JPS5975118A - Electromagnetic flowmeter - Google Patents

Electromagnetic flowmeter

Info

Publication number
JPS5975118A
JPS5975118A JP18449082A JP18449082A JPS5975118A JP S5975118 A JPS5975118 A JP S5975118A JP 18449082 A JP18449082 A JP 18449082A JP 18449082 A JP18449082 A JP 18449082A JP S5975118 A JPS5975118 A JP S5975118A
Authority
JP
Japan
Prior art keywords
ceramic
measuring electrode
electrode
tube
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.)
Pending
Application number
JP18449082A
Other languages
Japanese (ja)
Inventor
Katsumi Fujikawa
冨士川 克美
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.)
Yokogawa Electric Corp
Original Assignee
Yokogawa Hokushin Electric 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 Yokogawa Hokushin Electric Corp filed Critical Yokogawa Hokushin Electric Corp
Priority to JP18449082A priority Critical patent/JPS5975118A/en
Publication of JPS5975118A publication Critical patent/JPS5975118A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/56Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects
    • G01F1/58Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects by electromagnetic flowmeters
    • G01F1/584Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects by electromagnetic flowmeters constructions of electrodes, accessories therefor

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Volume Flow (AREA)

Abstract

PURPOSE:To make an exchange of a measuring electrode easy and to measure the flow rate of a high temp. and high pressure fluid by forming the measuring electrode of a liningless electromagnetic flowmeter in one body with ceramic and by providing the measuring electrode to a pipe body by a screw means. CONSTITUTION:The measuring electrode 3 is formed in one body with the ceramic covering the circumference. The electrode 3 is made to one body with a metal bush 8 fitted with screw to the pipe body 2 through the ceramic 7. Otherwise, the electrode 3 is pressed by a pressing screw 10 through the ceramic 7. Thereby, the electrode 3 can be removed and exchanged easily.

Description

【発明の詳細な説明】 本発明は電磁流量計に係り、特にライニングを持たない
電磁流量計(ライニングレス電磁流量計)の電極部を改
良[またものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electromagnetic flowmeter, and particularly to an improvement in the electrode portion of an electromagnetic flowmeter without a lining (a liningless electromagnetic flowmeter).

最近導管内面を絶縁性とするためのライニングを必要と
しない電磁流量計が発表されている。
Recently, an electromagnetic flowmeter has been announced that does not require a lining to insulate the inner surface of the conduit.

本発明の説明に先立ちこの従来例を以下に説明する。Prior to explaining the present invention, this conventional example will be explained below.

第1図において流量を測定する被測定流体1が流通する
非磁性で導電性の管体2には、磁界Bと直交する位置に
測定電極3,3aが設けられている。さらに測定電極3
.3af、囲んでリング状の給電端子4,4aが設けら
れている。
In FIG. 1, a non-magnetic and electrically conductive tube body 2 through which a fluid to be measured 1 whose flow rate is to be measured flows is provided with measurement electrodes 3, 3a at positions orthogonal to a magnetic field B. As shown in FIG. Furthermore, measurement electrode 3
.. 3af, ring-shaped power supply terminals 4 and 4a are provided surrounding it.

測定電極3,3aはエポキシ樹脂等の絶縁材6を介して
管体2に装着されている。帰還により利得が1にされた
増幅器5,5aは夫々測定電極3,3aにより検出され
た誘導電圧を給電端子4,4aに与えている。このため
給電端子4゜4aはそれぞれ測定電極3,3aと等電位
となり、かつ4,4a間には大きな電流が流れ、管体2
には電位降下が発生する。管体2の肉厚が均一なら給電
端子4,4a間の電位分布は管内周の長さにつき直線的
となる。流体1の管内壁附近の誘導電圧の分布は、磁界
Bが場所に拘らず均一でありかつ流れが管ビ1断面につ
き一様流である時には内周長さにつき正弦状となること
が知られている。従って給電端子4,4aの位置を適当
に選べば管体2の内周上のすべての点で管壁上の電位分
布と被測定流体1中の誘導電圧の分布とを近似的に尋し
くすることが出来る。
The measurement electrodes 3, 3a are attached to the tube body 2 via an insulating material 6 such as epoxy resin. Amplifiers 5 and 5a whose gains are set to 1 by feedback supply the induced voltages detected by measurement electrodes 3 and 3a to power supply terminals 4 and 4a, respectively. Therefore, the power supply terminals 4° 4a have the same potential as the measurement electrodes 3 and 3a, and a large current flows between them, causing the tube body 2
A potential drop occurs. If the wall thickness of the tube body 2 is uniform, the potential distribution between the power supply terminals 4 and 4a will be linear with respect to the length of the tube's inner circumference. It is known that the distribution of the induced voltage near the inner wall of the pipe of the fluid 1 is sinusoidal over the inner circumference when the magnetic field B is uniform regardless of the location and the flow is uniform across the cross section of the pipe 1. ing. Therefore, if the positions of the power supply terminals 4 and 4a are appropriately selected, the potential distribution on the tube wall and the distribution of induced voltage in the fluid to be measured 1 can be approximated at all points on the inner circumference of the tube body 2. I can do it.

