JPS6014175Y2 - electromagnetic flow meter - Google Patents
electromagnetic flow meterInfo
- Publication number
- JPS6014175Y2 JPS6014175Y2 JP8992079U JP8992079U JPS6014175Y2 JP S6014175 Y2 JPS6014175 Y2 JP S6014175Y2 JP 8992079 U JP8992079 U JP 8992079U JP 8992079 U JP8992079 U JP 8992079U JP S6014175 Y2 JPS6014175 Y2 JP S6014175Y2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- conduit
- magnetic pole
- electromagnetic flowmeter
- shaped
- 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
Landscapes
- Measuring Volume Flow (AREA)
Description
【考案の詳細な説明】
この考案は電磁流量計に関し、特に小口径電磁流量計を
容易に小型化できるようにしたものである。[Detailed Description of the Invention] This invention relates to an electromagnetic flowmeter, and in particular allows a small-diameter electromagnetic flowmeter to be easily miniaturized.
電磁流量計の励磁装置の一つを構造としてC字状磁気コ
アを用いたものがある。There is one that uses a C-shaped magnetic core as one of the excitation devices of an electromagnetic flowmeter.
このC字状磁気コアを用いた励磁装置は導管に対して一
方側から着脱できることから組立てが容易にできる点と
、小形軽量に作ることができる点で優れている。This excitation device using a C-shaped magnetic core is superior in that it can be easily assembled because it can be attached to and detached from one side of the conduit, and that it can be made small and lightweight.
然るにこのC字状磁気コアを用いた励磁装置は磁極間を
磁気的に連結する継鉄が一方側だけに存在するため、磁
界分界が乱れる欠点がある。However, the excitation device using this C-shaped magnetic core has the drawback that the magnetic field is disturbed because the yoke that magnetically connects the magnetic poles is present on only one side.
この考案はこの欠侭を一掃し測定誤差が小さいC字状磁
気コアを用いた電磁流量計を提供しようとするものであ
る。This invention aims to eliminate this deficiency and provide an electromagnetic flowmeter using a C-shaped magnetic core with small measurement errors.
従来の小口径電磁流量計は例えば第1図に示すように構
成される。A conventional small-diameter electromagnetic flowmeter is configured as shown in FIG. 1, for example.
第1図において1は被測定流体を流す導管である。In FIG. 1, 1 is a conduit through which a fluid to be measured flows.
導管1はその管軸に挾んで互に180°異なる位置に電
極2−2が取付けられる。Electrodes 2-2 are attached to the conduit 1 at positions 180° apart from each other across the tube axis.
電極2−2を結ぶ線と直交する方向にC字状磁気コア3
の磁極面3a、3bが設けられ、励磁コイル4−4が巻
装され、導管1内に電極2−2を結ぶ線を直交する方向
に磁界を形成するようにしている。C-shaped magnetic core 3 in the direction perpendicular to the line connecting the electrodes 2-2.
magnetic pole surfaces 3a and 3b are provided, and an excitation coil 4-4 is wound around the conduit 1 to form a magnetic field in a direction perpendicular to the line connecting the electrodes 2-2.
この構造を採る電磁流量計において全体の形状を小型化
するにはC字状コア3の背面部3cを導管1に近ずける
ようにC字状コア2を作ることが考えられる。In order to reduce the overall size of an electromagnetic flowmeter having this structure, it is conceivable to make the C-shaped core 2 so that the back surface 3c of the C-shaped core 3 is closer to the conduit 1.
然し乍らC字状コア3の背面部3cを導管1に近ずける
と、第2図に示すように磁極面3a、3b間で形成され
るはずの磁界が磁極面3aと背面部3c及び背面部3c
と磁極面3b間にも形成される。However, when the back surface 3c of the C-shaped core 3 is brought closer to the conduit 1, the magnetic field that is supposed to be formed between the magnetic pole surfaces 3a and 3b as shown in FIG. 3c
It is also formed between the magnetic pole face 3b and the magnetic pole face 3b.
この結果導管1内の磁界分布はC字状コア3の背面部3
cに近い側が乱れる。As a result, the magnetic field distribution inside the conduit 1 is
The side near c is disturbed.
この磁界分布の乱れは電極2の位置で最も大きく、軸対
称でない流速分布の流れに対して測定誤差を生じる。This disturbance in the magnetic field distribution is greatest at the position of the electrode 2, and causes measurement errors for flows with a non-axially symmetric flow velocity distribution.
