JPH09145435A - Electromagnetic flow meter - Google Patents

Electromagnetic flow meter

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Publication number
JPH09145435A
JPH09145435A JP30480095A JP30480095A JPH09145435A JP H09145435 A JPH09145435 A JP H09145435A JP 30480095 A JP30480095 A JP 30480095A JP 30480095 A JP30480095 A JP 30480095A JP H09145435 A JPH09145435 A JP H09145435A
Authority
JP
Japan
Prior art keywords
magnetic field
measuring tube
measured
electromotive force
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
JP30480095A
Other languages
Japanese (ja)
Inventor
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 JP30480095A priority Critical patent/JPH09145435A/en
Publication of JPH09145435A publication Critical patent/JPH09145435A/en
Pending legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To provide an electromagnetic flow meter having stable measurement efficiency without causing a measurement error affected by the external magnetic field by providing a magnetic field generating means, electrodes, and a magnetic shield plate. SOLUTION: A coil 4 is excited to generate the magnetic field in the direction perpendicular to the axis of a measuring tube 1, and electromotive force is generated when a measured fluid 2 is moved in the measuring tube 1 located in the magnetic field. If the magnetic field is generated perpendicularly to the electrically insulated measuring tube 1 and the conductivity of the flowing fluid is not too low, the electromotive force can be measured between a pair of electrodes 5. The electromotive force is converted into the signal corresponding to the fluid and outputted by a converter, and the flow can be measured. A magnetic shield plate 10 is provided at the position most apart from the coil 4, the plate 10 hardly attracts the magnetic flux generated by the coil 4, no adverse effect is inflicted on the detection efficiency, and stable measurement can be invariably made without impairing the measurement efficiency.

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2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. 2 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】図5は従来の電磁流量計を示す一部を切断
した正面図であり、図において、101は測定管、10
2は測定管101内を流れる導電性液体である被測定流
体、103は測定管101の外周に設けられたコア、1
04はそのコア103に巻かれた磁界発生手段としての
コイル、105は測定管101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、
107はコイル104を覆って上記測定管101に固定
する磁束帰還用アウターコア、108は測定管101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
104と測定管101との間に介在させたインナーコ
ア、109はコイル104、磁束帰還用アウターコア
7、インナーコア108の周囲を覆い、測定管101に
溶接により固定するケースである。
FIG. 5 is a partially cutaway front view showing a conventional electromagnetic flow meter. In the figure, 101 is a measuring tube and 10 is a measuring tube.
2 is a fluid to be measured which is a conductive liquid flowing in the measuring tube 101, 103 is a core provided on the outer circumference of the measuring tube 101,
Reference numeral 04 is a coil wound around the core 103 as a magnetic field generating means, reference numeral 105 is at least a pair of electrodes provided at positions facing each other on the diameter of the measuring tube 101 and intersecting the magnetic field,
Reference numeral 107 denotes a magnetic flux feedback outer core which covers the coil 104 and is fixed to the measuring tube 101, and 108 is interposed between the coil 104 and the measuring tube 101 in order to generate a magnetic field in parallel in the diameter range of the measuring tube 101. An inner core 109 is a case that covers the coil 104, the magnetic flux feedback outer core 7, and the inner core 108, and is fixed to the measuring tube 101 by welding.

【0004】次に動作について説明する。不図示の電源
から給電線4aを通じての給電によってコイル104を
励磁すると、コア103を通じて測定管101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
101に被測定流体102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101に直角に
生じ、流れている被測定流体102の導電率が低すぎな
ければ、一対の電極105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102の平均流
速と電極間距離に比例するもので、この起電力を電極1
05に接続した信号線106を通じて取り出し、ノイズ
を取り除き、前記図2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 104 is excited by power supply from a power supply (not shown) through the power supply line 4a, a magnetic field φ is generated through the core 103 in a direction orthogonal to the axis of the measuring tube 101. When the fluid to be measured 102 is moved to the measuring tube 101 in this magnetic field, an electromotive force is generated according to Faraday's law of electromagnetic induction. In this case, the magnetic field φ is generated at right angles to the electrically insulated measuring tube 101, and the electromotive force can be measured between the pair of electrodes 105 unless the conductivity of the fluid under measurement 102 is too low.
This electromotive force is proportional to the strength of the magnetic field φ, the average flow velocity of the fluid 102 to be measured, and the distance between the electrodes.
The flow rate can be measured by taking out through the signal line 106 connected to 05, removing noise, converting the signal into a signal corresponding to the fluid by the converter 56 and outputting the signal as shown in FIG.

