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JP2001241981A - Electromagnetic flow meter - Google Patents

Electromagnetic flow meter

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Publication number
JP2001241981A
JP2001241981A JP2000049886A JP2000049886A JP2001241981A JP 2001241981 A JP2001241981 A JP 2001241981A JP 2000049886 A JP2000049886 A JP 2000049886A JP 2000049886 A JP2000049886 A JP 2000049886A JP 2001241981 A JP2001241981 A JP 2001241981A
Authority
JP
Japan
Prior art keywords
coil
fluid
measuring
measured
tube
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
JP2000049886A
Other languages
Japanese (ja)
Inventor
Shigehiko Aramaki
成彦 荒牧
Yoshitomi Sameda
芳富 鮫田
Takuya Iijima
拓也 飯島
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.)
Toshiba Corp
Original Assignee
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP2000049886A priority Critical patent/JP2001241981A/en
Publication of JP2001241981A publication Critical patent/JP2001241981A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】 【課題】低い導電率の被測定流体や微少な流れの流速計
測を確実に行なって流量計測の性能を向上すること。 【解決手段】測定部の内壁断面を偏平にし、内部を被測
定流体が流れる測定管11と、測定管11の偏平にして
間隔が短くなった面に配置され、被測定流体に測定管1
1の管軸方向とほぼ直交する方向の磁界を与えるコイル
12と、測定管11の偏平にして間隔が長くなった面に
対向配置され、磁界中を被測定流体が移動することによ
って発生する起電力を取り出す一対の電磁13と、測定
管11、コイル12、および電極13を取り囲むように
配置され、コイルの12コアおよび帰磁路を形成するヨ
ーク14とを備える。
(57) [Summary] [PROBLEMS] To improve the performance of flow rate measurement by reliably measuring the flow velocity of a fluid to be measured having a low conductivity or a minute flow. The measuring section has an inner wall section that is flattened and the inside of which is arranged on a measuring tube 11 through which a fluid to be measured flows and a flattened surface of the measuring tube 11 with a short interval.
1, a coil 12 for applying a magnetic field in a direction substantially perpendicular to the tube axis direction, and a flat surface of the measuring tube 11 with a long interval therebetween, which is opposed to the coil 12 for generating a magnetic field. It includes a pair of electromagnetics 13 for extracting electric power, and a yoke 14 that is arranged so as to surround the measuring tube 11, the coil 12, and the electrode 13, and that forms a 12-core coil and a return path.

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】本発明は、測定管の内部に被
測定流体を流し、コイルで被測定流体に磁界をかけ、こ
の磁界の中を被測定流体が移動することによって発生す
る起電力を一対の電極で取り出し、この起電力から被測
定流体の流速を検出する電磁流量計に係り、特に流速計
測の性能を大幅に向上できるようにした電磁流量計に関
するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electromotive force generated by flowing a fluid to be measured inside a measuring tube, applying a magnetic field to the fluid to be measured by a coil, and moving the fluid to be measured in the magnetic field. The present invention relates to an electromagnetic flowmeter that takes out a pair of electrodes and detects the flow velocity of a fluid to be measured from the electromotive force, and particularly relates to an electromagnetic flowmeter that can greatly improve the performance of flow velocity measurement.

【0002】[0002]

【従来の技術】従来から、被測定流体の流速を検出する
電磁流量計の一つとして、測定管の内部に被測定流体を
流し、コイルで被測定流体に磁界をかけ、この磁界の中
を被測定流体が移動することによって発生する起電力を
一対の電極で取り出し、この起電力から被測定流体の流
速を検出する電磁流量計が用いられている。
2. Description of the Related Art Conventionally, as one of the electromagnetic flowmeters for detecting the flow velocity of a fluid to be measured, a fluid to be measured is caused to flow inside a measuring tube, and a magnetic field is applied to the fluid to be measured by a coil. Electromagnetic flowmeters are used in which an electromotive force generated by movement of a fluid to be measured is extracted by a pair of electrodes, and the flow rate of the fluid to be measured is detected from the electromotive force.

【0003】図6は、この種の従来の電磁流量計の測定
部の構成例を示す断面図である。
FIG. 6 is a sectional view showing an example of the configuration of a measuring section of a conventional electromagnetic flowmeter of this type.

【0004】図6において、電磁流量計は、内部を被測
定流体が流れる円筒形の測定管61と、測定管61に沿
って湾曲して測定管61の両面に配置され、被測定流体
に測定管61の管軸方向とほぼ直交する方向の磁界を与
える一対のコイル62と、コイル62とほぼ直交する方
向の両面に対向配置され、磁界中を被測定流体が移動す
ることによって発生する起電力を取り出す一対の電磁6
3と、測定管61、コイル62、および電極63を取り
囲むように配置され、コイル62のコアおよび帰磁路を
形成するヨーク64と備えて構成されている。
In FIG. 6, an electromagnetic flowmeter has a cylindrical measuring pipe 61 through which a fluid to be measured flows, and is arranged on both sides of the measuring pipe 61 so as to be curved along the measuring pipe 61 so as to measure the fluid to be measured. A pair of coils 62 for providing a magnetic field in a direction substantially perpendicular to the tube axis direction of the tube 61, and an electromotive force generated by the fluid to be measured moving in the magnetic field, disposed opposite to both surfaces in a direction substantially perpendicular to the coil 62. A pair of electromagnetic 6 to take out
3 and a yoke 64 that is arranged so as to surround the measurement tube 61, the coil 62, and the electrode 63, and forms a core of the coil 62 and a return magnetic path.

【0005】図7は、かかる従来の電磁流量計の流速計
測原理となるファラデーの電磁誘導法則を示す概念図で
ある。
FIG. 7 is a conceptual diagram showing Faraday's electromagnetic induction law, which is the principle of measuring the flow velocity of such a conventional electromagnetic flowmeter.

【0006】図7において、磁界の中を導体が通過する
と、磁界の磁束密度71と、磁束をほぼ垂直に横切る導
体の移動速度72と、導体の幅73とによって、磁束と
移動方向にほぼ垂直な方向に起電力74が発生する。
In FIG. 7, when a conductor passes through a magnetic field, the magnetic flux density 71 of the magnetic field, the moving speed 72 of the conductor that crosses the magnetic flux almost vertically, and the width 73 of the conductor make the magnetic flux and the moving direction substantially perpendicular. The electromotive force 74 is generated in a different direction.

【0007】起電力をe(V)、磁束密度をB(T)、
導体の幅をD(cm)、移動速度をv(cm/s)とす
ると、 e=B・D・v×10-4 が成り立つ。
The electromotive force is e (V), the magnetic flux density is B (T),
Assuming that the width of the conductor is D (cm) and the moving speed is v (cm / s), the following holds: e = B · D · v × 10 −4 .

【0008】すなわち、電磁流量計は、被測定流体が測
定管61の内部を流れ、コイル62が発生した磁界を、
ヨーク64によって被測定流体の流れとほぼ垂直方向に
かけ、被測定流体の流れと磁界にほぼ垂直な方向に発生
した起電力を一対の電極63で取り出す。
That is, in the electromagnetic flow meter, the fluid to be measured flows inside the measuring tube 61 and the magnetic field generated by the coil 62 is
The yoke 64 is applied in a direction substantially perpendicular to the flow of the fluid to be measured, and the electromotive force generated in a direction substantially perpendicular to the flow of the fluid to be measured and the magnetic field is taken out by the pair of electrodes 63.

