JPH0351707Y2 - - Google Patents
Info
- Publication number
- JPH0351707Y2 JPH0351707Y2 JP723484U JP723484U JPH0351707Y2 JP H0351707 Y2 JPH0351707 Y2 JP H0351707Y2 JP 723484 U JP723484 U JP 723484U JP 723484 U JP723484 U JP 723484U JP H0351707 Y2 JPH0351707 Y2 JP H0351707Y2
- Authority
- JP
- Japan
- Prior art keywords
- signal lead
- lead wire
- tube
- magnetic field
- metal plate
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 claims description 26
- 238000005259 measurement Methods 0.000 claims description 11
- 239000002184 metal Substances 0.000 claims description 9
- 239000012530 fluid Substances 0.000 claims description 8
- 230000005284 excitation Effects 0.000 claims description 7
- 230000002093 peripheral effect Effects 0.000 description 3
- 230000010363 phase shift Effects 0.000 description 3
- 239000000853 adhesive Substances 0.000 description 2
- 230000001070 adhesive effect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000009434 installation Methods 0.000 description 2
- 239000011810 insulating material Substances 0.000 description 2
- 229910000906 Bronze Inorganic materials 0.000 description 1
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 1
- 239000004809 Teflon Substances 0.000 description 1
- 229920006362 Teflon® Polymers 0.000 description 1
- 238000005452 bending Methods 0.000 description 1
- 239000010974 bronze Substances 0.000 description 1
- KUNSUQLRTQLHQQ-UHFFFAOYSA-N copper tin Chemical compound [Cu].[Sn] KUNSUQLRTQLHQQ-UHFFFAOYSA-N 0.000 description 1
- 238000010292 electrical insulation Methods 0.000 description 1
- 230000005674 electromagnetic induction Effects 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 229920001084 poly(chloroprene) Polymers 0.000 description 1
- 238000005476 soldering Methods 0.000 description 1
- 125000000391 vinyl group Chemical group [H]C([*])=C([H])[H] 0.000 description 1
- 229920002554 vinyl polymer Polymers 0.000 description 1
Landscapes
- Measuring Volume Flow (AREA)
Description
【考案の詳細な説明】
〔考案の技術分野〕
本考案は測定管内を流れる被測定流体の流量を
電気的に測定する電磁流量計に関する。[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to an electromagnetic flowmeter that electrically measures the flow rate of a fluid to be measured flowing within a measuring pipe.
一般に、電磁流量計はフアラデーの電磁誘導現
象を利用して測定管内を流れる導電性流体の流量
を電気信号に変換して測定を行うものであり、従
来より第1図に示すように構成されている。すな
わち符号1で示すものは両端に接続配管用のフラ
ンジ1a,1bを有する測定管で、内壁に例えば
テフロン、ネオプレン等の絶縁材からなるライニ
ング2が設けられている。この測定管1の外側に
は管内の被測定流体の流れ方向と直角に磁界を形
成する一対の励磁コイル(図示せず)が互いに対
向して取付けられている。また測定管1の管壁に
は、一対の電極3,4が測定管1内の被測定流体
の流れ方向と直角に磁界を介して互いに対向する
ように設けられている。これら電極3,4には接
続用端子盤5上の端子に電気的に接続するための
信号リード線6,7が前記測定管1の外側にそれ
ぞれ同方向に1/4周程度沿つた状態で取付けられ
ている。
In general, an electromagnetic flowmeter converts the flow rate of a conductive fluid flowing in a measurement pipe into an electrical signal using Faraday's electromagnetic induction phenomenon to measure the flow rate, and has conventionally been configured as shown in Figure 1. There is. That is, the measuring tube designated by the reference numeral 1 has flanges 1a and 1b for connection piping at both ends, and a lining 2 made of an insulating material such as Teflon or neoprene is provided on the inner wall. A pair of excitation coils (not shown) are attached to the outside of the measurement tube 1 to face each other and to form a magnetic field perpendicular to the flow direction of the fluid to be measured inside the tube. Further, a pair of electrodes 3 and 4 are provided on the wall of the measuring tube 1 so as to face each other via a magnetic field at right angles to the flow direction of the fluid to be measured in the measuring tube 1 . These electrodes 3 and 4 have signal lead wires 6 and 7 for electrically connecting them to the terminals on the connection terminal board 5, respectively, extending about 1/4 of the way around the outside of the measuring tube 1 in the same direction. installed.
