated, and the effect that flow rate measurement is performed with precision is obtained.

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4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51
内を流れる導電性液体である被測定流体、53は測定管
51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. 4 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 measuring tube 51.
A fluid to be measured which is a conductive liquid flowing therein, 53 is a core provided on the outer periphery of the measuring tube 51, 54 is a coil wound around the core 53 as a magnetic field generating means, and 55 is the measuring tube 51.
At least a pair of electrodes, which are provided at positions facing each other on the diameter of and intersecting the magnetic field, remove noise and the like from the electromotive force detected by the electrode 55, and according to the flow rate of the fluid 52 to be measured from this electromotive force. It is a converter for converting into a signal.

【0003】図5は従来の電磁流量計における測定管5
1に対するコア53、コイル54の取り付け状態を示す
概要図(コア53、コイル54は測定管51に軸対称に
設けるが、図示例はその片側だけを示す)であり、測定
管51の外周面に軸対象に円弧状のインナーコア57を
設け、そのインナーコアの中央部に円弧状のくら型のコ
ア53を設け、このコア53の周囲にコイル54を装着
したものである。
FIG. 5 shows a measuring tube 5 in a conventional electromagnetic flow meter.
1 is a schematic view showing a mounting state of a core 53 and a coil 54 with respect to No. 1 (the core 53 and the coil 54 are axially symmetrical to the measuring pipe 51, but the illustrated example shows only one side thereof), and the outer peripheral surface of the measuring pipe 51 is shown. An arc-shaped inner core 57 is provided on the axis, an arcuate paddle-shaped core 53 is provided in the center of the inner core, and a coil 54 is mounted around the core 53.

【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、コイルの巻き付け固定
はコアの側面を利用しており、コアの大きさはコイルの
大きさによって決められる。このため、コアは効率以上
の寸法が必要となり、重量が重く、コストアップとな
る。また、このコアは測定管周面に取り付けたインナー
コアに沿って円弧状のくら型コアに構成しなければなら
ないが、コアの厚みが厚いため、円弧状に制作すること
が面倒であるとともに測定管の軸線に対する平行度が保
てず、測定管の軸線に対し直交する磁界を均一に発生で
きない。しかも、コアはコイル寸法に合わせて異なるコ
アを用意しなければならず、製品管理上面倒である等の
課題があった。
Since the conventional electromagnetic flow meter is constructed as described above, the coil is wound and fixed by using the side surface of the core, and the size of the core is determined by the size of the coil. To be For this reason, the core is required to have a size larger than the efficiency, resulting in a heavy weight and an increase in cost. Also, this core must be configured as an arcuate paddle core along the inner core attached to the peripheral surface of the measuring tube, but since the core is thick, it is troublesome to make it in an arcuate shape and to measure. The parallelism with the axis of the tube cannot be maintained and a magnetic field orthogonal to the axis of the measuring tube cannot be generated uniformly. In addition, different cores have to be prepared according to the coil size, and there has been a problem that product management is obscure.

【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、コアの大きさがコイル寸法に制約
されることなく、測定管の軸線と直交して均一磁界を発
生させることができる軽量で安価な電磁流量計を得るこ
とを目的とする。
The present invention has been made to solve the above problems, and it is possible to generate a uniform magnetic field at right angles to the axis of the measuring tube without the size of the core being restricted by the coil size. The purpose is to obtain a lightweight and inexpensive electromagnetic flowmeter that can be used.

【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、被測定流体を通す測定管に直交する磁
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、前記測定管と前記磁界発生手
段との間に設けられたインナーコアとを備え、前記イン
ナーコアの中央部に前記磁界発生手段のコア載置平面部
を設けたものである。
An electromagnetic flowmeter according to the invention described in claim 1 is characterized by a magnetic field generating means for generating a magnetic field in the measuring pipe, the magnetic field being orthogonal to the measuring pipe through which the fluid to be measured is passed, and the action of the magnetic field. 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 fluid to be measured, and an inner provided between the measuring tube and the magnetic field generating means. A core, and the core mounting plane portion of the magnetic field generating means is provided in the central portion of the inner core.

