JPH04535B2 - - Google Patents

Info

Publication number
JPH04535B2
JPH04535B2 JP12431785A JP12431785A JPH04535B2 JP H04535 B2 JPH04535 B2 JP H04535B2 JP 12431785 A JP12431785 A JP 12431785A JP 12431785 A JP12431785 A JP 12431785A JP H04535 B2 JPH04535 B2 JP H04535B2
Authority
JP
Japan
Prior art keywords
metal conduit
wall surface
welded
flange plate
electromagnetic flowmeter
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
Application number
JP12431785A
Other languages
Japanese (ja)
Other versions
JPS61283824A (en
Inventor
Masato Kuroda
Masaru Tsuge
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.)
Azbil Corp
Original Assignee
Azbil 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 Azbil Corp filed Critical Azbil Corp
Priority to JP12431785A priority Critical patent/JPS61283824A/en
Publication of JPS61283824A publication Critical patent/JPS61283824A/en
Publication of JPH04535B2 publication Critical patent/JPH04535B2/ja
Granted legal-status Critical Current

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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] [Field of Industrial Application] The present invention relates to an improvement in 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. .

〔従来の技術〕[Conventional technology]

一般に、電磁流量計は、フアラデーの電磁誘導
現像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、このような
電磁流量計は、測定にあたつて可動部分がなく、
また測定のために圧力損失を生じることがなく、
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
も可能であるといつた利点を有し、各方面に多用
されている。
In general, an electromagnetic flowmeter uses Faraday's electromagnetic induction development 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. This kind of electromagnetic flowmeter has no moving parts during measurement.
Also, there is no pressure loss due to measurement.
Furthermore, corrosive fluids that are difficult to measure using other measurement methods,
It has the advantage of being able to measure the flow rate of mixed fluids containing slurry, solids, etc., and is widely used in various fields.

ところで、この種の電磁流量計は、概略第3図
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1で示すものは、第4図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1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1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。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1の外側には、前記フランジ板2,2の
外周部にO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。さらに、上述した測定管
1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縁内、
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。
By the way, this type of electromagnetic flowmeter had a configuration as schematically shown in FIG. To briefly explain this, as is clear from Fig. 4a, the reference numeral 1 in the figure is in a state in which annular flange plates 2, 2 for supporting the case are fitted around the outer periphery of both opening ends. A measurement tube 1 is made of a metal conduit 3 which is welded and fixed in place.The outer circumference of the measurement tube 1 is sandwiched from above and below, and has a diameter that corresponds to the flow direction of the fluid to be measured in the measurement tube 1. A pair of excitation coils 4, 4 and cores 5, 5, etc., wound in a substantially saddle shape, which apply a magnetic field in orthogonal directions, are arranged. 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 an O-ring or the like is provided on the outer periphery of the flange plates 2, 2 on the outside of the measuring tube 1. A cylindrical case 6 is fitted and fixed therebetween. Furthermore, in the above-mentioned measurement tube 1, a pair of electrodes 7 are provided in the direction perpendicular to the flow direction of the fluid to be measured and the direction of the magnetic field generated by the excitation coils 4, 4, as is well known.
(one not shown) are disposed to face each other, and are configured to extract the electromotive force generated in the conductive fluid to be measured. Note that 8 and 9 in FIG. 4a indicate the inner holes of the metal conduit 3 with the annular flange plates 2 and 2 fitted to the stepped portions 3a and 3a formed on the outer periphery of both open ends of the metal conduit 3. Inner side,
This is a welded part that is built up so that the outside is joined and fixed.

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10,10の端部にそれぞれ形成されたフラン
ジ部10a,10a同士を、通しボルト11およ
びナツト12等で締付け固定することで、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。
An electromagnetic flowmeter with such a configuration is
As is well known, by tightening and fixing the flanges 10a, 10a formed at the ends of the left and right piping 10, 10, respectively, with through bolts 11 and nuts 12, the fluid can be measured. It is installed and fixed in the middle of piping and measures the flow rate of the fluid to be measured.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

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
1では、流体配管10,10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1内を流れ
る被測定流体からの内圧も加わるものであつた。
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1の一部に集中して加わり、その結果測定管
1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。
However, in the conventional electromagnetic flowmeter having the above-mentioned configuration, the measuring tube 1 is formed by welding the annular flange plate 2 to both open ends of the metal conduit 3. A considerable amount of external force was applied to the flange plates 2, 2 from the outside in the axial direction, and internal pressure from the fluid to be measured flowing inside the measuring tube 1 was also applied.
The stress caused by these external forces is then applied to the metal conduit 3,
The force is concentrated on a part of the measuring tube 1 consisting of the flange plate 2 and the welded parts 8, 9, etc., and as a result, the measuring tube 1 is locally fatigued and deformed plastically, which deteriorates the reliability of measurement accuracy, etc. It is desired that some kind of countermeasure be taken to solve this problem.

〔問題点を解決するための手段〕[Means for solving problems]

このような要請に応えるために、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
やかな勾配をもつ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つて連続するテ
ーパ面を有しかつ滑らかな曲面をもつて折返す溝
部を形成するようにしたものである。
In order to meet such demands, the electromagnetic flowmeter according to the present invention has a measuring tube in which an annular flange plate is fitted onto the outer periphery of each opening end of a metal conduit and is fixed by welding. The inner wall surface of the 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 to the outer wall surface of the metal conduit opposite to the flange plate. , 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.

〔作用〕[Effect]

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つて、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, due to 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, stress concentration due to external force is avoided and appropriate stress distribution is achieved. It is possible.