【0009】[0009]

【発明が解決しようとする課題】しかしながら、このよ
うな従来の電磁流量計においては、次のような問題点が
ある。
However, such a conventional electromagnetic flowmeter has the following problems.

【0010】すなわち、低い導電率の被測定流体はフロ
ーノイズが大きいため、起電力を検知することが困難で
ある。特に、被測定流体の流速が速くなるとフローノイ
ズも大きくなり、流速計測を行なうことができない。
That is, since a fluid to be measured having a low conductivity has a large flow noise, it is difficult to detect an electromotive force. In particular, when the flow velocity of the fluid to be measured increases, the flow noise also increases, and the flow velocity cannot be measured.

【0011】一方、高い導電率の被測定流体はフローノ
イズが小さいが、微少な流れの流速計測を行なうことが
困難である。また、電磁流量計は、磁界をかける大きな
エネルギーが必要なため、消費電力が大きくなる。
On the other hand, the fluid to be measured having high conductivity has small flow noise, but it is difficult to measure the flow velocity of a minute flow. Further, the electromagnetic flowmeter requires large energy for applying a magnetic field, and thus consumes a large amount of power.

【0012】さらに、円筒形の測定管61の形状に合わ
せた構成部品の湾曲加工や組み立てが必要であり、結果
として電磁流量計の生産性が低下することになる。
Further, it is necessary to bend and assemble the components in accordance with the shape of the cylindrical measuring tube 61, and as a result, the productivity of the electromagnetic flowmeter is reduced.

【0013】本発明の第1の目的は、低い導電率の被測
定流体や微少な流れの流速計測を確実に行なって流量計
測の性能を向上することが可能で消費電力が小さい電磁
流量計を提供することにある。
A first object of the present invention is to provide an electromagnetic flowmeter which can reliably measure a flow rate of a fluid to be measured having a low electric conductivity or a minute flow, improve the performance of the flow measurement, and consume less power. To provide.

【0014】また、本発明の第2の目的は、生産性を向
上することが可能な電磁流量計を提供することにある。
[0014] A second object of the present invention is to provide an electromagnetic flowmeter capable of improving productivity.

【0015】[0015]

【課題を解決するための手段】上記第1の目的を達成す
るために、請求項1に対応する発明の電磁流量計は、測
定部の内壁断面を偏平にし、内部を被測定流体が流れる
測定管と、測定管の偏平にして間隔が短くなった面に配
置され、被測定流体に測定管の管軸方向とほぼ直交する
方向の磁界を与えるコイルと、測定管の偏平にして間隔
が長くなった面に対向配置され、磁界中を被測定流体が
移動することによって発生する起電力を取り出す一対の
電極と、測定管、コイル、および電極を取り囲むように
配置され、コイルのコアおよび帰磁路を形成するヨーク
とを備えて成る。
In order to achieve the first object, an electromagnetic flowmeter according to the present invention has a measurement section in which a cross section of an inner wall of a measurement section is flattened and a fluid to be measured flows inside the measurement section. A tube, a coil arranged on the flattened surface of the measuring tube and having a reduced interval, and applying a magnetic field to the fluid to be measured in a direction substantially perpendicular to the tube axis direction of the measuring tube; And a pair of electrodes that take out the electromotive force generated by the movement of the fluid to be measured in the magnetic field, and a measurement tube, a coil, and a core and return magnet that surround the electrodes. And a yoke forming a path.

【0016】従って、請求項1に対応する発明の電磁流
量計においては、測定管の測定部の内壁断面を偏平にす
ることにより、ファラデーの電磁誘導法則e=B・D・
v×10-4より、磁束密度と移動速度が変わらず被測定
流体の幅が大きくなるため、起電力が大きくなる。これ
により、低い導電率の被測定流体は起電力が大きくなる
ため、フローノイズの影響を受け難くなり、性能よく被
測定流体の流速を計測することができる。また、測定管
の測定部の内壁断面を偏平にすることにより、磁界をか
ける距離が短くなるため、高い導電率の被測定流体の流
速を計測する時には、磁束密度を小さくすることで磁界
をかけるエネルギーを小さくして、消費電力を小さくす
ることができる。
Therefore, in the electromagnetic flowmeter according to the first aspect of the present invention, the Faraday's law of electromagnetic induction e = BD
From v × 10 −4 , the magnetic flux density and the moving speed do not change and the width of the fluid to be measured is increased, so that the electromotive force is increased. As a result, the fluid to be measured having a low electrical conductivity has a large electromotive force, so that the fluid is hardly affected by flow noise, and the flow velocity of the fluid to be measured can be measured with good performance. Also, by flattening the cross section of the inner wall of the measuring part of the measuring tube, the distance for applying the magnetic field is shortened, so when measuring the flow velocity of the fluid to be measured having high conductivity, the magnetic field is applied by reducing the magnetic flux density. Energy can be reduced and power consumption can be reduced.

【0017】また、請求項2に対応する発明の電磁流量
計は、測定部の内壁断面を楕円形にし、内部を被測定流
体が流れる測定管と、測定管の楕円形にして間隔が短く
なった面に配置され、被測定流体に測定管の管軸方向と
ほぼ直交する方向の磁界を与えるコイルと、測定管の楕
円形にして間隔が長くなった面に対向配置され、磁界中
を被測定流体が移動することによって発生する起電力を
取り出す一対の電極と、測定管、コイル、および電極を
取り囲むように配置され、コイルのコアおよび帰磁路を
形成するヨークとを備えて成る。
In the electromagnetic flowmeter according to the second aspect of the present invention, the inner wall section of the measuring section is made elliptical, and the space between the measuring pipe and the measuring pipe through which the fluid to be measured flows is made shorter. And a coil that applies a magnetic field to the fluid to be measured in a direction substantially perpendicular to the tube axis direction of the measurement tube, and a coil that is disposed opposite to the elliptical surface of the measurement tube that has a long interval, and It comprises a pair of electrodes for extracting an electromotive force generated by the movement of the measurement fluid, a measurement tube, a coil, and a yoke which is arranged so as to surround the electrode and forms a coil core and a return path.

【0018】従って、請求項2に対応する発明の電磁流
量計においては、測定管の測定部の内壁断面を楕円形に
することにより、ファラデーの電磁誘導法則e=B・D
・v×10-4より、磁束密度と移動速度が変わらず被測
定流体の幅が大きくなるため、起電力が大きくなる。こ
れにより、低い導電率の被測定流体は起電力が大きくな
るため、フローノイズの影響を受け難くなり、性能よく
被測定流体の流速を計測することができる。また、測定
管の測定部の内壁断面を楕円形にすることにより、磁界
をかける距離が短くなるため、高い導電率の被測定流体
の流速を計測する時には、磁束密度を小さくすることで
磁界をかけるエネルギーを小さくして、消費電力を小さ
くすることができる。さらに、測定管の測定部の内壁断
面を楕円形にすることにより、測定管を圧力に強くする
ことができる。
Therefore, in the electromagnetic flow meter according to the second aspect of the present invention, the Faraday's law of electromagnetic induction e = BD
From v × 10 -4 , the magnetic flux density and the moving speed do not change and the width of the fluid to be measured is increased, so that the electromotive force is increased. As a result, the fluid to be measured having a low electrical conductivity has a large electromotive force, so that the fluid is hardly affected by flow noise, and the flow velocity of the fluid to be measured can be measured with good performance. Also, by making the cross section of the inner wall of the measuring section of the measuring tube elliptical, the distance over which the magnetic field is applied becomes shorter.When measuring the flow velocity of the fluid to be measured having high conductivity, the magnetic field is reduced by reducing the magnetic flux density. The applied energy can be reduced, and the power consumption can be reduced. Furthermore, by making the inner wall cross section of the measuring portion of the measuring tube elliptical, the measuring tube can be made resistant to pressure.