【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 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、据え付け時、斜線示の
ように強磁性材である鉄製の配管110a、110b
を、そのフランジ部110a−1、110b−1によっ
て測定管101に連結すると、ケース109内の磁束分
布がフランジ部110a−1、110b−1に引かれて
鎖線示のように変化し、信号線106を介して取り出さ
れる起電力が変化する。このため、配管110a,11
0bを取り付ける場合と取り付けない場合とでは、計測
値が変わり、計測誤差を生じるという課題があった。こ
の場合の起電力は数mVであり、一般にフランジ部を付
けない状態で電磁流量計検出器の初期設定を行っている
ので、上述のような磁束分布の変化は、起電力自体をシ
フトさせ、これが変換器(検出器からの信号を増幅する
もの:図示せず)で増幅され、結果的に初期状態とかな
りのズレを生じる。
Since the conventional electromagnetic flowmeter is constructed as described above, when installed, the iron pipes 110a and 110b made of a ferromagnetic material, as shown by hatching, are shown.
Is connected to the measuring tube 101 by the flange portions 110a-1 and 110b-1, the magnetic flux distribution in the case 109 is drawn by the flange portions 110a-1 and 110b-1 and changes as shown by the chain line, and the signal line The electromotive force extracted via 106 changes. Therefore, the piping 110a, 11
There is a problem in that the measurement value changes depending on whether 0b is attached or not, resulting in a measurement error. In this case, the electromotive force is several mV, and generally, the electromagnetic flowmeter detector is initialized without the flange portion attached. Therefore, the change in the magnetic flux distribution as described above shifts the electromotive force itself, This is amplified by the converter (which amplifies the signal from the detector: not shown), resulting in a considerable deviation from the initial state.

【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、外部磁界の影響による計測誤差を
受けることがなく、計測効率の安定した電磁流量計を得
ることを目的とする。
The present invention has been made to solve the above problems, and an object thereof is to obtain an electromagnetic flowmeter having stable measurement efficiency without being affected by a measurement error due to the influence of an external magnetic field.

【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、前記測定管両端鍔部に設けた磁気シールドプレ
ートとを備えたものである。
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. In order to measure the electromotive force generated in the measurement tube, at least a pair of electrodes are provided so as to face each other on the diameter of the measurement tube, and a magnetic shield plate is provided on the flanges at both ends of the measurement tube.

【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、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、10は測定管両端鍔部に設けた磁気
シールドプレートである。
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, in which 1 is a measuring pipe, 2 is a fluid to be measured which is a conductive liquid flowing in the measuring pipe 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, and 5 is provided on the diameter of the measuring tube 1 so as to face each other and intersect the magnetic field. At least a pair of electrodes, 7 is a magnetic flux feedback outer core which covers the coil 4 and is fixed to the measuring tube 1, and 8 is a coil 4 and the measuring tube 1 for generating parallel magnetic fields in the diameter range of the measuring tube 1. An inner core 9 interposed between the coil 4, the outer core 7 for magnetic flux return, and the inner core 8 is fixed to the measuring pipe 1 by welding. A case 10 is a magnetic shield provided at both ends of the measuring pipe. It is a plate.

【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、こ
のライニング処理時に測定管1の測定管両端鍔部1a,
1bの外面にリング状の磁気シールドプレート10を配
設して一体的に組付ける。そして、ライニング処理後の
測定管端面にはケース9内の検出部と測定流体とを同電
位にする接液リング13a,13bが取り付けられ、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13a,13b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 at the time of this lining treatment, the flange portions 1a at both ends of the measuring pipe 1 are
A ring-shaped magnetic shield plate 10 is arranged on the outer surface of 1b and assembled integrally. Then, on the end surface of the measuring tube after the lining treatment, liquid contact rings 13a and 13b that make the detection part in the case 9 and the measuring fluid the same potential are attached, and the material of the lining treatment 11 is, for example, fluorine resin or chloroprene. Rubber, polyurethane rubber, ceramics, etc. are used. As the material of the liquid contact rings 13a and 13b, for example, stainless steel, platinum / indium, tantalum, titanium, Hastelloy B, Hastelloy C, Monel, conductive fluororesin, or the like is used.