〔実施例〕〔Example〕

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1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つて
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つて連続するテーパ面2
0aを有しかつ滑らかな曲面20bをもつて折返
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, the annular flange plate 2,
In the measuring tube 1, the inner wall surfaces of the flange plates 2, 2 and the outer wall surface of the metal conduit 3 are connected to the outside of the metal conduit 3. Welding is performed by a build-up that rises from the wall surface with a gentle slope, and from the rising part P, a weld that is approximately the same as the build-up of the welding part 8 is applied to the outer wall surface of the metal conduit 3 on the opposite side from the flange plate 2. Continuous tapered surface 2 with a slope
It is characterized by forming a groove portion 20 which has a curved surface 20a 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1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
るだけであつたが、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1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1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σzmax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h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、し
かも測定管1全体の大型化等を招く等といつた問
題を生じてしまうものであつた。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
よる変位状態を図示している。
The reason for adopting such a configuration is as follows. In other words, in the measurement tube 1 of the electromagnetic flowmeter described above, the stress value due to external force on each part could conventionally be confirmed only as an approximate value at the flange part due to the structure of the pressure vessel according to the JIS standard. However, the present inventors adopted the finite element method (FEM), which has been attracting attention in recent years, to calculate and obtain the stress values at each part of the measurement tube 1 described above. From the calculation results, the stress in the axial direction (z-axis direction) of the measuring tube 1 with respect to the metal conduit 3 in the conventional structure is determined by the stress on the outer wall surface of the metal conduit 3 and the flange, as shown in Fig. 4a and b. Rising part P of the build-up of the welding part 8 that fixes the inner surface of the plate 2
It was confirmed that a sudden stress concentration (see arrow in FIG. 5) occurred at the position. In order to reduce the maximum stress value σzmax in this case, it is necessary to increase the axial length L of the welded part 8 and its build-up height t, as well as the wall thickness h of the metal conduit 3. This is not preferable in terms of material cost, and also causes problems such as increasing the size of the measuring tube 1 as a whole. In addition, the broken line in FIG. 5 illustrates the displacement state due to the application of concentrated stress in the conventional example.

したがつて、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
なつた結果、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2
0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つた外力による応力集中
を避け得るとともに、この溝部20の内面20
a,20bに沿つ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
散によつて、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σzmaxを小さくすることができ、ま
た測定管1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10〜30゜(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 have determined that the welding part rising part P is as shown in FIGS. 1 and 2. , a welded part 8 with built-up overlay and a groove part 2 formed continuously on the slope of the welded part 8
By positioning it between the tapered surface 20a of 0,
In addition to avoiding stress concentration due to external forces such as loads from the piping side, the inner surface 20 of this groove 20
It was confirmed that stress could be efficiently dispersed along lines a and 20b and that an appropriate stress distribution (indicated by arrows in FIG. 2) could be obtained. Of course, due to such stress dispersion, the overlay dimension of the welded part 8 and the thickness dimension of the conduit 3 as described above are not increased.
The maximum stress value σzmax can be reduced, and the measurement tube 1 as a whole can be made smaller and lighter. Note that 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 are, for example, 10 to 30° (especially around 15°).
It is sufficient to do so.

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 or 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.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、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つ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つて連続
するテーパ面を有しかつ滑らかな曲面をもつて折
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つて、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得る等といつた種々優
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 rise up with a gentle slope from the outer wall surface of the metal conduit. In addition to welding with a build-up of this kind, the outer wall surface of the metal conduit opposite to the flange plate from the rising part has a continuous tapered surface with approximately the same slope as the build-up of the welding part and is smooth. Despite the simple structure, the groove formed on the outer wall of the metal conduit on the inner side in the axial direction of the conduit than the rising part of the welded part with the flange plate is formed. Due to its presence, it is possible to avoid stress concentration due to external forces and to distribute stress appropriately, thereby improving the durability of the measuring tube and the reliability of measurement accuracy, as well as making the measuring tube smaller and lighter. There are various excellent effects such as cost reduction.

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

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。 1……測定管、2……円環状フランジ板、3…
…金属導管、6……ケース、8,9……溶接部、
10……流体配管、10a……フランジ部、11
……通しボルト、20……溝部、20a……テー
パ面、20b……曲面、P……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. Figures 4a and 4b are side sectional views and stress characteristic diagrams in the axial direction for explaining problems with the conventional example, and Figure 5 is a diagram showing the displacement state of the measuring tube analyzed by the finite element method. It is. 1... Measuring tube, 2... Annular flange plate, 3...
...Metal conduit, 6...Case, 8, 9...Welded part,
10...Fluid piping, 10a...Flange part, 11
...Through bolt, 20...Groove portion, 20a...Tapered surface, 20b...Curved surface, P...Welding portion rising portion.

Claims (1)

【特許請求の範囲】[Claims] 1 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
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つて立ち上がるよ
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
をもつて連続するテーパ面を有しかつ滑らかな曲
面をもつ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。
1. 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 by a build-up that rises at a gentle slope from the outer wall surface of the metal conduit, and the build-up of the welded part is welded from the rising part to the outer wall surface of the metal conduit on the opposite side from the flange plate. 1. An electromagnetic flowmeter characterized in that a groove portion is formed which has a continuous tapered surface with substantially the same slope as the curved surface and is folded back with a smooth curved surface.
JP12431785A 1985-06-10 1985-06-10 Electromagnetic flowmeter Granted JPS61283824A (en)

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 JPS61283824A (en) 1986-12-13
JPH04535B2 true 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)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0625681B2 (en) * 1988-05-19 1994-04-06 山武ハネウエル株式会社 Electromagnetic flow meter

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Publication number Publication date
JPS61283824A (en) 1986-12-13

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