ところが、前記した従来の電磁流量計において
は、往々にして信号リード線6,7が励磁コイル
により形成される磁界に測定管1の側方からみて
傾斜して取付けられてしまうため、両電極3,4
を結ぶ線Aおよび両信号リード線6,7によつて
形成される面積Sに二次的に比例した90°位相の
ずれによる雑音起電力が生じ、発信器側に雑音と
して送られるという不都合がある。 However, in the conventional electromagnetic flowmeter described above, the signal lead wires 6 and 7 are often attached to the magnetic field formed by the excitation coil at an angle when viewed from the side of the measuring tube 1. ,4
There is an inconvenience that a noise electromotive force is generated due to a 90° phase shift that is quadratically proportional to the area S formed by the line A connecting the signal leads 6 and 7, and is sent as noise to the transmitter side. be.
そこで、このような問題を解決するために、測
定管1の外周面に周方向に延在する溝(図示せ
ず)を設け、この溝内に信号リード線6,7をテ
ープ、接着剤により固定した電磁流量計が提案さ
れている。 Therefore, in order to solve this problem, a groove (not shown) extending in the circumferential direction is provided on the outer peripheral surface of the measuring tube 1, and the signal lead wires 6 and 7 are inserted into the groove using tape or adhesive. Fixed electromagnetic flowmeters have been proposed.
しかるに、この場合信号リード線6,7の取付
作業を煩雑にし、また加工工程数が嵩むという欠
点がある。 However, in this case, there is a drawback that the installation work of the signal lead wires 6, 7 is complicated and the number of processing steps is increased.
本考案はこのような事情に鑑みなされたもの
で、電極の信号リード線を弾性を有する帯状の金
属板で形成するというきわめて簡単な構成によ
り、90°位相のずれによる雑音を可能な限り小さ
くすることが確実に行えるだけでなく、信号リー
ド線の取付作業を容易に行える電磁流量計を提供
するものである。以下、その構成等を図に示す実
施例によつて詳細に説明する。
The present invention was developed in view of these circumstances, and uses an extremely simple structure in which the signal lead wire of the electrode is formed from an elastic band-shaped metal plate, thereby minimizing the noise caused by a 90° phase shift. The purpose of the present invention is to provide an electromagnetic flowmeter that not only allows reliable operation but also facilitates the installation work of signal lead wires. Hereinafter, the configuration and the like will be explained in detail by referring to embodiments shown in the drawings.
第2図および第3図は本考案に係る電磁流量計
の一実施例を示す概略斜視図と断面図、第4図は
同じく電磁流量計に使用される信号リード線を示
す側面図である。これらの図において、11は被
測定流体がその内部を流れる測定管で、内壁に絶
縁材からなるライニング12が設けられており、
外側には管内の被測定流体の流れ方向と直角に磁
界を形成する一対の励磁コイル13が互いに対向
して設けられている。また測定管11の管壁には
一対の電極14が前記磁界を介して互いに対向す
るように設けられ、被測定流体の各点に発生した
起電力を検出するように構成されている。15は
端子16を有する端子盤で、取付けねじ17によ
りケース18に固定されており、前記電極14に
よる起電力の検出値を図示しないコントロール部
に送出するように構成されている。19は前記電
極の信号リード線で、例えばリン青銅板、
SUS304等の弾性を有する板厚0.1〜0.2mm程度の
金属板をプレス加工あるいはエツチングして幅2
〜5mm程度の帯状に形成されており、前記測定管
11の外周方向に延在して測定管11に取付けら
れ、両端がそれぞれ電極14、端子16に接続さ
れている。この信号リード線19には電気絶縁の
ために図中鎖線で示すように熱収縮チユーブやビ
ニールチユーブ20が被覆されている。また信号
リード線19は電極側の一端に取付用の孔として
長孔21が穿設されており、これにより周方向の
長さの調整が可能となり、寸法公差や組立時のば
らつきを吸収することができる。
2 and 3 are a schematic perspective view and a sectional view showing an embodiment of the electromagnetic flowmeter according to the present invention, and FIG. 4 is a side view showing a signal lead wire used in the electromagnetic flowmeter. In these figures, 11 is a measurement tube through which the fluid to be measured flows, and a lining 12 made of an insulating material is provided on the inner wall.
