JPS61283824A - Electromagnetic flowmeter - Google Patents
Electromagnetic flowmeterInfo
- Publication number
- JPS61283824A JPS61283824A JP12431785A JP12431785A JPS61283824A JP S61283824 A JPS61283824 A JP S61283824A JP 12431785 A JP12431785 A JP 12431785A JP 12431785 A JP12431785 A JP 12431785A JP S61283824 A JPS61283824 A JP S61283824A
- Authority
- JP
- Japan
- Prior art keywords
- wall surface
- flange plate
- metal conduit
- welded
- annular flange
- 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.)
- Granted
Links
Landscapes
- Measuring Volume Flow (AREA)
Abstract
Description
【発明の詳細な説明】
・ 〔産業上の利用分野〕
本発明は、金属導管の両開口端外周に円環状フランジ板
を溶接して固着してなる測定管を備えてなる電磁流量計
の改良に関する。[Detailed Description of the Invention] - [Industrial Application Field] The present invention is an improvement of an electromagnetic flowmeter comprising a measuring tube formed by welding and fixing annular flange plates to the outer periphery of both open ends of a metal conduit. Regarding.
一般に、電磁流量計は、ファラデーの電磁誘導現象を利
用して測定管内を通過する導電性を有する被測定流体の
流量を電気信号に変換し、その流量測定を行なうもので
ある。そして5このような電磁流量計は、測定にあたっ
て可動部分がなく。In general, an electromagnetic flowmeter uses Faraday's electromagnetic induction phenomenon to convert the flow rate of a conductive fluid to be measured passing through a measuring tube into an electrical signal, and measures the flow rate. 5 Such electromagnetic flowmeters have no moving parts during measurement.
また測定のために圧力損失を生じることがなく。Also, there is no pressure loss during measurement.
さらに他の測定方式では測定困難な腐食性流体、スラリ
、固形物などを含んだ混合流体の流量測定も可能である
といった利点を有し、各方面に多用されている。Furthermore, it has the advantage of being able to measure the flow rate of mixed fluids containing corrosive fluids, slurries, solids, etc. that are difficult to measure using other measurement methods, and is widely used in various fields.
ところで、この種の電磁流量計は、概略路354に示す
ような構成とされていた。これを簡単に説明すると、図
中符号lで示すものは、第4図(a)。By the way, this type of electromagnetic flowmeter had a configuration as shown schematically by a path 354. To briefly explain this, the symbol l in the figure is shown in FIG. 4(a).
から明らかなように、その両開口端外周にケース支持用
としての円環状フランジ板2,2を嵌装させた状態で溶
接して固着させてなる金属導管3による測定管lで、こ
の測定管1の外周部には、これを上、下方向から挟むよ
うにして、測定管l内の被測定流体の流れの方向と直交
する方向に磁界を与える略々鞍形状に巻回された一対の
励磁コイル4.4およびコア5,5等が配設されている
。As is clear from the figure, the measuring tube 1 is made up of a metal conduit 3 formed by welding and fixing annular flange plates 2, 2 for supporting the case fitted to the outer periphery of both open ends. A pair of excitation coils are wound around the outer periphery of the tube 1 in a substantially saddle shape to apply a magnetic field in a direction perpendicular to the flow direction of the fluid to be measured in the measurement tube 1, sandwiching the excitation coil from above and below. 4.4, cores 5, 5, etc. are arranged.
また、この測定管1の内壁面には、テフロン等の絶縁ラ
イニング(図示せず)が形成され、かつこれら測定管l
の外側には、前記フランジ板2.2の外周部に0リング
等を介して筒状のケース6が嵌装して固定されている。Further, an insulating lining (not shown) made of Teflon or the like is formed on the inner wall surface of the measuring tube 1, and
A cylindrical case 6 is fitted and fixed to the outer circumference of the flange plate 2.2 via an O-ring or the like.