【0009】請求項2記載の発明に係る電磁流量計は、
被測定流体を通す測定管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、前記測定管と前記磁界発生手段との間に設けら
れたインナーコアとを備え、前記インナーコアに前記磁
界発生手段のコイルを位置決め固定する立ち上げ部を設
けたものである。
The electromagnetic flowmeter according to the second aspect of the invention is
On the diameter of the measuring tube so as to measure the electromotive force generated in the measured fluid by the action of the magnetic field, a magnetic field generating means for generating in the measuring tube a magnetic field orthogonal to the measuring tube through which the fluid to be measured is passed. A rising portion including at least a pair of electrodes provided to face each other and an inner core provided between the measuring tube and the magnetic field generating means, and positioning and fixing a coil of the magnetic field generating means to the inner core. Is provided.

【0010】[0010]

【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
を切断した側面図であり、図1、2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
の間に設けたインナーコア、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 Embodiment 1 of the present invention, and FIG. 2 is a partially cutaway side view thereof. In FIGS. 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, 4 is a coil wound around the core 3 as a magnetic field generating means, 5 is the measuring tube 1 At least a pair of electrodes provided at positions facing each other on the diameter of and crossing the magnetic field, 6 is a lead wire connected to the electrode 5, and 7 is an outer core for magnetic flux feedback that covers the coil 4 and is fixed to the measuring tube 1. , 8 is an inner core provided between the coil 4 and the measuring tube 1 in order to generate a magnetic field in parallel in the diameter range of the measuring tube 1, 9 is a periphery of the coil 4, the magnetic flux feedback outer core 7 and the inner core 8. With a case that covers the Ri, accommodation hole 9-1 of the measuring tube 1, has an accommodating chamber 9-2 of the electrode 5.

【0011】図3はコア3とインナーコア8との関係図
を示すもので、図3(a)は正面図、図3(b)は平面
図である。インナーコア8はその中央部に前記磁界発生
手段のコア載置平面部8−1を、その平面部8−1の周
囲に前記磁界発生手段のコイル4を位置決め固定する立
ち上げ部8−2a,8−2bを設けている。そして、コ
ア3は平面部8−1に載置しねじ10で固定し、コイル
4は立ち上げ部8−2a,8−2bを巻き芯として巻き
付け固定する。
3A and 3B are views showing the relationship between the core 3 and the inner core 8. FIG. 3A is a front view and FIG. 3B is a plan view. The inner core 8 has a core mounting flat surface portion 8-1 of the magnetic field generating means at the center thereof, and a rising portion 8-2a for positioning and fixing the coil 4 of the magnetic field generating means around the flat surface portion 8-1. 8-2b is provided. Then, the core 3 is placed on the flat surface portion 8-1 and fixed by the screw 10, and the coil 4 is fixed by winding the rising portions 8-2a and 8-2b as winding cores.

【0012】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 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.

【0013】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5
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 by abutting the collar seat 5b of the electrode rod 5a on the receiving seat 11a formed by the running process and pressing the coil spring 13 abutting on the other surface of the collar seat 5b. A cap 14 is screwed into and fixed to the electrode mounting hole 1b of the tube 1. 15 is an electrode rod 5
Reference numeral 17 denotes a screw for attaching the lead wire 6 to a, and 17 denotes a lid body screwed into the inlet of the electrode housing chamber 9-2 of the measuring tube 1.

