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JPH0530203B2 - - Google Patents
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JPH0530203B2 - - Google Patents

Info

Publication number
JPH0530203B2
JPH0530203B2 JP59035413A JP3541384A JPH0530203B2 JP H0530203 B2 JPH0530203 B2 JP H0530203B2 JP 59035413 A JP59035413 A JP 59035413A JP 3541384 A JP3541384 A JP 3541384A JP H0530203 B2 JPH0530203 B2 JP H0530203B2
Authority
JP
Japan
Prior art keywords
magnetic
electromagnetic
current meter
main body
pair
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 - Lifetime
Application number
JP59035413A
Other languages
Japanese (ja)
Other versions
JPS60179613A (en
Inventor
Masaaki Shinjo
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.)
TOHO KEISOKU KENKYUSHO KK
Original Assignee
TOHO KEISOKU KENKYUSHO KK
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 TOHO KEISOKU KENKYUSHO KK filed Critical TOHO KEISOKU KENKYUSHO KK
Priority to JP3541384A priority Critical patent/JPS60179613A/en
Publication of JPS60179613A publication Critical patent/JPS60179613A/en
Publication of JPH0530203B2 publication Critical patent/JPH0530203B2/ja
Granted 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

Landscapes

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

Description

【発明の詳細な説明】 本発明は、電磁式流速測定装置に関するもので
あつて、管路内の流体の流速を長期にわたつて安
定して計測できるようにすることを目的とする。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electromagnetic flow rate measuring device, and an object thereof is to be able to stably measure the flow rate of a fluid in a pipe line over a long period of time.

上下水道等の管路内の流体流量を計測する手段
として、羽根車式流量計、差圧式流量計、渦流流
量計、電磁式流量計等が開発されており、特に羽
根車式流量計が一般的であるが、可動部分を有す
る機械的な構成であるが故に、摩耗損失等の故障
が絶えず、低流速では作動が不確実であり、更に
は既設管への取付工事に手間のかかる欠点が存し
ている。
Impeller type flowmeters, differential pressure type flowmeters, vortex flowmeters, electromagnetic type flowmeters, etc. have been developed as means for measuring fluid flow rates in water and sewerage pipes, etc., and impeller type flowmeters are particularly popular. However, because it has a mechanical structure with moving parts, it suffers from frequent failures such as wear and loss, is unstable in operation at low flow speeds, and has the disadvantages that installation work to existing pipes is time-consuming. Exists.

そこで精度的に優れた電磁流量計が所期の効果
を得る流量計として用いられている。
Therefore, electromagnetic flowmeters with excellent accuracy are used as flowmeters that achieve the desired effect.

周知のように電磁流量計は、電気伝導性流体が
流れる管路に垂直に磁場を作用させ、磁場の方向
と流体の流れの方向とに垂直な方向の管壁に向か
い合つた電極を設け、電磁誘導で電極間に生じる
電圧を測定して流量を求める構成である。
As is well known, an electromagnetic flowmeter applies a magnetic field perpendicularly to a pipe through which an electrically conductive fluid flows, and provides electrodes facing the pipe wall in a direction perpendicular to the direction of the magnetic field and the direction of fluid flow. The configuration is such that the flow rate is determined by measuring the voltage generated between the electrodes due to electromagnetic induction.

しかしながらこの種の流量計は、管路内の流量
を測定する場合、管の外部に装着するものである
為に、構造的に大規模となり、電磁石の場合には
形状が特殊であるので成形にコストが嵩む等の不
満点が存した。
However, when measuring the flow rate in a pipe, this type of flowmeter is attached to the outside of the pipe, so it is structurally large, and in the case of an electromagnet, it has a special shape, so it cannot be molded. There were some dissatisfied points such as increased cost.

また少なくとも計測箇所の管は非磁性材製でな
ければ正確な測定は得られないので、既設管に装
着する場合には、管の部分的な交換を必要とし、
作業性に劣る欠点も存する。
In addition, accurate measurements cannot be obtained unless the pipe at the measurement point is made of non-magnetic material, so if it is installed on an existing pipe, it will be necessary to partially replace the pipe.
It also has the disadvantage of poor workability.

即ち従来の電磁式流量計にあつては、流体管路
に対する設置に際し、管路の口径に対応して相応
の大きさを有する機種を選定しなければならない
為に、多くの機種を用意しなければならず、必然
的に大口径の管路に対しては大きさ、重量、コス
トが嵩み、設置作業に機械を導入しなければなら
ないので取扱いが困難であつて作業性の低下を招
き、大規模な装置であれば、消費電力も多くなつ
て非経済的である。
In other words, when conventional electromagnetic flowmeters are installed in a fluid pipeline, it is necessary to select a model with an appropriate size according to the diameter of the pipeline, so many models must be prepared. Inevitably, large-diameter pipes require increased size, weight, and cost, and require the introduction of machinery for installation work, which makes handling difficult and reduces work efficiency. If the device is large-scale, it will consume a lot of power, making it uneconomical.