よって管体2の内壁が導電性であっても管体2と被測定
流体1との間の電流の出入がないので測定電極3,3a
により取出し増幅器5,5aを経て端子6,6aより得
られる電圧は通常のライニングを有する場合と同じ誘導
電圧となるこのように管内壁に絶縁性を与えるためのラ
イニングが不要になれば、ライニングの変形、破損等の
トラブルが防止出来て電磁流量計の信頼性を高めること
が可能となる。更に、熱に弱−ライニングが不要である
ため、高温流体の測定が可能になるという期待が寄せら
れていた。
Therefore, even if the inner wall of the tube body 2 is conductive, there is no current flowing between the tube body 2 and the fluid to be measured 1, so the measurement electrodes 3, 3a
Therefore, the voltage obtained from the terminals 6, 6a via the take-out amplifiers 5, 5a is the same induced voltage as in the case with a normal lining.If the lining to provide insulation to the inner wall of the pipe is no longer necessary, the lining Troubles such as deformation and damage can be prevented and the reliability of the electromagnetic flowmeter can be improved. Furthermore, since a thermally sensitive lining is not required, there have been expectations that high temperature fluids can be measured.

ところで第1図に示す従来技術では、エポキシ樹脂等の
高分子材料からなる絶縁材6を用いているため、現実に
は高温流体を測定することはできなかった。これは高分
子材料の耐熱温度が低い(例えばエポキシ樹脂では80
℃)ためである。このためライニングを不要としたライ
ニングレス電磁流量計が開発されたにもがかわらず、絶
縁材6がネックとなって高温流体の測定ができず、ライ
ニングレス電磁流量計の長所が十分には引き出されてい
なかった。更に、測定電極3,3aは絶縁材6に固着さ
れているため、測定電極3,3aの接液面が汚れてもこ
の測定電極3,3aを交換できなかった。したがって接
液面の汚れに起因して、正確な流量測定が妨げられるこ
ともあった。
However, in the conventional technique shown in FIG. 1, since the insulating material 6 made of a polymeric material such as epoxy resin is used, it is not possible to actually measure high-temperature fluids. This is due to the low heat resistance temperature of polymer materials (e.g. 80% for epoxy resins).
℃). For this reason, although a liningless electromagnetic flowmeter that did not require a lining was developed, the insulating material 6 became a bottleneck that made it impossible to measure high-temperature fluids, and the advantages of the liningless electromagnetic flowmeter could not be fully exploited. It wasn't. Furthermore, since the measuring electrodes 3, 3a are fixed to the insulating material 6, even if the liquid contact surfaces of the measuring electrodes 3, 3a become dirty, the measuring electrodes 3, 3a cannot be replaced. Therefore, accurate flow rate measurement may be hindered due to contamination of the liquid contact surface.

本発明は、上記従来技術に鑑み、高温流体を測定できる
とともに測定電極を交換できる電磁流量計を提供するこ
とを目的とする。かかる目的を達成する本発明は、ライ
ニングレス電磁流量計の測定電極をセラミックと一体に
形成し、この測定電極を螺合手段により管体に備えた点
をその技術思想の基礎とするものである。
SUMMARY OF THE INVENTION In view of the above-mentioned prior art, an object of the present invention is to provide an electromagnetic flowmeter that can measure high-temperature fluids and replace measuring electrodes. The technical idea of the present invention, which achieves this object, is that the measurement electrode of a liningless electromagnetic flowmeter is formed integrally with ceramic, and the measurement electrode is attached to the pipe body by screwing means. .