A pair of excitation coils 13 are provided on the outside facing each other to form a magnetic field perpendicular to the flow direction of the fluid to be measured inside the tube. Further, a pair of electrodes 14 are provided on the wall of the measurement tube 11 so as to face each other via the magnetic field, and are configured to detect the electromotive force generated at each point of the fluid to be measured. Reference numeral 15 denotes a terminal board having terminals 16, which is fixed to the case 18 with mounting screws 17, and is configured to send the value of the electromotive force detected by the electrode 14 to a control section (not shown). 19 is a signal lead wire of the electrode, for example, a phosphor bronze plate,
Pressing or etching an elastic metal plate such as SUS304 with a thickness of about 0.1 to 0.2 mm to create a width of 2 mm.
It is formed into a band shape of about 5 mm, extends in the outer circumferential direction of the measuring tube 11 and is attached to the measuring tube 11, and both ends are connected to the electrode 14 and the terminal 16, respectively. This signal lead wire 19 is covered with a heat-shrinkable tube or vinyl tube 20 as shown by the chain line in the figure for electrical insulation. In addition, the signal lead wire 19 has a long hole 21 bored at one end on the electrode side as a mounting hole, which makes it possible to adjust the length in the circumferential direction and absorb dimensional tolerances and variations during assembly. I can do it.
このように構成された電磁流量計においては、
信号リード線19として帯状の金属板を用いてい
るため、金属板幅方向の撓みが無くなり、第5図
に鎖線で示すように信号リード線19が測定管1
1の軸線方向にずれて取付けられることがない。
換言すれば、信号リード線19が測定管11の側
方からみて励磁コイル13により形成される磁界
に傾斜して取付けられることはない。 In the electromagnetic flowmeter configured in this way,
Since a band-shaped metal plate is used as the signal lead wire 19, there is no bending in the width direction of the metal plate, and the signal lead wire 19 is connected to the measuring tube 1 as shown by the chain line in FIG.
1 will not be installed misaligned in the axial direction.
In other words, the signal lead wire 19 is not attached obliquely to the magnetic field formed by the excitation coil 13 when viewed from the side of the measurement tube 11.
また、信号リード線19が弾性を有する金属板
で形成されているため、その弾性を利用して信号
リード線19を測定管11に確実に取付けること
ができる。 Further, since the signal lead wire 19 is formed of an elastic metal plate, the signal lead wire 19 can be reliably attached to the measurement tube 11 by utilizing its elasticity.
さらに、信号リード線19が0.1〜0.2mmの薄い
金属板であるため、励磁コイル13,コア(図示
せず)を測定管11に接近した状態で取付けるこ
とができ、その効率を向上させることができる。 Furthermore, since the signal lead wire 19 is a thin metal plate of 0.1 to 0.2 mm, the excitation coil 13 and core (not shown) can be installed close to the measurement tube 11, improving its efficiency. can.
なお、本考案による電磁流量計の信号リード線
19取付けにおいては、第6図および第7図に示
すように外部端子台22、中継端子台23を用い
て行う場合があり、信号リード線19は一端が外
部端子台22、中継端子台23の端子に半田付け
あるいはねじにより、また他端が電極14にねじ
により取付けられている。ここで前者の場合、後
者の場合に比べて信号リード線19が測定管11
の外周面と大きな間隔を隔てた位置に位置付けら
れているが、測定管11外周面の曲率より僅かに
小さい曲率をもつた形状に信号リード線19を形
成すれば、これを測定管11の外周面に密着して
取付けることができる。この場合、第8図に示す
ように測定管11の外周面に周方向に延在する溝
24を設ければ信号リード線19の取付けが一層
容易に行い得る。ただし、この溝24の深さは信
号リード線19の厚さが薄いため浅くてよく、し
たがつて測定管11の管厚を特に厚くする必要が
ない。 Note that when attaching the signal lead wire 19 of the electromagnetic flowmeter according to the present invention, the external terminal block 22 and the relay terminal block 23 may be used as shown in FIGS. 6 and 7, and the signal lead wire 19 is One end is attached to the terminals of the external terminal block 22 and relay terminal block 23 by soldering or screws, and the other end is attached to the electrode 14 by screws. In the former case, the signal lead wire 19 is connected to the measuring tube 11 compared to the latter case.