【0014】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
面に軸対称にインナーコア8、このインナーコア8の平
面部8−1にコア3を載置し、インナーコア8の立ち上
げ部8−2a,8−2bにコイル4を巻き付け、これら
全体を測定管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の取り出し室9−3より取り出す。
Next, a method of assembling the electromagnetic flowmeter composed of the above-mentioned components will be described. First, the inner core 8 is placed axially symmetrically on the outer peripheral surface of the measuring tube 1, the core 3 is placed on the flat surface portion 8-1 of the inner core 8, and the rising portions 8-2a and 8-2b of the inner core 8 are coiled. 4 is wound, and a magnetic flux feedback outer core 7 is attached to the measuring tube 1 so as to press and fix the whole on the outer surface of the measuring tube 1. After that, the measuring tube 1 is inserted into the case 9 through the accommodation hole 9-1 and the joint portion (both ends) of the case 9 and the measuring tube 1 is welded. Then, in the electrode housing chamber 9-2 of the case 9, the electrode 5 is attached to the measuring tube 1 and the coil 4 and each lead wire 4 of the electrode 5 are attached.
The a and 6 are taken out from the take-out chamber 9-3 of the case 9.

【0015】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-mentioned 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.

【0016】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を励磁すると、コア3、イ
ンナーコア8のによって測定管1の軸線と直交する方向
に磁界が発生する。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4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 feeding power from a power source (not shown), a magnetic field is generated by the core 3 and the inner core 8 in a direction orthogonal to the axis of the measuring tube 1. Fluid to be measured 2 in the measuring tube in this magnetic field
When is moved, an electromotive force is generated by Faraday's law of electromagnetic induction. 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.

【0017】以上のように、この実施の形態1によれ
ば、インナーコア8の平面部8−1にコア3を取り付
け、その平面部8−1の両側の立ち上がり部8−2a,
8−2bを巻き芯としてコイル4を巻き付けることによ
り、コア3はコイル4の寸法に制約されることなく適正
な寸法に設計でき、コアの共通化が可能となり、製品管
理が容易となったった。また、コア3は測定管1の軸線
と平行に配設できることになり、軸線と直交した磁界を
均一に発生させることができる等の効果が得られる。
As described above, according to the first embodiment, the core 3 is attached to the flat surface portion 8-1 of the inner core 8 and the rising portions 8-2a on both sides of the flat surface portion 8-1.
By winding the coil 4 around the winding core 8-2b, the core 3 can be designed to have an appropriate size without being restricted by the size of the coil 4, the core can be shared, and product management becomes easy. Further, since the core 3 can be arranged parallel to the axis of the measuring tube 1, it is possible to obtain an effect such that a magnetic field orthogonal to the axis can be generated uniformly.

【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、インナーコアの中央部に前記磁界発生手段のコア
載置平面部を設けて構成したので、上記平面部にコアを
取り付けることにより、コアは測定管の軸線と平行に配
設できることになり、軸線と直交した磁界を均一に発生
させることができ、流量計測を精度よくできる効果が得
られる。
As described above, according to the first aspect of the present invention, the core mounting plane portion of the magnetic field generating means is provided in the central portion of the inner core, so that the core is attached to the plane portion. As a result, the core can be arranged in parallel with the axis of the measuring tube, the magnetic field orthogonal to the axis can be uniformly generated, and the effect of accurately measuring the flow rate can be obtained.

【0019】請求項2記載の発明によれば、インナーコ
アに前記磁界発生手段のコイルを位置決め固定する立ち
上げ部を設けて構成したので、その立ち上げ部を巻き芯
としてコイルを巻き付けることにより、コアはコイルの
寸法に制約されることなく適正な寸法に設計でき、小型
化およびコアの共通化が可能となり、製品管理が容易に
なるという効果が得られる。
According to the second aspect of the present invention, since the inner core is provided with the rising portion for positioning and fixing the coil of the magnetic field generating means, the rising portion is used as the winding core to wind the coil. The core can be designed to have an appropriate size without being restricted by the size of the coil, downsizing and sharing of the core can be achieved, and product management becomes easy.

【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側面図であ
る。
FIG. 2 is a side view in which a part of the electromagnetic flow meter is cut away.