以下本発明の実施例を図面に基づき詳細に説明する。な
お、従来技術と同一部分には同一番号を付し重複する説
明は省略する。
Embodiments of the present invention will be described in detail below based on the drawings. Note that parts that are the same as those in the prior art are given the same numbers and redundant explanations will be omitted.

第2図は本発明の第1の実施例を示す。図中、3は測定
電極、7はセラミック、8Fi金属ブツシユであり、こ
れら三者は一体に焼成されている。金属ブツシュ8は管
体2に螺合されているため、金属ブツシュ8と一体とな
った測定室1極3は容易に取り外し・交換ができる。金
属ブツシュ8と管体2との間には圧力変形し難い金属性
中空Oリング9が介装されている。しかも、測定電極3
及びセラミック7は、管体2の径方向に亘り1会が漸増
するテーパ状の鍔部を有しているため、外周側に抜は出
ることはない。このため、鍔部と中空Oリング9との効
果が共働することにより、1000 krf /ca程
度の高圧流体を測定することができる。更に測定電極3
を絶縁するセラミック7は熱に強いので、500℃程度
の高温流体の測定が可能となる。もちろん本実施例では
、ライニングを有しないため、第1図に示した実施例と
同じように管体1に電流を供給する給電手段等(図示省
略)が備えられており、このために被測定流体中には大
きな誘導起電力が生起される。なお、次に述べる第2、
第3の実施例においても、図示けしないが、給電手段等
を備えてしる。
FIG. 2 shows a first embodiment of the invention. In the figure, 3 is a measurement electrode, 7 is a ceramic, and an 8Fi metal bushing, and these three are fired as one unit. Since the metal bushing 8 is screwed onto the tube body 2, the measuring chamber 1 pole 3 integrated with the metal bushing 8 can be easily removed and replaced. A hollow metallic O-ring 9, which is not easily deformed by pressure, is interposed between the metal bush 8 and the tube body 2. Moreover, the measurement electrode 3
Since the ceramic 7 has a tapered flange whose width gradually increases in the radial direction of the tubular body 2, the flange does not protrude toward the outer circumference. Therefore, the effects of the collar and the hollow O-ring 9 work together, making it possible to measure high-pressure fluid of about 1000 krf/ca. Furthermore, measurement electrode 3
Since the ceramic 7 that insulates the sensor is resistant to heat, it is possible to measure fluids at a high temperature of about 500°C. Of course, since this embodiment does not have a lining, it is equipped with a power supply means (not shown) for supplying current to the tube body 1, as in the embodiment shown in FIG. A large induced electromotive force is generated in the fluid. In addition, the second
Although not shown in the drawings, the third embodiment also includes a power supply means and the like.

第3図は本発明の第2の実施例を示しており、この実施
例では測定電極3が被測定流体1に接触しない容量検出
型電極となっている。なお、他の部分の構成・作用は第
2図に示す実施例と同一である。
FIG. 3 shows a second embodiment of the present invention, in which the measurement electrode 3 is a capacitance detection type electrode that does not come into contact with the fluid 1 to be measured. Note that the configuration and operation of other parts are the same as the embodiment shown in FIG.

第4図は本発明の第3の実施例を示している。FIG. 4 shows a third embodiment of the invention.

本実施例では測定電極3はセラミック7と一体に焼成さ
れている。押(−ねじ1oは、管体2に螺合されて前記
セラミック7を図中下方に押圧することにより、セラミ
ック7と一体の測定電極3を管体2に装着している。こ
の実施例においても、測定電極3の交換が容易であり、
また高温・高圧流体の測定も可能である。
In this embodiment, the measuring electrode 3 is fired integrally with the ceramic 7. A push screw 1o is screwed into the tube body 2 and presses the ceramic 7 downward in the figure, thereby attaching the measurement electrode 3 integrated with the ceramic 7 to the tube body 2. Also, the measurement electrode 3 is easy to replace,
It is also possible to measure high temperature and high pressure fluids.