このため従来はC字状コア3の背面部3cを導管1から
充分遠ざけ磁極面3a、3b間で形成される磁界を乱さ
ないようにしている。For this reason, conventionally, the back surface 3c of the C-shaped core 3 is kept sufficiently away from the conduit 1 so as not to disturb the magnetic field formed between the magnetic pole faces 3a and 3b.
よって全体の形状は大型になっている。Therefore, the overall shape is large.
この考案の目的はC字状コア3の背面部3Cを導管1に
近ずけて小型化を達すると共に磁界分布の乱れを少なく
し小型ながら精度が高い小口径電磁流量計を提供するに
ある。The purpose of this invention is to provide a small-diameter electromagnetic flowmeter that is compact but highly accurate by bringing the back surface 3C of the C-shaped core 3 closer to the conduit 1 to achieve miniaturization and to reduce disturbances in the magnetic field distribution.
この考案では導管1の管軸を含み電極2−2を結ぶ線と
直交する面に対し、磁気コアの磁極面を非対称に形成し
、この磁極面の非対称によって導管内の磁界分布を均一
化するように構成するものである。In this device, the magnetic pole surface of the magnetic core is formed asymmetrically with respect to a plane that includes the tube axis of the conduit 1 and is perpendicular to the line connecting the electrodes 2-2, and the asymmetry of the magnetic pole surface equalizes the magnetic field distribution within the conduit. It is configured as follows.
以下にこの考案の一実施例を図面を用いて詳細に説明す
る。An embodiment of this invention will be described below in detail with reference to the drawings.
第3図にこの考案の一実施例を示す。FIG. 3 shows an embodiment of this invention.
この第3図の実施例ではC字状磁気コア3の磁極面3a
。In the embodiment shown in FIG. 3, the magnetic pole surface 3a of the C-shaped magnetic core 3 is
.
3bの背面3cに近い側の辺に台形状の断面形状を持つ
磁性体から戊る突条5−5を取付け、この磁性体から戊
る突条5−5の取付けによって磁極面3a、3bは導管
1の管軸を含み電極2−2を結ぶ面と直交する面に対し
非対称となる。A protrusion 5-5 made of a magnetic material having a trapezoidal cross-sectional shape is attached to the side near the back surface 3c of 3b, and by attaching the protrusion 5-5 made of the magnetic material, the magnetic pole faces 3a and 3b are It is asymmetrical with respect to a plane that includes the tube axis of the conduit 1 and is perpendicular to the plane that connects the electrodes 2-2.
この磁極面の非対称により磁極面3at3bと背面部3
Cとにより形成される磁界は充分減少し、第3図に示す
ような磁界分布にすることができた。Due to the asymmetry of this magnetic pole surface, the magnetic pole surface 3at3b and the back surface 3
The magnetic field formed by C was sufficiently reduced, and the magnetic field distribution as shown in FIG. 3 was achieved.
このときの実際の各部の寸法を示すと、導管1の内径=
10orIrI4、磁極面3a、3b間の間隙:125
閣、磁極面の巾W : 95mm、磁極面の奥行: 9
5mm。To show the actual dimensions of each part at this time, the inner diameter of conduit 1 =
10orIrI4, gap between magnetic pole faces 3a and 3b: 125
Cabinet, width W of magnetic pole surface: 95mm, depth of magnetic pole surface: 9
5mm.
磁極の一端と背面部3cまでの距離L1 : 313m
5゜C字状コアの折曲り部分から導管1の管軸までの距
離L2 : 100mm、このような寸法のC字状コア
3に対し磁性突条5−5の寸法は第4図に示すように底
面L3: 187701.高さL4:9mm、上辺の長
さ′L5: 3 WAz全体の長さ95rIrI14で
あった。Distance L1 from one end of the magnetic pole to the back part 3c: 313m
5° Distance L2 from the bent part of the C-shaped core to the pipe axis of the conduit 1: 100 mm.For the C-shaped core 3 having such dimensions, the dimensions of the magnetic protrusion 5-5 are as shown in FIG. Bottom surface L3: 187701. Height L4: 9 mm, length of upper side 'L5: 3 WAz overall length 95rIrI14.
上述のような磁性体から戒る突条5−5を磁極面3a、
3bに取付けることにより導管1内の磁界分布は均一化
され流量測定精度を向上することができた。The protrusion 5-5 that prevents the magnetic material as described above is attached to the magnetic pole surface 3a,
3b, the magnetic field distribution within the conduit 1 was made uniform and the accuracy of flow measurement could be improved.
尚、磁極面3a、3bに取付けた磁性体から戒る突条5
−5の断面形状は第5図乃至第11図に示すように各種
の形状のものが考えられる。In addition, the protrusions 5 that should be avoided from the magnetic material attached to the magnetic pole surfaces 3a and 3b
-5 can have various shapes as shown in FIGS. 5 to 11.