【0019】さらに、請求項3に対応する発明の電磁流
量計は、測定部の内壁断面を長方形にし、内部を被測定
流体が流れる測定管と、測定管の長方形にして間隔が短
くなった面に配置され、被測定流体に測定管の管軸方向
とほぼ直交する方向の磁界を与えるコイルと、測定管の
長方形にして間隔が長くなった面に対向配置され、磁界
中を被測定流体が移動することによって発生する起電力
を取り出す一対の電極と、測定管、コイル、および電極
を取り囲むように配置され、コイルのコアおよび帰磁路
を形成するヨークとを備えて成る。
Further, in the electromagnetic flowmeter according to the invention, the inner wall cross section of the measuring section is made rectangular, and the inside of the measuring pipe through which the fluid to be measured flows is made rectangular, and the surface of the measuring pipe is made rectangular and the interval is shortened. And a coil for applying a magnetic field to the fluid to be measured in a direction substantially perpendicular to the tube axis direction of the measurement tube, and a coil arranged to face the rectangular and long-spaced surface of the measurement tube. It comprises a pair of electrodes for extracting an electromotive force generated by the movement, a measurement tube, a coil, and a yoke arranged so as to surround the electrode and forming a coil core and a return path.

【0020】従って、請求項3に対応する発明の電磁流
量計においては、測定管の測定部の内壁断面を長方形に
することにより、ファラデーの電磁誘導法則e=B・D
・v×10-4より、磁束密度と移動速度が変わらず被測
定流体の幅が大きくなるため、起電力が大きくなる。こ
れにより、低い導電率の被測定流体は起電力が大きくな
るため、フローノイズの影響を受け難くなり、性能よく
被測定流体の流速を計測することができる。また、測定
管の測定部の内壁断面を長方形にすることにより、磁界
をかける距離が短くなるため、高い導電率の被測定流体
の流速を計測する時には、磁束密度を小さくすることで
磁界をかけるエネルギーを小さくして、消費電力を小さ
くすることができる。さらに、測定管の測定部の内壁断
面を長方形にすることにより、測定管を作り易くするこ
とができる。
Therefore, in the electromagnetic flowmeter according to the third aspect of the present invention, the Faraday's law of electromagnetic induction e = BD
From v × 10 -4 , the magnetic flux density and the moving speed do not change and the width of the fluid to be measured is increased, so that the electromotive force is increased. As a result, the fluid to be measured having a low electrical conductivity has a large electromotive force, so that the fluid is hardly affected by flow noise, and the flow velocity of the fluid to be measured can be measured with good performance. In addition, by making the inner wall cross section of the measurement part of the measurement tube rectangular, the distance for applying the magnetic field is shortened. Therefore, when measuring the flow velocity of the fluid to be measured having high conductivity, the magnetic field is applied by reducing the magnetic flux density. Energy can be reduced and power consumption can be reduced. Further, by making the inner wall cross section of the measuring portion of the measuring tube rectangular, it is possible to easily make the measuring tube.

【0021】さらにまた、請求項4に対応する発明の電
磁流量計は、上記請求項1乃至請求項3のいずれか1項
に対応する発明の電磁流量計において、測定管の測定部
の内壁断面積を出入口よりも小さな断面積としている。
According to a fourth aspect of the present invention, there is provided the electromagnetic flow meter according to any one of the first to third aspects, wherein the inner wall of the measuring section of the measuring pipe is cut off. The area is smaller than the entrance.

【0022】従って、請求項4に対応する発明の電磁流
量計においては、測定管の測定部の内壁断面積を出入口
よりも小さな断面積とすることにより、ファラデーの電
磁誘導法則e=B・D・v×10-4より、磁束密度が変
わらず、被測定流体の幅が同じか大きくなり、移動速度
が速くなるため、起電力がより一層大きくなる。これに
より、低い導電率の被測定流体は起電力がより一層大き
くなるため、フローノイズの影響を受け難くなり、より
一層性能よく被測定流体の流速を計測することができ
る。また、測定管の測定部の内壁断面積を出入口よりも
小さな断面積とすることにより、磁界をかける距離がよ
り一層短くなるため、高い導電率の被測定流体の流速を
計測する時には、磁束密度を小さくすることで磁界をか
けるエネルギーをより一層小さくして、消費電力をより
一層小さくすることができる。
Therefore, in the electromagnetic flowmeter according to the present invention, the inner wall cross-sectional area of the measuring section of the measuring tube is made smaller than the entrance and exit, so that Faraday's law of electromagnetic induction e = BD From v × 10 −4 , the magnetic flux density does not change, the width of the fluid to be measured is the same or larger, and the moving speed is increased, so that the electromotive force is further increased. As a result, the electromotive force of the fluid to be measured having a low conductivity is further increased, so that the fluid is less affected by the flow noise, and the flow velocity of the fluid to be measured can be measured with higher performance. In addition, by setting the cross-sectional area of the inner wall of the measuring section of the measuring tube to be smaller than that of the entrance and exit, the distance over which the magnetic field is applied is further shortened. , The energy for applying the magnetic field can be further reduced, and the power consumption can be further reduced.

【0023】一方、上記第2の目的を達成するために、
請求項5に対応する発明の電磁流量計は、測定部の外壁
断面を四角形にし、内部を被測定流体が流れる測定管
と、測定管を横切る両方の平面に配置され、被測定流体
に測定管の管軸方向とほぼ直交する方向の磁界を与える
コイルと、測定管のコイルとほぼ直交する方向の両方の
平面に対向配置され、磁界中を被測定流体が移動するこ
とによって発生する起電力を取り出す一対の電極と、測
定管、コイル、および電極を取り囲むように配置され、
コイルのコアおよび帰磁路を形成するヨークとを備えて
成る。
On the other hand, in order to achieve the second object,
An electromagnetic flowmeter according to the invention according to claim 5, wherein the cross section of the outer wall of the measuring section is quadrangular, and the inside is arranged on both the measuring pipe through which the fluid to be measured flows and the plane crossing the measuring pipe. A coil that provides a magnetic field in a direction substantially perpendicular to the tube axis direction and a coil that is disposed opposite to both surfaces in a direction substantially perpendicular to the coil of the measurement tube. A pair of electrodes to be taken out, a measurement tube, a coil, and arranged to surround the electrodes,
And a yoke forming a return magnetic path.