以上実施例とともに具体的に説明したように本発明によ
れば、測定電極の取換が容易であるとともに、高温・高
圧流体の測定が可能な電磁流量計を提供することができ
る。
As specifically explained above in conjunction with the embodiments, according to the present invention, it is possible to provide an electromagnetic flowmeter that allows easy replacement of measurement electrodes and is capable of measuring high-temperature and high-pressure fluids.

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

第1図は従来のライニングレス電磁流量計を示す断面図
、第2図〜第4図は本発明の名種実施例を示す断面図で
ある。 図面中 1は被測定流体、 2は管体、 3.3aは測定電極、 7はセラミック、 8は金属ブツシュ、 9は金属性中空Oリング、 10け押しねじ である。 特許出願人 株式会社 北辰電機製作所 代理人 弁理士  光 石 士 部(他1名)
FIG. 1 is a sectional view showing a conventional liningless electromagnetic flowmeter, and FIGS. 2 to 4 are sectional views showing exemplary embodiments of the present invention. In the drawings, 1 is a fluid to be measured, 2 is a tube body, 3.3a is a measurement electrode, 7 is a ceramic, 8 is a metal bushing, 9 is a hollow metal O-ring, and 10 is a set screw. Patent applicant Hokushin Electric Manufacturing Co., Ltd. Patent attorney Shibu Mitsuishi (and 1 other person)

Claims (2)

【特許請求の範囲】[Claims] (1)被測定流体を流すための導電性の管体と、この管
体に磁界を印加するための磁界発生手段と、前記被測定
流体中に発生する誘導起電力を取り出すために前記管体
に絶縁されて備えられた測定電極と、少くとも前記測定
電極付近において前記誘導起電力とほぼ等しい電位分布
を前記管体に形成する給電手段とを具備する電磁流量計
において、前記測定電極はその周囲を覆うセラミックと
一体に形成されており、しかも測定電極は前記管体に螺
合された螺合手段とセラミックを介して一体となるか若
しくはセラミックを介して前記螺合手段で押圧されるこ
とにより前記管体に備えられていることを特徴とする電
磁流量針。
(1) A conductive tube for flowing the fluid to be measured, a magnetic field generating means for applying a magnetic field to the tube, and the tube for extracting the induced electromotive force generated in the fluid to be measured. In an electromagnetic flowmeter, the electromagnetic flowmeter is equipped with a measuring electrode that is insulated and provided, and a power supply means that forms a potential distribution in the pipe body that is approximately equal to the induced electromotive force at least near the measuring electrode, the measuring electrode is The measuring electrode is formed integrally with the surrounding ceramic, and the measuring electrode is either integrated with the screwing means screwed onto the tube through the ceramic, or is pressed by the screwing means through the ceramic. An electromagnetic flow needle, characterized in that the tube body is provided with an electromagnetic flow needle.
(2)前記測定電極及びセラミックの少くとも一方は、
管体の径方向に亘り内周側の部分の径が外周側の部分の
径よりも大きい鍔部を有することを特徴とする特許請求
の範囲第1項記載の電磁流量計。
(2) At least one of the measurement electrode and the ceramic,
The electromagnetic flowmeter according to claim 1, characterized in that the tube body has a flange portion in which the diameter of the inner circumference side portion is larger than the diameter of the outer circumference side portion in the radial direction of the pipe body.
JP18449082A 1982-10-22 1982-10-22 Electromagnetic flowmeter Pending JPS5975118A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18449082A JPS5975118A (en) 1982-10-22 1982-10-22 Electromagnetic flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18449082A JPS5975118A (en) 1982-10-22 1982-10-22 Electromagnetic flowmeter

Publications (1)

Publication Number Publication Date
JPS5975118A true JPS5975118A (en) 1984-04-27

Family

ID=16154084

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18449082A Pending JPS5975118A (en) 1982-10-22 1982-10-22 Electromagnetic flowmeter

Country Status (1)

Country Link
JP (1) JPS5975118A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3908698A1 (en) * 1988-03-17 1989-09-28 Yamatake Honeywell Co Ltd ELECTRODE STRUCTURE FOR ELECTROMAGNETIC FLOW METERS

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3908698A1 (en) * 1988-03-17 1989-09-28 Yamatake Honeywell Co Ltd ELECTRODE STRUCTURE FOR ELECTROMAGNETIC FLOW METERS

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