However, if the signal lead wire 19 is formed in a shape with a curvature slightly smaller than the curvature of the outer circumferential surface of the measuring tube 11, the signal lead wire 19 can be separated from the outer circumferential surface of the measuring tube 11. Can be mounted closely to the surface. In this case, if a circumferentially extending groove 24 is provided on the outer peripheral surface of the measuring tube 11 as shown in FIG. 8, the signal lead wire 19 can be attached more easily. However, the depth of this groove 24 may be small because the thickness of the signal lead wire 19 is thin, and therefore there is no need to make the measurement tube 11 particularly thick.
以上説明したように本考案によれば、信号リー
ド線を帯状の金属板で形成したので、信号リード
線を測定管の側方からみて励磁コイルにより形成
される磁界と平行な位置に確実に位置付けること
ができ、90°位相のずれによる雑音を可能な限り
確実に小さくすることができる。また、信号リー
ド線の取付けにあたり信号リード線の弾性を利用
して取付けることができるから、従来のようにテ
ープ接着剤を用いる必要がなくなり、その取付作
業をきわめて容易に行うことができる。さらに、
測定管の外周面に溝を設ける必要がないから、加
工工程数を削減できるという効果もある。
As explained above, according to the present invention, since the signal lead wire is formed of a band-shaped metal plate, the signal lead wire can be reliably positioned in a position parallel to the magnetic field formed by the excitation coil when viewed from the side of the measurement tube. This makes it possible to reliably reduce noise due to a 90° phase shift as much as possible. Further, since the signal lead wire can be attached by utilizing its elasticity, there is no need to use tape adhesive as in the conventional case, and the attachment work can be performed extremely easily. moreover,
Since there is no need to provide a groove on the outer peripheral surface of the measuring tube, there is also the effect that the number of processing steps can be reduced.
第1図は従来の電磁流量計を示す概略斜視図、
第2図および第3図は本考案に係る電磁流量計の
一実施例を示す概略斜視図と断面図、第4図は同
じく電磁流量計に使用される信号リード線を示す
側面図、第5図は信号リード線の電極への取付状
態を示す側面図、第6図、第7図および第8図は
信号リード線の取付状態を示す断面図である。
11……測定管、13……励磁コイル、14…
…電極、19……信号リード線。
Figure 1 is a schematic perspective view showing a conventional electromagnetic flowmeter.
2 and 3 are a schematic perspective view and a sectional view showing an embodiment of an electromagnetic flowmeter according to the present invention, FIG. 4 is a side view showing a signal lead wire used in the electromagnetic flowmeter, and FIG. The figure is a side view showing how the signal lead wire is attached to the electrode, and FIGS. 6, 7, and 8 are sectional views showing how the signal lead wire is attached. 11...Measuring tube, 13...Exciting coil, 14...
...Electrode, 19...Signal lead wire.
Claims (1)
れ方向と直角に磁界を形成する一対の励磁コイル
と、前記磁界を介して互いに対向するように管壁
に設けられた一対の電極とを備えた電磁流量計に
おいて、前記電極の信号リード線を弾性を有する
帯状の金属板で形成すると共に、この金属板を前
記測定管の外周方向に延在させたことを特徴とす
る電磁流量計。 A pair of excitation coils are provided outside the measurement tube and form a magnetic field perpendicular to the flow direction of the fluid to be measured in the tube, and a pair of electrodes are provided on the tube wall so as to face each other across the magnetic field. An electromagnetic flowmeter characterized in that the signal lead wire of the electrode is formed of an elastic band-shaped metal plate, and the metal plate extends in the outer circumferential direction of the measurement tube.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP723484U JPS60120323U (en) | 1984-01-24 | 1984-01-24 | electromagnetic flow meter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP723484U JPS60120323U (en) | 1984-01-24 | 1984-01-24 | electromagnetic flow meter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60120323U JPS60120323U (en) | 1985-08-14 |
| JPH0351707Y2 true JPH0351707Y2 (en) | 1991-11-07 |
Family
ID=30485402
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP723484U Granted JPS60120323U (en) | 1984-01-24 | 1984-01-24 | electromagnetic flow meter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60120323U (en) |
-
1984
- 1984-01-24 JP JP723484U patent/JPS60120323U/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60120323U (en) | 1985-08-14 |
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