さらに、上述した測定管lにおいて、被測定流体の流れ
の方向および前記励磁コイル4.4による磁界の方向の
それぞれと直交する方向には、周知のように、一対の電
極7(一方は図示せず)が対向して配設され、これによ
り導電性を有する被測定流体中で生じる起電力を取出す
ような構成とされている。なお、第4図(a)中8.9
は前記金属導管3の両開口端外周に切欠き形成された段
部3a、3aに対し円環状フランジ板2.2を嵌装させ
た状態でその内孔繰向、外を接合固定するようにして肉
盛りされた溶接部である。Furthermore, in the above-mentioned measurement tube l, a pair of electrodes 7 (one of which is not shown) is provided in a direction perpendicular to the flow direction of the fluid to be measured and the direction of the magnetic field generated by the excitation coil 4.4, as is well known. (2) are disposed facing each other, and are configured to extract the electromotive force generated in the conductive fluid to be measured. In addition, 8.9 in Figure 4(a)
In this case, the annular flange plate 2.2 is fitted to the stepped portions 3a, 3a formed on the outer periphery of both opening ends of the metal conduit 3, and the inner hole is bent and the outside is joined and fixed. This is a welded part that has been overlaid.
そして、このような構成による電磁流量計は、周知のよ
うに、被測定流体の左、右一対をなす配管to、10の
端部にそれぞれ形成されたフランジ部10a、10a同
士を、通しポル)11およびす“シト12等で締付は固
定することで、流体配管途中に介装されて配設固定され
、被測定流体の流量を測定するものである。As is well known, an electromagnetic flowmeter having such a configuration is capable of passing the fluid to be measured through the flanges 10a, 10a formed at the ends of the left and right piping 10, respectively. By tightening and fixing with screws 11 and 12, etc., it is inserted and fixed in the middle of a fluid piping, and the flow rate of the fluid to be measured is measured.
しかしながら、上述した構成による従来の電磁流量計に
おいて、金属導管3の両開口端に円環状フランジ板2を
溶接することで形成される測定管lでは、流体配管to
、toとの接合により、そのフランジ板2.2に対し
軸線方向外側からかなりの値の外力が加わり、さらに測
定管l内を流れる被測定流体からの内圧も加わるもので
あった。However, in the conventional electromagnetic flowmeter having the above-mentioned configuration, the measurement tube l formed by welding the annular flange plates 2 to both open ends of the metal conduit 3 does not allow the fluid piping to
, to, a considerable amount of external force was applied to the flange plate 2.2 from the outside in the axial direction, and internal pressure from the fluid to be measured flowing inside the measuring tube l was also applied.
そして、これらの外力による応力が金属導管3.フラン
ジ板2.および溶接部8.9等からなる測定管lの一部
に集中して加わり、その結果測定管lが局部的に疲労し
て塑性変形してしまい、測定精度の信頼性等の面で問題
となるもので、このような問題を解決し得る何らかの対
策を講じることが望まれている。The stress caused by these external forces is then applied to the metal conduit 3. Flange plate 2. It concentrates on a part of the measuring tube 1 consisting of welded parts 8, 9, etc., and as a result, the measuring tube 1 is locally fatigued and deformed plastically, which causes problems in terms of reliability of measurement accuracy, etc. Therefore, it is desired that some kind of countermeasure be taken to solve such problems.
このような要請に応えるために1本発明に係る電磁流量
計は、円環状フランジ板が金属導管の各開口端外周に嵌
装した状態で溶接して固着されてなる測定管において、
円環状フランジ板の内壁面と金属導管の外壁面とを、金
属導管外壁面から緩やかな勾配をもって立ち上がるよう
な肉盛りにより溶接するとともに、その立ち上がり部か
らフランジ板とは反対側の金属導管外壁面に、前記溶接
部の肉盛りと略々同一の勾配をもって連続するテーパ面
を有しかつ滑らかな曲面をもって折返す溝部を形成する
ようにしたものである。In order to meet such demands, an electromagnetic flowmeter according to the present invention is a measuring tube in which an annular flange plate is fitted to the outer periphery of each opening end of a metal conduit and is welded and fixed to the outer periphery of each opening end of the metal conduit.
The inner wall surface of the annular flange plate and the outer wall surface of the metal conduit are welded by a build-up that rises at a gentle slope from the outer wall surface of the metal conduit, and from the rising part, the outer wall surface of the metal conduit opposite to the flange plate is welded. Further, a groove portion is formed which has a continuous tapered surface with substantially the same slope as the build-up of the welded portion and is folded back with a smooth curved surface.