【0024】従って、請求項5に対応する発明の電磁流
量計においては、測定管の測定部の外壁断面を四角形に
することにより、電磁流量計の構成部品が平面に対して
取り付けられるため、湾曲加工が不要となり、測定管へ
の密着性も良くすることができる。また、電磁流量計の
構成部品の梱包を簡単に行なうことができる。これによ
り、電磁流量計を生産する際に加工工程が少なくなり、
組み立て精度が向上し、輸送効率が良くなるため、生産
性を向上することができる。
Therefore, in the electromagnetic flow meter according to the present invention, since the cross-section of the outer wall of the measuring section of the measuring tube is made rectangular, the components of the electromagnetic flow meter are attached to a flat surface, so that the curved portion is curved. Processing becomes unnecessary, and the adhesion to the measurement tube can be improved. Also, the components of the electromagnetic flowmeter can be easily packed. This reduces the number of processing steps when producing electromagnetic flow meters,
Since the assembling accuracy is improved and the transportation efficiency is improved, productivity can be improved.

【0025】[0025]

【発明の実施の形態】以下、本発明の実施の形態につい
て図面を参照して詳細に説明する。
Embodiments of the present invention will be described below in detail with reference to the drawings.

【0026】(第1の実施の形態)図1は、本実施の形
態による電磁流量計の測定部の構成例を示す断面図であ
る。
(First Embodiment) FIG. 1 is a sectional view showing an example of the configuration of a measuring section of an electromagnetic flowmeter according to the present embodiment.

【0027】本実施の形態の電磁流量計は、図1に示す
ように、測定部の内壁断面を偏平にして出入口とほぼ同
じ断面積とし、内部を被測定流体が流れる測定管11
と、測定管11の偏平にして間隔が短くなった面に配置
され、被測定流体に測定管11の管軸方向とほぼ直交す
る方向の磁界を与える一対のコイル12と、測定管11
の偏平にして間隔が長くなった面に対向配置され、磁界
中を被測定流体が移動することによって発生する起電力
を取り出す一対の電磁13と、測定管11、コイル1
2、および電極13を取り囲むように配置され、コイル
12のコアおよび帰磁路を形成するヨーク14とから構
成している。
As shown in FIG. 1, the electromagnetic flow meter according to the present embodiment has a measurement section 11 in which the inner wall of the measuring section is flattened to have a cross-sectional area substantially equal to that of the entrance and exit.
A pair of coils 12 arranged on a flattened surface of the measuring tube 11 at a reduced interval to apply a magnetic field to the fluid to be measured in a direction substantially perpendicular to the tube axis direction of the measuring tube 11;
A pair of electromagnetic 13 for taking out an electromotive force generated by movement of a fluid to be measured in a magnetic field, a measurement tube 11, and a coil 1
2, and a yoke 14 which is arranged to surround the electrode 13 and forms a core of the coil 12 and a return path.

【0028】次に、以上のように構成した本実施の形態
の電磁流量計においては、測定管11の測定部の内壁断
面を偏平にして出入口とほぼ同じ断面積としていること
により、ファラデーの電磁誘導法則e=B・D・v×1
-4より、磁束密度Bと移動速度vが変わらず、被測定
流体の幅Dが大きくなるため、起電力eが大きくなる。
Next, in the electromagnetic flowmeter of the present embodiment configured as described above, the inner wall of the measuring section of the measuring tube 11 is made flat to have the same cross-sectional area as the entrance and exit, so that the Faraday electromagnetic Guidance law e = BDV x 1
Since the magnetic flux density B and the moving speed v do not change from 0 -4 and the width D of the fluid to be measured increases, the electromotive force e increases.

【0029】これにより、低い導電率の被測定流体は起
電力が大きくなるため、フローノイズの影響を受け難く
なり、性能よく被測定流体の流速を計測することができ
る。また、測定管11の測定部の内壁断面を偏平にして
出入口とほぼ同じ断面積としていることにより、磁界を
かける距離が短くなるため、高い導電率の被測定流体の
流速を計測する時には、磁束密度Bを小さくすることで
磁界をかけるエネルギーを小さくして、消費電力を小さ
くすることができる。
As a result, the fluid to be measured having a low conductivity has a large electromotive force, so that the fluid is hardly affected by flow noise, and the flow velocity of the fluid to be measured can be measured with good performance. Further, since the inner wall cross section of the measuring portion of the measuring tube 11 is flattened to have substantially the same cross sectional area as the entrance and exit, the distance for applying a magnetic field is shortened. By reducing the density B, the energy for applying a magnetic field can be reduced, and the power consumption can be reduced.

【0030】上述したように、本実施の形態の電磁流量
計では、測定管11の測定部の内壁断面を偏平にして出
入口とほぼ同じ断面積とするようにしているので、被測
定流体の幅Dが大きくなり、磁界をかける距離が短くな
るため、低い導電率の被測定流体や微少な流れの流速計
測を確実に行なって流量計測の性能を向上することがで
きると共に、消費電力を小さくすることが可能となる。
As described above, in the electromagnetic flowmeter according to the present embodiment, the inner wall of the measuring section of the measuring tube 11 is made flat so as to have substantially the same cross-sectional area as the entrance and exit, so that the width of the fluid to be measured is Since D becomes large and the distance over which the magnetic field is applied becomes short, the flow rate measurement performance of the fluid to be measured having a low conductivity or a small flow can be reliably measured to improve the performance of the flow rate measurement, and the power consumption is reduced. It becomes possible.

【0031】(第2の実施の形態)図2は、本実施の形
態による電磁流量計の測定部の構成例を示す断面図であ
る。
(Second Embodiment) FIG. 2 is a sectional view showing an example of the configuration of a measuring section of an electromagnetic flowmeter according to the present embodiment.

【0032】本実施の形態の電磁流量計は、図2に示す
ように、測定部の内壁断面を楕円形にして出入口とほぼ
同じ断面積とし、内部を被測定流体が流れる測定管21
と、測定管21の楕円形にして間隔が短くなった面に配
置され、被測定流体に測定管21の管軸方向とほぼ直交
する方向の磁界を与える一対のコイル22と、測定管2
1の楕円形にして間隔が長くなった面に対向配置され、
磁界中を被測定流体が移動することによって発生する起
電力を取り出す一対の電磁23と、測定管21、コイル
22、および電極23を取り囲むように配置され、コイ
ル22のコアおよび帰磁路を形成するヨーク24とから
構成している。
As shown in FIG. 2, the electromagnetic flow meter according to the present embodiment has an elliptical inner wall cross section having substantially the same cross-sectional area as the entrance and exit, and a measurement pipe 21 through which the fluid to be measured flows.
A pair of coils 22 arranged on an elliptical surface of the measurement tube 21 having a reduced interval and applying a magnetic field to the fluid to be measured in a direction substantially orthogonal to the tube axis direction of the measurement tube 21;
It is arranged opposite to the elliptical shape of 1 and the surface where the interval is long,
A pair of electromagnetic waves 23 for extracting an electromotive force generated by the movement of the fluid to be measured in the magnetic field, and a pair of electromagnetic waves 23 are arranged so as to surround the measurement tube 21, the coil 22, and the electrode 23, and form a core and a return path of the coil 22. And the yoke 24 which is formed.