【0011】上記構成の電磁流量計は、据え付け時、斜
線示のように強磁性材である鉄製の配管12a、12b
を、そのフランジ部12a−1、12b−1によって測
定管1に連結接続するが、この連結接続の仕方には、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。
When installed, the electromagnetic flowmeter having the above-mentioned structure is provided with iron pipes 12a, 12b made of a ferromagnetic material, as indicated by hatching.
Are connected to the measuring pipe 1 by the flange portions 12a-1 and 12b-1, and various methods such as a flange connection method, a flange clamping method, a sanitary connection method, and a screw connection method can be used for this connection connection. is there.

【0012】次に動作について説明する。不図示の電源
から給電線4aを通じて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1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2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. The coil 4 is excited by power feeding from a power source (not shown) through the power feeding line 4a, and a magnetic field is generated in a direction orthogonal to the axis of the measuring tube 1,
When the fluid to be measured 2 is moved to the measuring tube 1 in this magnetic field,
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.

【0013】以上のように、この実施の形態1によれ
ば、測定管両端鍔部1a,1bの外面、つまりケース9
内のコイル4から最も離れた位置に磁気シールドプレー
ト10を設けたことにより、この磁気シールドプレート
はコイル4により発生された磁束を引き付けることが少
なく、検出効率に悪影響を生じない。また、接液リング
13a,13bを介して測定管両端鍔部1a,1bに配
管12a、12bのフランジ部12a−1、12b−1
を連結しても、磁気シールドプレート10によって上記
磁束には何らの影響も及ぼさないので、計測効率を損な
うことがなく、常に安定した計測を行うことができる効
果が得られる。
As described above, according to the first embodiment, the outer surfaces of the flange portions 1a and 1b at both ends of the measuring tube, that is, the case 9
Since the magnetic shield plate 10 is provided at a position farthest from the coil 4 inside, the magnetic shield plate hardly attracts the magnetic flux generated by the coil 4 and does not adversely affect the detection efficiency. Further, the flange portions 12a-1, 12b-1 of the pipes 12a, 12b are attached to the flange portions 1a, 1b at both ends of the measuring pipe via the liquid contact rings 13a, 13b.
Since the magnetic shield plate 10 does not have any influence on the magnetic flux even if is connected, measurement efficiency is not impaired and stable measurement can always be performed.

【0014】実施の形態2.図3はこの発明の実施の形
態2による電磁流量計を示す一部を切断した正面図であ
り、上記実施の形態1では、測定管両端鍔部1a,1b
の外面にリング状の磁気シールドプレート10を配設し
たが、本実施の形態2は測定管両端鍔部1a,1bの内
面に図4に示す円弧状の磁気シールドプレート10a〜
10dをリング状に配置し、例えば、接着剤等で組付け
固定したもので、コイル4からの磁束が多少、磁気シー
ルドプレート10a〜10dに流れ易くなるが、実施の
形態1と同様の作用効果が得られる。
Embodiment 2 FIG. FIG. 3 is a partially cut-away front view showing an electromagnetic flowmeter according to a second embodiment of the present invention. In the above-described first embodiment, the measuring tube both end flange portions 1a, 1b are shown.
Although the ring-shaped magnetic shield plate 10 is arranged on the outer surface of the above, in the second embodiment, the arc-shaped magnetic shield plate 10a shown in FIG.
10d arranged in a ring shape and assembled and fixed with, for example, an adhesive or the like makes it easier for the magnetic flux from the coil 4 to slightly flow to the magnetic shield plates 10a to 10d, but the same effect as the first embodiment. Is obtained.

