JPH0428063Y2 - - Google Patents
Info
- Publication number
- JPH0428063Y2 JPH0428063Y2 JP257186U JP257186U JPH0428063Y2 JP H0428063 Y2 JPH0428063 Y2 JP H0428063Y2 JP 257186 U JP257186 U JP 257186U JP 257186 U JP257186 U JP 257186U JP H0428063 Y2 JPH0428063 Y2 JP H0428063Y2
- Authority
- JP
- Japan
- Prior art keywords
- probe
- tube
- velocity
- flow
- current meter
- 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
- 239000000523 sample Substances 0.000 claims description 19
- 239000012530 fluid Substances 0.000 description 9
- 238000005253 cladding Methods 0.000 description 6
- BGPVFRJUHWVFKM-UHFFFAOYSA-N N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] Chemical compound N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] BGPVFRJUHWVFKM-UHFFFAOYSA-N 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 230000004907 flux Effects 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 1
- 238000009826 distribution Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005672 electromagnetic field Effects 0.000 description 1
- 230000005674 electromagnetic induction Effects 0.000 description 1
- 239000000284 extract Substances 0.000 description 1
- 239000011810 insulating material Substances 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 229910001338 liquidmetal Inorganic materials 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- 238000004904 shortening Methods 0.000 description 1
Landscapes
- Measuring Volume Flow (AREA)
Description
【考案の詳細な説明】
産業上の利用分野
本考案は、導電性流体の流速を測定する電磁流
速計のプローブに関し、液体金属流速計、潮流用
流速計などに利用することができる。[Detailed Description of the Invention] Industrial Application Field The present invention relates to an electromagnetic current meter probe for measuring the flow velocity of a conductive fluid, and can be used in liquid metal current meters, tidal flow current meters, and the like.
従来の技術
導電性の流体の流れの速度を測定するために、
電磁式の流速計が用いられている。Prior Art To measure the velocity of a conductive fluid flow,
An electromagnetic current meter is used.
第3図は開きよ内の流体の流速の計測状態を示
す例で、参照符号1は開きよ、2は流体、3は電
磁流速計用のプローブの被覆管、5aおよび5b
はプローブの出力信号を取り出す電磁を示してい
る。第4図は第3図のx−x断面を示している。
プローブの被覆管3の内部には、永久磁石4が組
み込まれ、電極5a,5bが被覆管3の内壁に溶
着されている。 Fig. 3 is an example showing the state of measurement of the flow velocity of a fluid in an open side, where reference numeral 1 indicates the open side, 2 indicates the fluid, 3 indicates the cladding tube of the electromagnetic current meter probe, 5a and 5b.
indicates an electromagnetic field that extracts the output signal of the probe. FIG. 4 shows the xx section of FIG. 3.
A permanent magnet 4 is incorporated inside the cladding tube 3 of the probe, and electrodes 5a and 5b are welded to the inner wall of the cladding tube 3.
この電磁流速計用プローブの出力は、フレミン
グの右手の法則により、磁界を切る流れの速度に
比例した電圧が電極5a,5b間に誘起され、次
式で表わされる。 The output of this electromagnetic current meter probe is expressed by the following equation, in which a voltage proportional to the velocity of the flow that cuts the magnetic field is induced between the electrodes 5a and 5b according to Fleming's right-hand rule.
E=KvB
但し、Eは出力電圧、Bは磁束密度、vは流れの
速度、は電極間の距離、Kはプローブの形状な
どによつて定まる係数である。E=K v B where E is the output voltage, B is the magnetic flux density, v is the velocity of the flow, is the distance between the electrodes, and K is a coefficient determined by the shape of the probe, etc.
考案が解決しようとする問題点
第5図は、開きよ1の深さ方向における開きよ
内の流れの速度vの分布を示す例である。このよ
うに、深さ方向に速度差がある場合、一定の大き
さを持つたプローブで計測すると、そのプローブ
の大きさに相当する深さ領域の平均的な流速を示
すことになり、局所の下速を正しく示さないこと
になる。このため、流反計のプローブ直径をでき
る限り小さくする必要があるが、小型にすること
による製作性の面、および電極間の距離が小さ
くなるために出力が低下することなど、限界があ
る。Problems to be Solved by the Invention FIG. 5 is an example showing the distribution of the velocity v of the flow within the aperture in the depth direction of the aperture 1. In this way, when there is a velocity difference in the depth direction, when measured with a probe of a certain size, it will show the average flow velocity in the depth region corresponding to the size of the probe, and the local This will not indicate the lower speed correctly. For this reason, it is necessary to make the diameter of the probe of the flowmeter as small as possible, but there are limitations such as the reduction in manufacturability due to miniaturization and the reduction in output due to the shortening of the distance between the electrodes.
本考案は上記事情に基いてなされたもので、液
体の流れに急な速度勾配がある場合にでも、より
正確に局所の速度を計測できるような、電磁式の
流速計用プローブを提供することを目的とする。 The present invention has been made based on the above circumstances, and it is an object of the present invention to provide an electromagnetic current velocity probe that can more accurately measure local velocity even when there is a steep velocity gradient in the flow of liquid. With the goal.