【0033】次に、以上のように構成した本実施の形態
の電磁流量計においては、測定管21の測定部の内壁断
面を楕円形にして出入口とほぼ同じ断面積としているこ
とにより、ファラデーの電磁誘導法則e=B・D・v×
10-4より、磁束密度Bと移動速度vが変わらず、被測
定流体の幅Dが大きくなるため、起電力eが大きくな
る。
Next, in the electromagnetic flow meter according to the present embodiment configured as described above, the inner wall of the measuring section of the measuring tube 21 is made elliptical to have substantially the same cross-sectional area as the entrance and exit, so that the Faraday Electromagnetic induction law e = BDVx
From 10 -4 , the magnetic flux density B and the moving speed v do not change, and the width D of the fluid to be measured increases, so that the electromotive force e increases.

【0034】これにより、低い導電率の被測定流体は起
電力が大きくなるため、フローノイズの影響を受け難く
なり、性能よく被測定流体の流速を計測することができ
る。また、測定管21の測定部の内壁断面を楕円形にし
て出入口とほぼ同じ断面積としていることにより、磁界
をかける距離が短くなるため、高い導電率の被測定流体
の流速を計測する時には、磁束密度Bを小さくすること
で磁界をかけるエネルギーを小さくして、消費電力を小
さくすることができる。
Thus, the fluid to be measured having a low conductivity has a large electromotive force, so that the fluid is hardly affected by flow noise, and the flow velocity of the fluid to be measured can be measured with good performance. Further, since the inner wall cross section of the measuring section of the measuring tube 21 is made elliptical and has substantially the same cross sectional area as the entrance and exit, the distance for applying a magnetic field is shortened. Therefore, when measuring the flow velocity of the fluid to be measured having high conductivity, By reducing the magnetic flux density B, the energy for applying a magnetic field can be reduced, and power consumption can be reduced.

【0035】さらに、測定管21の測定部の内壁断面を
楕円形にしていることにより、測定管21を圧力に強く
することができる。
Further, by making the inner wall cross section of the measuring portion of the measuring tube 21 elliptical, the measuring tube 21 can be made resistant to pressure.

【0036】上述したように、本実施の形態の電磁流量
計では、測定管21の測定部の内壁断面を楕円形にして
出入口とほぼ同じ断面積とするようにしているので、被
測定流体の幅Dが大きくなり、磁界をかける距離が短く
なるため、低い導電率の被測定流体や微少な流れの流速
計測を確実に行なって流量計測の性能を向上することが
できると共に、消費電力を小さくすることが可能とな
り、さらに測定管21を圧力に強くすることが可能とな
る。
As described above, in the electromagnetic flow meter according to the present embodiment, the inner wall of the measuring section of the measuring tube 21 is made elliptical so as to have substantially the same cross-sectional area as the entrance and exit. Since the width D increases and the distance over which the magnetic field is applied decreases, the flow rate measurement performance can be improved by reliably measuring the flow rate of the fluid to be measured having a low conductivity or a minute flow, and the power consumption can be reduced. And the pressure of the measuring tube 21 can be increased.

【0037】(第3の実施の形態)図3は、本実施の形
態による電磁流量計の測定部の構成例を示す断面図であ
る。
(Third Embodiment) FIG. 3 is a sectional view showing an example of a configuration of a measuring section of an electromagnetic flowmeter according to the present embodiment.

【0038】本実施の形態の電磁流量計は、図3に示す
ように、測定部の内壁断面を長方形にして出入口とほぼ
同じ断面積とし、内部を被測定流体が流れる測定管31
と、測定管31の長方形にして間隔が短くなった面に配
置され、被測定流体に測定管31の管軸方向とほぼ直交
する方向の磁界を与える一対のコイル32と、測定管3
1の長方形にして間隔が長くなった面に対向配置され、
磁界中を被測定流体が移動することによって発生する起
電力を取り出す一対の電磁33と、測定管31、コイル
32、および電極33を取り囲むように配置され、コイ
ル32のコアおよび帰磁路を形成するヨーク34とから
構成している。
As shown in FIG. 3, the electromagnetic flow meter according to the present embodiment has a rectangular cross section of the inner wall of the measuring section, which has substantially the same cross sectional area as the entrance and exit, and a measuring pipe 31 inside which the fluid to be measured flows.
A pair of coils 32 arranged on a rectangular surface of the measuring tube 31 with a short interval and applying a magnetic field to the fluid to be measured in a direction substantially perpendicular to the tube axis direction of the measuring tube 31;
It is arranged opposite to the surface where the interval has become longer by making one rectangle,
A pair of electromagnetic waves 33 for extracting an electromotive force generated by the movement of the fluid to be measured in the magnetic field, and a pair of electromagnetic waves 33 are arranged so as to surround the measurement tube 31, the coil 32, and the electrode 33, and form a core and a return path of the coil 32. And the yoke 34 to be used.

【0039】次に、以上のように構成した本実施の形態
の電磁流量計においては、測定管31の測定部の内壁断
面を長方形にして出入口とほぼ同じ断面積としているこ
とにより、ファラデーの電磁誘導法則e=B・D・v×
10-4より、磁束密度Bと移動速度vが変わらず、被測
定流体の幅Dが大きくなるため、起電力eが大きくな
る。
Next, in the electromagnetic flowmeter according to the present embodiment configured as described above, the inner wall of the measuring section of the measuring tube 31 is made rectangular and has substantially the same cross-sectional area as the entrance and exit, so that the Faraday electromagnetic Guidance law e = BDVx
From 10 -4 , the magnetic flux density B and the moving speed v do not change, and the width D of the fluid to be measured increases, so that the electromotive force e increases.

【0040】これにより、低い導電率の被測定流体は起
電力が大きくなるため、フローノイズの影響を受け難く
なり、性能よく被測定流体の流速を計測することができ
る。また、測定管31の測定部の内壁断面を長方形にし
て出入口とほぼ同じ断面積としていることにより、磁界
をかける距離が短くなるため、高い導電率の被測定流体
の流速を計測する時には、磁束密度Bを小さくすること
で磁界をかけるエネルギーを小さくして、消費電力を小
さくすることができる。
As a result, the fluid to be measured having a low conductivity has a large electromotive force, so that the fluid is hardly affected by flow noise, and the flow velocity of the fluid to be measured can be measured with good performance. In addition, since the inner wall of the measuring section of the measuring tube 31 has a rectangular cross-section and has substantially the same cross-sectional area as the entrance and exit, the distance over which the magnetic field is applied becomes shorter. By reducing the density B, the energy for applying a magnetic field can be reduced, and the power consumption can be reduced.

【0041】上述したように、本実施の形態の電磁流量
計では、測定管31の測定部の内壁断面を長方形にして
出入口とほぼ同じ断面積とするようにしているので、被
測定流体の幅Dが大きくなり、磁界をかける距離が短く
なるため、低い導電率の被測定流体や微少な流れの流速
計測を確実に行なって流量計測の性能を向上することが
できると共に、消費電力を小さくすることが可能とな
り、さらに測定管31を作り易くすることが可能とな
る。
As described above, in the electromagnetic flowmeter of the present embodiment, the inner wall of the measuring section of the measuring tube 31 has a rectangular cross-section and has substantially the same cross-sectional area as the entrance and exit, so that the width of the fluid to be measured is Since D becomes large and the distance over which the magnetic field is applied becomes short, the flow rate measurement performance of the fluid to be measured having a low conductivity or a small flow can be reliably measured to improve the performance of the flow rate measurement, and the power consumption is reduced. This makes it possible to make the measuring tube 31 easier.