本発明によれば、金属導管外壁面でフランジ板との溶接
部の立ち上がり部よりも導管の軸線方向内側部分に形成
した溝部の存在によって、外力による応力集中を避け、
適切な応力分散が可能となるものである。According to the present invention, stress concentration due to external force is avoided by the presence of the groove formed on the outer wall surface of the metal conduit in the axially inner part of the conduit than the rising part of the welded part with the flange plate.
This enables appropriate stress distribution.
以下、本発明を図面に示した実施例を用いて詳細に説明
する。Hereinafter, the present invention will be explained in detail using embodiments shown in the drawings.
第1図および第2図は本発明に係る電磁流量計の一実施
例を示すものであり、これらの図において、前述した第
3図等と同一または相当する部分には、同一番号を付し
てその説明は省略する。Figures 1 and 2 show an embodiment of the electromagnetic flowmeter according to the present invention, and in these figures, parts that are the same as or correspond to those in Figure 3, etc. described above are designated by the same numbers. Therefore, the explanation will be omitted.
さて、本発明によれば、円環状フランジ板2゜2が金属
導管3の各開口端外周に嵌装した状態で溶接して固着さ
れてなる測定管lにおいて、フランジ板2.2の内壁面
と金属導管3の外壁面とを、金属導管3外壁面から緩や
かな勾配をもって立ち上がるような肉盛りにより溶接す
るとともに、その立ち上がり部Pからフランジ板2とは
反対側の金属導管3外壁面に、前記溶接部8の肉盛りと
略々同一の勾配をもって連続するテーパ面20aを有し
かつ滑らかな曲面20bをもって折返す溝部20を形成
したところに特徴を有している。Now, according to the present invention, in the measuring tube l in which the annular flange plate 2.2 is fitted onto the outer periphery of each open end of the metal conduit 3 and fixed by welding, the inner wall surface of the flange plate 2.2 and the outer wall surface of the metal conduit 3 are welded by a build-up that rises at a gentle slope from the outer wall surface of the metal conduit 3, and from the rising portion P to the outer wall surface of the metal conduit 3 on the opposite side from the flange plate 2, The groove 20 is characterized in that it has a continuous tapered surface 20a with substantially the same slope as the build-up of the welded portion 8, and is folded back with a smooth curved surface 20b.
このような構成を採用した理由は、次の通りである。す
なわち、上述した電磁流量計における測定管lにおいて
、その各部に対する外力による応力値は、従来、JIS
規格による圧力容器の構造等で、そのフランジ部分での
概略値のみを確認し得るだけであったが、本発明者らは
、近年注目されている有限要素法(FEM)を採用して
、上述した測定管l各部での応力値を計算して求めるこ
ととした。そして、これによる計算結果から、従来構造
での測定管lの金属導管3に対する軸線方向(z軸方向
)での応力は、第4図(a)、(b)に示すように、金
属導管3外壁面とフランジ板2内側面とを固着させる溶
接部8の肉盛りの立ち上がり部P位置で、急激な応力集
中(第5図中矢印参照)を生じていることが確認された
。この場合の最大応力値・σ zwaxを小さくするた
めには、溶接部8の軸線方向長さLおよびその肉盛り高
さt、さらには金属導管3の肉厚りを大きくすることが
必要で、いずれも材料コスト面から好ましくなく、シか
も測定管l全体の大型化等を招く等といった問題を生じ
てしまうものであった。なお、第5図中破線は、従来例
において集中応力が加わることによる変位状態を拡大し
て図示している。The reason for adopting such a configuration is as follows. That is, in the measuring tube l of the electromagnetic flowmeter mentioned above, the stress value due to external force on each part has conventionally been determined according to JIS
Due to the structure of the pressure vessel according to the standards, it was only possible to confirm the approximate value at the flange part, but the present inventors adopted the finite element method (FEM), which has been attracting attention in recent years, to calculate the above-mentioned value. The stress values at each part of the measuring tube 1 were calculated and determined. From the calculation results, the stress in the axial direction (z-axis direction) of the measuring tube l with respect to the metal conduit 3 in the conventional structure is as shown in FIGS. 4(a) and (b). It was confirmed that a sudden stress concentration (see the arrow in FIG. 5) occurred at the position P of the build-up of the weld portion 8 that fixed the outer wall surface and the inner surface of the flange plate 2. In order to reduce the maximum stress value σ zwax in this case, it is necessary to increase the axial length L of the welded portion 8 and its build-up height t, as well as the wall thickness of the metal conduit 3. All of these methods are unfavorable from the viewpoint of material cost, and may also lead to problems such as an increase in the size of the entire measuring tube. Note that the broken line in FIG. 5 shows an enlarged view of the displacement state caused by the application of concentrated stress in the conventional example.