またこのように磁性体から戊る突条5−5を附加して磁
極面3a、3bを非対称化するのみならず、第12図に
示すように磁極面3a、3bの背面部3Cから最も離れ
た位置の辺に切欠6−6を形成するようにしても良い。In addition, by adding the protrusions 5-5 cut out from the magnetic material in this way, not only the magnetic pole faces 3a and 3b are made asymmetrical, but also the pole faces 3a and 3b are furthest away from the back surface 3C of the magnetic pole faces 3a and 3b, as shown in FIG. A notch 6-6 may be formed on the side at the position where the cutout 6-6 is located.
上述したようにこの考案によればC字状コア3の背面部
3cを導管1に近ずけても簡単な構成によって導管1内
の磁界分布を均一化することができた。As described above, according to this invention, even if the back surface 3c of the C-shaped core 3 is brought closer to the conduit 1, the magnetic field distribution within the conduit 1 can be made uniform with a simple configuration.
よって小型ながら測定精度が高い小口径の電磁流量計を
得ることができ、その効果は実用に供して頗る大である
。Therefore, it is possible to obtain a small-diameter electromagnetic flowmeter that is compact but has high measurement accuracy, and its effects are extremely large in practical use.
第1図は従来の電磁流量計を説明するための断面図、第
2図は従来の電磁流量計の不都合を説明するための断面
図、第3図はこの考案の一実施例を示す断面図、第4図
はこの考案の要部の実際の寸法を一例を説明する側面図
、第5図乃至第11図はその要部の他の例を示す側面図
、第12図はこの考案の他の実施例を示す断面図である
。
1・・・・・・導管、2・・・・・・電極、3・・・・
・・C字状磁気コア、3ay3b・・・・・・磁極面、
3c・・・・・・背面部、4・・・・・・励磁コイル。Fig. 1 is a cross-sectional view to explain a conventional electromagnetic flowmeter, Fig. 2 is a cross-sectional view to explain the disadvantages of the conventional electromagnetic flowmeter, and Fig. 3 is a cross-sectional view showing an embodiment of this invention. , FIG. 4 is a side view illustrating one example of the actual dimensions of the main part of this invention, FIGS. 5 to 11 are side views showing other examples of the main part, and FIG. FIG. 1... Conduit, 2... Electrode, 3...
...C-shaped magnetic core, 3ay3b...magnetic pole surface,
3c... Back part, 4... Excitation coil.
Claims (1)
挾むように配置され、前記磁気コアに励磁コイルが施さ
れた電磁流量計において、前記導管の管軸を含み両磁極
面に直角な管軸方向の断面に対し前記背面部側の前記磁
極面に磁性体の突条を形成するか前記背面部側とは反対
の前記磁極面に切欠きを形成するかの何れか一方を選定
し、前記導管内の磁界分布を均一化するように構成した
電磁流量計。In an electromagnetic flowmeter in which magnetic pole surfaces are arranged at both ends of a C-shaped magnetic core having a back surface so as to sandwich a conduit, and an excitation coil is applied to the magnetic core, a C-shaped magnetic core including a tube axis of the conduit and perpendicular to both magnetic pole surfaces is provided. Either a protrusion of a magnetic material is formed on the magnetic pole face on the back side with respect to the cross section in the tube axis direction, or a notch is formed on the magnetic pole face opposite to the back side. , an electromagnetic flowmeter configured to equalize magnetic field distribution within the conduit.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8992079U JPS6014175Y2 (en) | 1979-06-29 | 1979-06-29 | electromagnetic flow meter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8992079U JPS6014175Y2 (en) | 1979-06-29 | 1979-06-29 | electromagnetic flow meter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS569018U JPS569018U (en) | 1981-01-26 |
| JPS6014175Y2 true JPS6014175Y2 (en) | 1985-05-07 |
Family
ID=29323044
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8992079U Expired JPS6014175Y2 (en) | 1979-06-29 | 1979-06-29 | electromagnetic flow meter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6014175Y2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2024208817A1 (en) * | 2023-04-06 | 2024-10-10 | Sensus Spectrum Llc. | Electromagnetic flow sensor |
-
1979
- 1979-06-29 JP JP8992079U patent/JPS6014175Y2/en not_active Expired
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2024208817A1 (en) * | 2023-04-06 | 2024-10-10 | Sensus Spectrum Llc. | Electromagnetic flow sensor |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS569018U (en) | 1981-01-26 |
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