【0042】(第4の実施の形態)図4は、本実施の形
態による電磁流量計の測定部の構成例を示す断面図であ
る。
(Fourth Embodiment) FIG. 4 is a sectional view showing an example of the configuration of a measuring section of an electromagnetic flowmeter according to the present embodiment.

【0043】本実施の形態の電磁流量計は、図4に示す
ように、測定部の内壁断面を偏平にして出入口よりも小
さな断面積とし、内部を被測定流体が流れる測定管41
と、測定管41の偏平にして間隔が短くなった面に配置
され、被測定流体に測定管41の管軸方向とほぼ直交す
る方向の磁界を与える一対のコイル42と、測定管41
の偏平にして間隔が長くなった面に対向配置され、磁界
中を被測定流体が移動することによって発生する起電力
を取り出す一対の電磁43と、測定管41、コイル4
2、および電極43を取り囲むように配置され、コイル
42のコアおよび帰磁路を形成するヨーク44とから構
成している。
As shown in FIG. 4, the electromagnetic flow meter according to the present embodiment has a flat cross section of the inner wall of the measuring section to have a smaller cross sectional area than the entrance and exit, and the inside of the measuring pipe 41 through which the fluid to be measured flows.
A pair of coils 42 arranged on the flattened surface of the measuring tube 41 and having a reduced interval to apply a magnetic field to the fluid to be measured in a direction substantially perpendicular to the tube axis direction of the measuring tube 41;
A pair of electromagnetic 43 for taking out an electromotive force generated by the movement of the fluid to be measured in the magnetic field, a measuring tube 41, and a coil 4.
2, and a yoke 44 that is arranged so as to surround the electrode 43 and forms a core of the coil 42 and a return path.

【0044】次に、以上のように構成した本実施の形態
の電磁流量計においては、測定管41の測定部の内壁断
面を偏平にして出入口よりも小さな断面積としているこ
とにより、ファラデーの電磁誘導法則e=B・D・v×
10-4より、磁束密度Bが変わらず、被測定流体の幅D
が同じか大きくなり、移動速度vが速くなるため、前記
第1の実施の形態に比べて、起電力eがより一層大きく
なる。
Next, in the electromagnetic flow meter according to the present embodiment configured as described above, the inner wall of the measuring portion of the measuring tube 41 is made flat to have a smaller cross-sectional area than the entrance, so that the Faraday electromagnetic Guidance law e = BDVx
From 10 -4 , the magnetic flux density B does not change and the width D of the fluid to be measured is
Are the same or larger, and the moving speed v becomes faster, so that the electromotive force e is further increased as compared with the first embodiment.

【0045】これにより、低い導電率の被測定流体は起
電力がより一層大きくなるため、フローノイズの影響を
受け難くなり、より一層性能よく被測定流体の流速を計
測することができる。また、測定管41の測定部の内壁
断面積を出入口よりも小さな断面積としていることによ
り、磁界をかける距離がより一層短くなるため、高い導
電率の被測定流体の流速を計測する時には、磁束密度を
小さくすることで磁界をかけるエネルギーをより一層小
さくして、前記第1の実施の形態に比べて、消費電力を
より一層小さくすることができる。
As a result, the fluid to be measured having a low conductivity has a larger electromotive force, so that the fluid is less affected by flow noise, and the flow velocity of the fluid to be measured can be measured with higher performance. Further, since the cross-sectional area of the inner wall of the measuring portion of the measuring tube 41 is smaller than that of the entrance and exit, the distance for applying a magnetic field is further shortened. By reducing the density, the energy for applying the magnetic field can be further reduced, and the power consumption can be further reduced as compared with the first embodiment.

【0046】上述したように、本実施の形態の電磁流量
計では、測定管41の測定部の内壁断面を偏平にして出
入口よりも小さな断面積とするようにしているので、被
測定流体の移動速度が速くなるため、前記第1の実施の
形態に比べて、低い導電率の被測定流体や微少な流れの
流速計測をより一層確実に行なって流量計測の性能をよ
り一層向上することができると共に、消費電力をより一
層小さくすることが可能となる。
As described above, in the electromagnetic flowmeter according to the present embodiment, the inner wall of the measuring section of the measuring tube 41 is made flat to have a smaller sectional area than the entrance and exit, so that the movement of the fluid to be measured is performed. Since the speed is increased, the flow rate measurement performance of the fluid to be measured having a low conductivity or a minute flow can be more reliably measured as compared with the first embodiment, and the performance of the flow rate measurement can be further improved. At the same time, power consumption can be further reduced.

【0047】(変形例)本実施の形態の電磁流量計で
は、測定管の測定部の内壁断面を偏平にした前記第1の
実施の形態の電磁流量計において、測定管の測定部の内
壁断面を出入口よりも小さな断面積とする場合について
説明したが、これに限らず、測定管の測定部の内壁断面
を楕円形または長方形にした前記第2または第3の実施
の形態の電磁流量計において、測定管の測定部の内壁断
面を出入口よりも小さな断面積とするようにしても、本
実施の形態の場合と同様の作用効果を得ることが可能で
ある。
(Modification) In the electromagnetic flowmeter of the present embodiment, the inner wall section of the measuring section of the measuring tube is different from the electromagnetic flowmeter of the first embodiment in which the inner wall section of the measuring section of the measuring pipe is flattened. Is described as having a smaller cross-sectional area than the entrance and exit. However, the present invention is not limited to this. In the electromagnetic flow meter according to the second or third embodiment in which the inner wall cross section of the measuring portion of the measuring tube is made elliptical or rectangular. Even when the cross section of the inner wall of the measuring section of the measuring tube is smaller than the entrance and exit, the same operation and effect as in the case of the present embodiment can be obtained.

【0048】(第5の実施の形態)図5は、本実施の形
態による電磁流量計の測定部の構成例を示す断面図であ
る。
(Fifth Embodiment) FIG. 5 is a sectional view showing an example of the configuration of a measuring section of an electromagnetic flowmeter according to the present embodiment.

【0049】本実施の形態の電磁流量計は、図5に示す
ように、測定部の外壁断面を四角形にし、内部を被測定
流体が流れる測定管51と、測定管51を横切る両方の
平面に配置され、被測定流体に測定管51の管軸方向と
ほぼ直交する方向の磁界を与える一対のコイル52と、
測定管51のコイル52とほぼ直交する方向の両方の平
面に対向配置され、磁界中を被測定流体が移動すること
によって発生する起電力を取り出す一対の電極53と、
測定管51、コイル52、および電極53を取り囲むよ
うに配置され、コイル52のコアおよび帰磁路を形成す
るヨーク54とから構成している。
As shown in FIG. 5, the electromagnetic flow meter according to the present embodiment has a rectangular section on the outer wall of the measuring section, and has a measuring pipe 51 inside which the fluid to be measured flows and a plane crossing the measuring pipe 51. A pair of coils 52 arranged to apply a magnetic field to the fluid to be measured in a direction substantially perpendicular to the tube axis direction of the measurement tube 51;
A pair of electrodes 53 disposed opposite to both planes in a direction substantially orthogonal to the coil 52 of the measurement tube 51 to extract an electromotive force generated by the movement of the fluid to be measured in the magnetic field;
It is arranged so as to surround the measurement tube 51, the coil 52, and the electrode 53, and includes a core of the coil 52 and a yoke 54 forming a return path.