したがって、本発明者らは、上述した有限要素法による
計算結果に基づいて種々検討、実験を行なった結果、溶
接部立ち上がり部Pを、第1図および第2図から明らか
なように、肉盛りされた溶接部8とその傾斜勾配に連続
して形成した溝部20のテーパ面20aとの間に位置さ
せることで、配管側からの荷重等といった外力による応
力集中を避は得るとともに、この溝部20の内面20a
、20bに沿って応力を効率よく分散させ、適切な応
力の分散分布(第2図中矢印で示す)が得られることを
確認した。勿論、このような応力分散によって、前述し
たような溶接部8の肉盛り寸法や導管3の厚み寸法等を
増大させることなく;最大応力値σ zmaxを小さく
することができ、また測定管l全体の小型かつ軽量化等
をも達成し得るものである。なお、上述した溶接部8の
肉盛り傾斜角度および溝部20のテーパ面20aの傾斜
角度θとしては、たとえばlO〜300(特に15゜付
近)とすればよいものである。Therefore, as a result of various studies and experiments based on the above-mentioned calculation results using the finite element method, the inventors of the present invention have determined that the rising part P of the weld is built up as shown in FIGS. 1 and 2. By positioning the welded portion 8 between the welded portion 8 and the tapered surface 20a of the groove portion 20 formed continuously on the slope thereof, stress concentration due to external forces such as loads from the piping side can be avoided, and this groove portion 20 inner surface 20a of
, 20b, and it was confirmed that an appropriate stress distribution distribution (indicated by arrows in FIG. 2) could be obtained. Of course, by such stress dispersion, the maximum stress value σ zmax can be reduced without increasing the build-up size of the welded part 8 or the thickness size of the conduit 3 as described above, and the overall measurement tube l It is also possible to achieve smaller size and lighter weight. The build-up inclination angle of the welded portion 8 and the inclination angle θ of the tapered surface 20a of the groove portion 20 may be, for example, 10 to 300 (particularly around 15°).
なお、本発明は上述した実施例構造に限定されず、各部
の形状、構造等を、適宜変形、変更することは自由であ
る。たとえば本発明を特徴づける溝部20は、金属導管
3の外壁面に予め成形加工してもよいし、また溶接後に
加工してもよいことは明らかであろう。Note that the present invention is not limited to the structure of the embodiment described above, and the shape, structure, etc. of each part may be modified and changed as appropriate. For example, it will be clear that the groove portion 20 that characterizes the present invention may be formed in advance on the outer wall surface of the metal conduit 3, or may be formed after welding.
以上説明したように1本発明に係る電磁流量計によれば
、測定管を構成する円環状フランジ板の内壁面と金属導
管の外壁面とを、金属導管外壁面から緩やかな勾配をも
って立ち上がるような肉盛りにより溶接するとともに、
その立ち上がり部からフランジ板とは反対側の金属導管
外壁面に、前記溶接部の肉盛りと略々同一の勾配をもっ
て連続するテーパ面を有しかつ滑らかな曲面をもって折
返す溝部を形成するようにしたので、簡単な構成にもか
かわらず、金属導管外壁面でフランジ板との溶接部の立
ち上がり部よりも導管の軸線方向内側に形成した溝部の
存在によって、外力による応力集中を避け、適切な応力
分散が可能で、これにより測定管の耐久性や測定精度の
信頼性等を向上させ得るとともに、測定管の小型かつ軽
量化を図り、コスト低減化を達成し樽る等といった種々
優れた効果がある。As explained above, according to the electromagnetic flowmeter according to the present invention, the inner wall surface of the annular flange plate constituting the measuring tube and the outer wall surface of the metal conduit are formed such that they rise with a gentle slope from the outer wall surface of the metal conduit. In addition to welding by overlaying,
A groove portion is formed on the outer wall surface of the metal conduit on the side opposite to the flange plate from the rising portion, the groove portion having a continuous tapered surface with substantially the same slope as the build-up of the welded portion and folded back with a smooth curved surface. Therefore, despite the simple configuration, the presence of a groove formed on the outer wall of the metal conduit on the inner side of the axial direction of the conduit than the rising part of the welded part with the flange plate avoids stress concentration due to external forces and maintains appropriate stress. Dispersion is possible, which not only improves the durability of the measuring tube and the reliability of measurement accuracy, but also allows the measuring tube to be made smaller and lighter, resulting in cost reduction and various excellent effects such as barreling. be.