問題点を解決するための手段
本考案によれば、偏平な管と、同管内に挿入さ
れた表面と裏面で極性を異にする板状の永久磁石
と、上記管内であつて上記永久磁石の両側へ対向
して配置された一対の電極とを有し、流速の変化
する方向の厚みを小さくしたことを特徴とする電
磁流速計用プローブが提供される。Means for Solving the Problems According to the present invention, a flat tube, a plate-shaped permanent magnet inserted into the tube and having different polarities on the front and back sides, and a permanent magnet inside the tube are provided. Provided is an electromagnetic current meter probe characterized in that it has a pair of electrodes disposed opposite to each other on both sides and has a reduced thickness in the direction in which the flow velocity changes.
実施例
第1図は本考案による電磁流速計用プローブの
外形図、第2図は上面または下面がNまたはSの
極性を有するテープ状の磁石4を挿入した部分の
拡大断面図である。被覆管3は磁石4を挿入した
部分が偏平となつている。製作手順を述べれば、
まず円形の被覆管3をL字状に曲げたあと、電極
5a,5bを円管内に溶着する。つづいて、扁平
にする部分にプレスをかけて、均一に圧縮し、変
形させる。平板状の磁石4を挿入し、電気的絶縁
材(例えばアルミナ)をすきまに充填し先端にキ
ヤツプを溶着して、全体を滑らかに仕上げる。Embodiment FIG. 1 is an external view of a probe for an electromagnetic current meter according to the present invention, and FIG. 2 is an enlarged sectional view of a portion into which a tape-shaped magnet 4 having an N or S polarity on the upper or lower surface is inserted. The portion of the cladding tube 3 into which the magnet 4 is inserted is flat. Describing the manufacturing procedure,
First, the circular cladding tube 3 is bent into an L-shape, and then the electrodes 5a and 5b are welded into the circular tube. Next, press the part to be flattened to uniformly compress and deform it. A flat magnet 4 is inserted, the gap is filled with an electrical insulating material (for example, alumina), a cap is welded to the tip, and the whole is finished smoothly.
作 用
上述のように構成された電磁流速計用プローブ
を流体2の流れの中に挿入すれば、フアラデーの
電磁誘導則によつて、電極5a,5bに流速に応
じた誘導起電力が得られる。Operation When the electromagnetic current meter probe configured as described above is inserted into the flow of the fluid 2, an induced electromotive force corresponding to the flow velocity can be obtained at the electrodes 5a and 5b according to Faraday's law of electromagnetic induction. .
考案の効果
本考案によれば、プローブを偏平化することに
よつて、流体流れの速度勾配を生じている方向に
対するプローブの厚みが薄くなり、流体のより局
所的な流速の検出が可能となつた。Effects of the invention According to the invention, by flattening the probe, the thickness of the probe in the direction in which a fluid flow velocity gradient is generated becomes thinner, making it possible to detect a more local flow velocity of the fluid. Ta.
また、電極間の距離が長くなり、偏平磁石によ
り磁束の幅も大きくなつたので、出力が大きく高
感度になつた。 Additionally, the distance between the electrodes was increased and the width of the magnetic flux was also increased due to the flat magnets, resulting in larger output and higher sensitivity.
第1図は本考案による電磁流速計用プローブを
計測状態で示す外形図、第2図は第1図のy−y
断面を示す図、第3図は従来のプローブを示す外
形図、第4図は第3図のx−x断面を示す図、第
5図は流体流れの速度勾配を示す図である。
1……開きよ、2……流体、3……電磁流速計
用プローブの被覆管、4……磁石、5a,5b…
…電極。
Figure 1 is an external view showing the electromagnetic current meter probe according to the present invention in a measurement state, and Figure 2 is y-y of Figure 1.
FIG. 3 is a diagram showing a cross section, FIG. 3 is an outline diagram showing a conventional probe, FIG. 4 is a diagram showing a cross section taken along line xx in FIG. 3, and FIG. 5 is a diagram showing a velocity gradient of fluid flow. 1... Open, 2... Fluid, 3... Electromagnetic current meter probe cladding tube, 4... Magnet, 5a, 5b...
…electrode.
Claims (1)
極性を異にする板状の永久磁石と、上記管内であ
つて上記永久磁石の両側へ対向して配置された一
対の電極とを有することを特徴とする電磁流速計
用プローブ。 It has a flat tube, a plate-shaped permanent magnet inserted into the tube and having different polarities on the front and back surfaces, and a pair of electrodes arranged inside the tube and facing each other on both sides of the permanent magnet. An electromagnetic current meter probe characterized by:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP257186U JPH0428063Y2 (en) | 1986-01-14 | 1986-01-14 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP257186U JPH0428063Y2 (en) | 1986-01-14 | 1986-01-14 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62115667U JPS62115667U (en) | 1987-07-23 |
| JPH0428063Y2 true JPH0428063Y2 (en) | 1992-07-07 |
Family
ID=30781534
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP257186U Expired JPH0428063Y2 (en) | 1986-01-14 | 1986-01-14 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0428063Y2 (en) |
-
1986
- 1986-01-14 JP JP257186U patent/JPH0428063Y2/ja not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62115667U (en) | 1987-07-23 |
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