【0050】次に、以上のように構成した本実施の形態
の電磁流量計においては、測定管51の測定部の外壁断
面を四角形としていることにより、電磁流量計の構成部
品が平面に対して取り付けられるため、湾曲加工が不要
となり、測定管51への密着性も良くすることができ
る。
Next, in the electromagnetic flow meter according to the present embodiment configured as described above, since the cross section of the outer wall of the measuring section of the measuring tube 51 is rectangular, the components of the electromagnetic flow meter can be arranged with respect to a plane. Since it is attached, bending work is not required, and the adhesion to the measurement tube 51 can be improved.

【0051】また、電磁流量計の構成部品の梱包を簡単
に行なうことができる。
Further, the components of the electromagnetic flowmeter can be easily packed.

【0052】これにより、電磁流量計を生産する際に加
工工程が少なくなり、組み立て精度が向上し、輸送効率
が良くなるため、生産性を向上することができる。
This reduces the number of processing steps when producing the electromagnetic flow meter, improves the assembly accuracy, and improves the transport efficiency, so that the productivity can be improved.

【0053】上述したように、本実施の形態の電磁流量
計では、測定管51の測定部の外壁断面を四角形とする
ようにしているので、電磁流量計の構成部品が平面に対
して取り付けられるため、湾曲加工が不要となり、測定
管への密着性も良くすることができると共に、電磁流量
計の構成部品の梱包を簡単に行なうことが可能となる。
これにより、電磁流量計を生産する際に加工工程が少な
くなり、組み立て精度が向上し、輸送効率が良くなるた
め、生産性を向上することができる。
As described above, in the electromagnetic flow meter according to the present embodiment, since the outer wall section of the measuring section of the measuring tube 51 is made rectangular, the components of the electromagnetic flow meter are mounted on a flat surface. Therefore, the bending process is not required, the adhesion to the measuring tube can be improved, and the components of the electromagnetic flowmeter can be easily packed.
Thereby, when manufacturing the electromagnetic flow meter, the number of processing steps is reduced, assembling accuracy is improved, and transportation efficiency is improved, so that productivity can be improved.

【0054】[0054]

【発明の効果】以上説明したように本発明によれば、低
い導電率の被測定流体や微少な流れの流速計測を確実に
行なって流量計測の性能を向上することが可能で消費電
力が小さい電磁流量計が提供できる。
As described above, according to the present invention, the flow rate measurement performance can be improved by reliably measuring the flow rate of a fluid to be measured having a low conductivity or a minute flow, and the power consumption can be reduced. An electromagnetic flow meter can be provided.

【0055】また、本発明によれば、生産性を向上する
ことが可能な電磁流量計が提供できる。
Further, according to the present invention, it is possible to provide an electromagnetic flowmeter capable of improving productivity.

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

【図1】本発明による電磁流量計の測定部の第1の実施
の形態を示す断面図。
FIG. 1 is a sectional view showing a first embodiment of a measuring unit of an electromagnetic flowmeter according to the present invention.

【図2】本発明による電磁流量計の測定部の第2の実施
の形態を示す断面図。
FIG. 2 is a sectional view showing a second embodiment of the measuring section of the electromagnetic flow meter according to the present invention.

【図3】本発明による電磁流量計の測定部の第3の実施
の形態を示す断面図。
FIG. 3 is a sectional view showing a third embodiment of the measuring section of the electromagnetic flow meter according to the present invention.

【図4】本発明による電磁流量計の測定部の第4の実施
の形態を示す横断面図および縦断面図。
FIGS. 4A and 4B are a cross-sectional view and a vertical cross-sectional view illustrating a fourth embodiment of the measuring unit of the electromagnetic flowmeter according to the present invention.

【図5】本発明による電磁流量計の測定部の第5の実施
の形態を示す断面図。
FIG. 5 is a sectional view showing a fifth embodiment of the measuring section of the electromagnetic flow meter according to the present invention.

【図6】従来の電磁流量計の測定部の構成例を示す断面
図。
FIG. 6 is a cross-sectional view illustrating a configuration example of a measurement unit of a conventional electromagnetic flowmeter.

【図7】従来の電磁流量計の計測原理を示す概念図。FIG. 7 is a conceptual diagram showing the measurement principle of a conventional electromagnetic flow meter.

【符号の説明】[Explanation of symbols]

1…測定管 12…コイル 13…電極 14…ヨーク 21…測定芦 22…コイル 23…電極 24…ヨーク 31…測定管 32…コイル 33…電極 34…ヨーク 41…測定管 42…コイル 43…電極 44…ヨーク 51…測定管 52…コイル 53…電極 54…ヨーク 61…測定管 62…コイル 63…電極 64…ヨーク 71…磁東密度 72…移動速度 73…導体の幅 74…起電力。 DESCRIPTION OF SYMBOLS 1 ... Measuring tube 12 ... Coil 13 ... Electrode 14 ... Yoke 21 ... Measuring reed 22 ... Coil 23 ... Electrode 24 ... Yoke 31 ... Measuring tube 32 ... Coil 33 ... Electrode 34 ... Yoke 41 ... Measuring tube 42 ... Coil 43 ... Electrode 44 ... Yoke 51 ... Measurement tube 52 ... Coil 53 ... Electrode 54 ... Yoke 61 ... Measurement tube 62 ... Coil 63 ... Electrode 64 ... Yoke 71 ... Magnetic east density 72 ... Movement speed 73 ... Conductor width 74 ... Electromotive force.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 飯島 拓也 東京都府中市東芝町1番地 株式会社東芝 府中工場内 Fターム(参考) 2F035 BA01  ──────────────────────────────────────────────────続 き Continued on the front page (72) Inventor Takuya Iijima 1 Toshiba-cho, Fuchu-shi, Tokyo F-term in the Fuchu factory of Toshiba Corporation (reference) 2F035 BA01