第1図は本発明に係る電磁流量計の一実施例を示す測定
管の要部拡大断面図、第2図はその動作説明図、第3図
は電磁流量計の概略構成を示す要部断面図、第4図(a
)、(b)は従来例による問題点を説明するための側断
面図およびその軸線方向での応力特性図、第5図は有限
要素法により解析した測定管の変位状態を示す図である
。
111@−・測定管、2・拳・・円環状フランジ板、3
・・・・金属導管、6・・争・ケース。
8.9・・・・溶接部、10−・・・流体配管、10a
拳・拳・フランジ部、11φ拳・・通しボルト、20・
・・・溝部、20a・・Φ争テーパ面、20b−−・・
曲面、P−・拳φ溶接部立ち上がり部。Fig. 1 is an enlarged sectional view of the main part of a measuring tube showing one embodiment of the electromagnetic flowmeter according to the present invention, Fig. 2 is an explanatory diagram of its operation, and Fig. 3 is a sectional view of the main part showing the schematic configuration of the electromagnetic flowmeter. Figure 4 (a
) and (b) are a side sectional view and a stress characteristic diagram in the axial direction for explaining the problems with the conventional example, and FIG. 5 is a diagram showing the displacement state of the measuring tube analyzed by the finite element method. 111@-・Measuring tube, 2・Fist・annular flange plate, 3
...Metal conduit, 6.Dispute/case. 8.9...Welded part, 10-...Fluid piping, 10a
Fist, fist, flange, 11φ fist, through bolt, 20.
...Groove portion, 20a...Φ tapered surface, 20b---
Curved surface, rising part of P-/kistφ welding part.
Claims (1)
状態で溶接して固着されてなる測定管を備えた電磁流量
計において、前記円環状フランジ板の内壁面と金属導管
の外壁面とは、金属導管の外壁面から緩やかな勾配をも
って立ち上がるような肉盛りにより溶接されるとともに
、その立ち上がり部からフランジ板とは反対側の金属導
管外壁面には、前記溶接部の肉盛りと略々同一の勾配を
もって連続するテーパ面を有しかつ滑らかな曲面をもっ
て折返す溝部が形成されていることを特徴とする電磁流
量計。In an electromagnetic flowmeter equipped with a measurement tube in which an annular flange plate is fitted onto the outer periphery of each opening end of a metal conduit and then welded and fixed, the inner wall surface of the annular flange plate and the outer wall surface of the metal conduit is welded with a build-up that rises with a gentle slope from the outer wall surface of the metal conduit, and from the rising part on the outer wall surface of the metal conduit opposite to the flange plate, there is approximately the same build-up of the welded part. An electromagnetic flowmeter characterized in that a groove portion is formed that has a continuous tapered surface with the same slope and is folded back with a smooth curved surface.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12431785A JPS61283824A (en) | 1985-06-10 | 1985-06-10 | Electromagnetic flowmeter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12431785A JPS61283824A (en) | 1985-06-10 | 1985-06-10 | Electromagnetic flowmeter |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS61283824A true JPS61283824A (en) | 1986-12-13 |
JPH04535B2 JPH04535B2 (en) | 1992-01-07 |
Family
ID=14882336
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP12431785A Granted JPS61283824A (en) | 1985-06-10 | 1985-06-10 | Electromagnetic flowmeter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61283824A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE3915160A1 (en) * | 1988-05-19 | 1989-11-30 | Yamatake Honeywell Co Ltd | ELECTROMAGNETIC FLOW METER |
-
1985
- 1985-06-10 JP JP12431785A patent/JPS61283824A/en active Granted
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE3915160A1 (en) * | 1988-05-19 | 1989-11-30 | Yamatake Honeywell Co Ltd | ELECTROMAGNETIC FLOW METER |
Also Published As
Publication number | Publication date |
---|---|
JPH04535B2 (en) | 1992-01-07 |
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