【図3】コア3とインナーコア8との関係図を示すもの
で、図3(a)は正面図、図3(b)は平面図である。
3A and 3B are views showing a relationship between a core 3 and an inner core 8, FIG. 3A being a front view and FIG. 3B being a plan view.

【図4】電磁流量計の測定原理を説明する概略構成図で
ある。
FIG. 4 is a schematic configuration diagram illustrating a measurement principle of an electromagnetic flow meter.

【図5】従来の電磁流量計におけるコイルとコアとの関
係を示す概要図である。
FIG. 5 is a schematic diagram showing a relationship between a coil and a core in a conventional electromagnetic flow meter.

【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 8 インナーコア 8−1 平面部 8−2a,8−2b 立ち上げ部 DESCRIPTION OF SYMBOLS 1 Measuring tube 2 Fluid to be measured 4 Coil (magnetic field generating means) 5 Electrode 7 Outer core for magnetic flux feedback 8 Inner core 8-1 Plane part 8-2a, 8-2b Rising part

Claims (2)

【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、前記磁界の作用により前記被測定流体中に発
生した信号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、前記測定管と
前記磁界発生手段との間に設けられたインナーコアとを
備えた電磁流量計において、前記インナーコアの中央部
に前記磁界発生手段のコア載置平面部を設けたことを特
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 orthogonal to the fluid to be measured in the measuring pipe, and a signal generated in the fluid to be measured by the action of the magnetic field is measured. As described above, in the electromagnetic flowmeter including at least a pair of electrodes provided so as to face each other on the diameter of the measurement tube, and an inner core provided between the measurement tube and the magnetic field generating means, An electromagnetic flowmeter characterized in that a core mounting plane portion of the magnetic field generating means is provided in a central portion of the core.
【請求項2】 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
生した信号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、前記測定管と
前記磁界発生手段との間に設けられたインナーコアとを
備えた電磁流量計において、前記インナーコアに前記磁
界発生手段のコイルを位置決め固定する立ち上げ部を設
けたことを特徴とする電磁流量計。
2. A measuring pipe through which a fluid to be measured is passed, a magnetic field generating means for generating a magnetic field orthogonal to the fluid to be measured in the measuring pipe, and a signal generated in the fluid to be measured by the action of the magnetic field is measured. As described above, in the electromagnetic flowmeter including at least a pair of electrodes provided so as to face each other on the diameter of the measurement tube, and an inner core provided between the measurement tube and the magnetic field generating means, An electromagnetic flowmeter, wherein a rising portion for positioning and fixing the coil of the magnetic field generating means is provided on the core.
JP29717695A 1995-11-15 1995-11-15 Electromagnetic flowmeter Pending JPH09138148A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29717695A JPH09138148A (en) 1995-11-15 1995-11-15 Electromagnetic flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29717695A JPH09138148A (en) 1995-11-15 1995-11-15 Electromagnetic flowmeter

Publications (1)

Publication Number Publication Date
JPH09138148A true JPH09138148A (en) 1997-05-27

Family

ID=17843168

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29717695A Pending JPH09138148A (en) 1995-11-15 1995-11-15 Electromagnetic flowmeter

Country Status (1)

Country Link
JP (1) JPH09138148A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2016095257A (en) * 2014-11-17 2016-05-26 横河電機株式会社 Electromagnetic flowmeter
CN111649790A (en) * 2020-06-13 2020-09-11 江苏华海测控技术有限公司 Antidetonation type digit vortex flowmeter

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2016095257A (en) * 2014-11-17 2016-05-26 横河電機株式会社 Electromagnetic flowmeter
CN111649790A (en) * 2020-06-13 2020-09-11 江苏华海测控技术有限公司 Antidetonation type digit vortex flowmeter
CN111649790B (en) * 2020-06-13 2022-01-21 江苏华海测控技术有限公司 Antidetonation type digit vortex flowmeter

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