【0015】[0015]

【発明の効果】以上のように、請求項1記載の発明によ
れば、測定管両端鍔部の外面に、請求項1記載の発明よ
れば、測定管両端鍔部の内面に磁気シールドプレートを
組付けて構成したので、この磁気シールドプレートはケ
ース内のコイルから最も離れた位置にあり、このコイル
により発生した磁束を引き付けることが少なく、検出効
率に悪影響を生じない。また、測定管両端鍔部に配管の
フランジ部を連結しても、上記磁束は磁気シールドプレ
ートで磁気シールドされており、何らの影響も受けな
い。従って、計測効率を損なうことがなく、常に安定し
た計測を行うことができる効果がある。
As described above, according to the first aspect of the present invention, the magnetic shield plate is provided on the outer surface of the flange portion at both ends of the measuring tube, and according to the first aspect of the invention, the inner surface of the flange portion at both ends of the measuring tube is provided. Since the magnetic shield plate is assembled, the magnetic shield plate is located farthest from the coil in the case, the magnetic flux generated by the coil is hardly attracted, and the detection efficiency is not adversely affected. Further, even if the flange portions of the pipe are connected to the flange portions at both ends of the measuring pipe, the magnetic flux is magnetically shielded by the magnetic shield plate and is not affected at all. Therefore, there is an effect that stable measurement can be always performed without impairing the measurement efficiency.

【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 flowmeter according to a first embodiment of the present invention.

【図2】電磁流量計の原理を説明する図である。FIG. 2 is a diagram illustrating the principle of an electromagnetic flow meter.

【図3】この発明の実施の形態2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. 3 is a partially cutaway front view showing an electromagnetic flow meter according to a second embodiment of the present invention.

【図4】実施の形態2で用いる磁気シールドの正面図で
ある。
FIG. 4 is a front view of a magnetic shield used in the second embodiment.

【図5】従来の電磁流量計を示す一部を切断した正面図
である。
FIG. 5 is a partially cutaway front view showing a conventional electromagnetic flowmeter.

【符号の説明】[Explanation of symbols]

1 測定管 1a,1b 測定管両端鍔部 2 被測定流体 4 コイル(磁界発生手段) 5 電極 10 磁気シールドプレート 12a,12b 配管 12a−1,12b−1 フランジ部 DESCRIPTION OF SYMBOLS 1 Measuring pipe 1a, 1b Measuring pipe both ends collar part 2 Fluid to be measured 4 Coil (magnetic field generating means) 5 Electrode 10 Magnetic shield plate 12a, 12b Piping 12a-1, 12b-1 Flange part

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、前記磁界の作用により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、前記測定管両端鍔部に設けた磁
気シールドプレートとを備えた電磁流量計。
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 the measurement so as to measure an electromotive force generated by the action of the magnetic field. An electromagnetic flowmeter comprising: at least a pair of electrodes provided to face each other on the diameter of the tube; and a magnetic shield plate provided on both end flanges of the measurement tube.
JP30480095A 1995-11-22 1995-11-22 Electromagnetic flow meter Pending JPH09145435A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP30480095A JPH09145435A (en) 1995-11-22 1995-11-22 Electromagnetic flow meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30480095A JPH09145435A (en) 1995-11-22 1995-11-22 Electromagnetic flow meter

Publications (1)

Publication Number Publication Date
JPH09145435A true JPH09145435A (en) 1997-06-06

Family

ID=17937400

Family Applications (1)

Application Number Title Priority Date Filing Date
JP30480095A Pending JPH09145435A (en) 1995-11-22 1995-11-22 Electromagnetic flow meter

Country Status (1)

Country Link
JP (1) JPH09145435A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005172645A (en) * 2003-12-12 2005-06-30 Yokogawa Electric Corp Wafer type electromagnetic flowmeter
DE102006014677A1 (en) * 2006-03-28 2007-10-04 Endress + Hauser Flowtec Ag Magneto inductive flow meter for measuring volume flow or mass flow of medium, has screening units between pole shoes and guide plate to reduce magnetic stray fields in outer space of tube and to increase field strength of magnetic field
CN102636224A (en) * 2012-05-11 2012-08-15 沈阳北星仪表制造有限公司 Intelligent photoelectric magnetic flow meter

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005172645A (en) * 2003-12-12 2005-06-30 Yokogawa Electric Corp Wafer type electromagnetic flowmeter
DE102006014677A1 (en) * 2006-03-28 2007-10-04 Endress + Hauser Flowtec Ag Magneto inductive flow meter for measuring volume flow or mass flow of medium, has screening units between pole shoes and guide plate to reduce magnetic stray fields in outer space of tube and to increase field strength of magnetic field
CN102636224A (en) * 2012-05-11 2012-08-15 沈阳北星仪表制造有限公司 Intelligent photoelectric magnetic flow meter

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