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 測定部の内壁断面を偏平にし、内部を被
測定流体が流れる測定管と、 前記測定管の偏平にして間隔が短くなった面に配置さ
れ、前記被測定流体に測定管の管軸方向とほぼ直交する
方向の磁界を与えるコイルと、 前記測定管の偏平にして間隔が長くなった面に対向配置
され、前記磁界中を被測定流体が移動することによって
発生する起電力を取り出す一対の電極と、 前記測定管、コイル、および電極を取り囲むように配置
され、前記コイルのコアおよび帰磁路を形成するヨーク
と、 を備えて成ることを特徴とする電磁流量計。
1. A measuring pipe in which a cross section of an inner wall of a measuring section is flattened and a fluid to be measured flows inside the measuring pipe; A coil for applying a magnetic field in a direction substantially perpendicular to the tube axis direction, and an electromotive force generated when the fluid to be measured moves in the magnetic field, the coil being arranged to face the flattened surface of the measurement tube at a longer interval. An electromagnetic flowmeter comprising: a pair of electrodes to be taken out; and a yoke arranged to surround the measurement tube, the coil, and the electrode, and to form a core and a return path of the coil.
【請求項2】 測定部の内壁断面を楕円形にし、内部を
被測定流体が流れる測定管と、 前記測定管の楕円形にして間隔が短くなった面に配置さ
れ、前記被測定流体に測定管の管軸方向とほぼ直交する
方向の磁界を与えるコイルと、 前記測定管の楕円形にして間隔が長くなった面に対向配
置され、前記磁界中を被測定流体が移動することによっ
て発生する起電力を取り出す一対の電極と、 前記測定管、コイル、および電極を取り囲むように配置
され、前記コイルのコアおよび帰磁路を形成するヨーク
と、 を備えて成ることを特徴とする電磁流量計。
2. A measuring pipe having an elliptical inner wall cross section and a measuring pipe through which a fluid to be measured flows, and an elliptical surface of the measuring pipe arranged at a shorter interval to measure the fluid to be measured. A coil for applying a magnetic field in a direction substantially perpendicular to the tube axis direction of the tube; and a coil which is disposed opposite to the elliptical surface of the measurement tube having a longer interval, and which is generated when the fluid to be measured moves in the magnetic field. An electromagnetic flowmeter comprising: a pair of electrodes for extracting an electromotive force; and a yoke arranged to surround the measurement tube, the coil, and the electrode, and to form a core and a return path of the coil. .
【請求項3】 測定部の内壁断面を長方形にし、内部を
被測定流体が流れる測定管と、 前記測定管の長方形にして間隔が短くなった面に配置さ
れ、前記被測定流体に測定管の管軸方向とほぼ直交する
方向の磁界を与えるコイルと、 前記測定管の長方形にして間隔が長くなった面に対向配
置され、前記磁界中を被測定流体が移動することによっ
て発生する起電力を取り出す一対の電極と、 前記測定管、コイル、および電極を取り囲むように配置
され、前記コイルのコアおよび帰磁路を形成するヨーク
と、 を備えて成ることを特徴とする電磁流量計。
3. The measuring section has a rectangular inner wall cross section, the inside of which is arranged on a measuring pipe through which a fluid to be measured flows, and a rectangular section of the measuring pipe, which is disposed on a surface with a short interval. A coil that applies a magnetic field in a direction substantially perpendicular to the tube axis direction; and a coil that is disposed to face a rectangular and long-spaced surface of the measurement tube, and generates an electromotive force generated when the fluid to be measured moves in the magnetic field. An electromagnetic flowmeter comprising: a pair of electrodes to be taken out; and a yoke arranged to surround the measurement tube, the coil, and the electrode, and to form a core and a return path of the coil.
【請求項4】 前記請求項1乃至請求項3のいずれか1
項に記載の電磁流量計において、 前記測定管の測定部の内壁断面積を出入口よりも小さな
断面積としたことを特徴とする電磁流量計。
4. The method according to claim 1, wherein
3. The electromagnetic flowmeter according to claim 1, wherein the cross-sectional area of the inner wall of the measuring section of the measuring tube is smaller than that of the entrance.
【請求項5】 測定部の外壁断面を四角形にし、内部を
被測定流体が流れる測定管と、 前記測定管を横切る両方の平面に配置され、前記被測定
流体に測定管の管軸方向とほぼ直交する方向の磁界を与
えるコイルと、 前記測定管のコイルとほぼ直交する方向の両方の平面に
対向配置され、前記磁界中を被測定流体が移動すること
によって発生する起電力を取り出す一対の電極と、 前記測定管、コイル、および電極を取り囲むように配置
され、前記コイルのコアおよび帰磁路を形成するヨーク
と、 を備えて成ることを特徴とする電磁流量計。
5. The measuring section has a rectangular outer wall cross section, and has a measuring pipe through which a fluid to be measured flows, and is disposed on both planes crossing the measuring pipe. A coil for providing a magnetic field in a direction perpendicular to the coil, and a pair of electrodes disposed opposite to both planes in a direction substantially perpendicular to the coil of the measurement tube and for extracting an electromotive force generated by movement of the fluid to be measured in the magnetic field And a yoke arranged to surround the measuring tube, the coil, and the electrode, and forming a core and a return path of the coil.
JP2000049886A 2000-02-25 2000-02-25 Electromagnetic flow meter Pending JP2001241981A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2000049886A JP2001241981A (en) 2000-02-25 2000-02-25 Electromagnetic flow meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2000049886A JP2001241981A (en) 2000-02-25 2000-02-25 Electromagnetic flow meter

Publications (1)

Publication Number Publication Date
JP2001241981A true JP2001241981A (en) 2001-09-07

Family

ID=18571752

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2000049886A Pending JP2001241981A (en) 2000-02-25 2000-02-25 Electromagnetic flow meter

Country Status (1)

Country Link
JP (1) JP2001241981A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005265831A (en) * 2004-02-19 2005-09-29 Yokogawa Electric Corp Electromagnetic flow meter
JP2006162615A (en) * 2004-12-02 2006-06-22 Krohne Ag Magnetic induction flow meter and method of manufacturing magnetic induction flow meter
CN103134558A (en) * 2011-12-02 2013-06-05 克洛纳有限公司 Magnetic-inductive flow measuring apparatus
CN104101391A (en) * 2013-04-08 2014-10-15 Smc株式会社 Electromagnetic flowmeter
DE102016112742A1 (en) * 2016-07-12 2018-01-18 Endress+Hauser Flowtec Ag Method for measuring the flow velocity or the volume flow of a medium by means of a magnetic-inductive flowmeter and a magnetic-inductive flowmeter

Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005265831A (en) * 2004-02-19 2005-09-29 Yokogawa Electric Corp Electromagnetic flow meter
JP2006162615A (en) * 2004-12-02 2006-06-22 Krohne Ag Magnetic induction flow meter and method of manufacturing magnetic induction flow meter
CN103134558A (en) * 2011-12-02 2013-06-05 克洛纳有限公司 Magnetic-inductive flow measuring apparatus
EP2600119A1 (en) * 2011-12-02 2013-06-05 Krohne AG Magnetic-inductive flow measuring apparatus
JP2013117531A (en) * 2011-12-02 2013-06-13 Krohne Ag Magnetic induction type flow measurement device and measurement tube
RU2594620C2 (en) * 2011-12-02 2016-08-20 Кроне Аг Magnetic-inductive flow meter
CN103134558B (en) * 2011-12-02 2016-09-21 克洛纳有限公司 Magnetic-inductive flow measurement instrument
CN104101391A (en) * 2013-04-08 2014-10-15 Smc株式会社 Electromagnetic flowmeter
JP2014202662A (en) * 2013-04-08 2014-10-27 Smc株式会社 Electromagnetic flowmeter
US9109933B2 (en) 2013-04-08 2015-08-18 Smc Corporation Electromagnetic flowmeter
DE102016112742A1 (en) * 2016-07-12 2018-01-18 Endress+Hauser Flowtec Ag Method for measuring the flow velocity or the volume flow of a medium by means of a magnetic-inductive flowmeter and a magnetic-inductive flowmeter
US11029182B2 (en) 2016-07-12 2021-06-08 Endress+Hauser Flowtec Ag Magnetic-inductive flowmeter and method for measuring the flow velocity of low conductivity media with a narrowing measuring tube and a field guide-back device

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