また羽根車式、電磁式を含め、既設管へのその
設置時には一度断水して管を切断する必要があ
り、保守点検等の際にも、断水して、或いは予め
設けたバイパス管を使用しなければならず、工事
自体が大がかりにならざるを得ない。そして電磁
式流量計の最も確実な校正手段は実流量校正であ
るが、この実流量校正装置に設置する場合にも、
使用せんとする管径に対応した規模の流量計を用
意しなければならず、更には従来の流量計の流速
感度は0.3m/sec程度以上であつて、この数値以
下の低流速に対する精度が得られない憾があつ
た。
In addition, when installing any type of equipment, including impeller type and electromagnetic type, into existing pipes, it is necessary to cut off the water supply and cut the pipe, and during maintenance inspections, etc., it is necessary to cut off the water supply or use a pre-installed bypass pipe. Therefore, the construction itself would have to be large-scale. The most reliable means of calibrating an electromagnetic flowmeter is actual flow rate calibration, but even when installed in this actual flow rate calibration device,
It is necessary to prepare a flowmeter of a scale corresponding to the pipe diameter to be used, and furthermore, the flow velocity sensitivity of conventional flowmeters is about 0.3 m/sec or more, and the accuracy for low flow velocity below this value is poor. I regret not being able to get it.

つまり従来の流量計では、作業性、経済性、精
度に於て、あらゆる点で欠点、不都合が存してい
たのである。
In other words, conventional flowmeters had drawbacks and inconveniences in all respects in terms of workability, economy, and accuracy.

本発明は上述した従来の欠点、不都合に鑑みて
開発された電磁式流速測定装置に関するものであ
つて、既設管に簡単に装着でき、しかも高い精度
が得られるように構成したものである。
The present invention relates to an electromagnetic flow rate measuring device developed in view of the above-mentioned conventional drawbacks and inconveniences, and is configured so that it can be easily installed in existing pipes and can provide high accuracy.

以下本発明の一実施例を図面に従つて説明す
る。
An embodiment of the present invention will be described below with reference to the drawings.

先ず図中符号1は流速計本体である。 First, reference numeral 1 in the figure is the main body of the current meter.

この流速計本体1は、電磁コイル2が巻回され
たコア3と電極5とを樹脂モールド7により一体
化した流線形状であり、両側中央には前後方向に
沿つてガイド溝8が形成されており、上端中央に
保持杆9が一体突設されている。
The current meter main body 1 has a streamlined shape in which a core 3 around which an electromagnetic coil 2 is wound and an electrode 5 are integrated by a resin mold 7, and a guide groove 8 is formed in the center of both sides along the front-rear direction. A holding rod 9 is integrally protruded from the center of the upper end.

そして本体1内にあつて、保持杆9と同一方向
である上下方向に垂直姿勢となつたコア3の上下
両端の両磁極には、ヨーク4が一体設される。
Inside the main body 1, a yoke 4 is integrally provided with both magnetic poles at both upper and lower ends of the core 3, which is vertically aligned in the same direction as the holding rod 9.

上端のヨーク4aは両側下方に延出位置し、下
端のヨーク4bは両側上方に延出位置しており、
上端のヨーク4a先端と下端のヨーク4b先端と
は、前記ガイド溝8の幅とほぼ同一長さ間隔をも
つて近接して対向し、従つて本体1の両側にあつ
て、ガイド溝8の幅方向に沿つて垂直に一対の磁
路Aが形成されることになる。
The yoke 4a at the upper end extends downward on both sides, and the yoke 4b at the lower end extends upward on both sides.
The tip of the yoke 4a at the upper end and the tip of the yoke 4b at the lower end are close to each other and face each other with a length interval that is approximately the same as the width of the guide groove 8. A pair of magnetic paths A are formed perpendicularly along the direction.

また二つの電極5は、前記両磁路A間に夫々位
置し、一部が外方に露出する形態でガイド溝8中
央に設けられており、更に本体1前端にはニユー
トラル電極6が露出位置している。
The two electrodes 5 are located between the two magnetic paths A, and are provided in the center of the guide groove 8 with a portion exposed to the outside, and a neutral electrode 6 is located at the exposed position at the front end of the main body 1. are doing.

尚、電磁コイル2、電極5,6のリード線は保
持杆9内を通つて外部に導出される。
Incidentally, the lead wires of the electromagnetic coil 2 and the electrodes 5 and 6 are led out through the holding rod 9.

上述した流速計本体1は上水道等の管路10内
に設置固定されるが、その姿勢は、前端を流体の
上流方向に向け流路に沿つた状態である。
The above-described current meter main body 1 is installed and fixed in a pipe line 10 of a water supply or the like, and its posture is along the flow path with the front end facing upstream of the fluid.

さて上述した測定装置にあつて、電磁コイル2
を商用電源、バツテリー、乾電池等を用いて低周
波矩形波方式により励磁し、本体1の両側に於け
るヨーク4間に夫々磁路Aを形成する。
Now, in the above-mentioned measuring device, the electromagnetic coil 2
is excited by a low frequency rectangular wave method using a commercial power source, battery, dry cell, etc., and magnetic paths A are formed between the yokes 4 on both sides of the main body 1, respectively.

そして本体1両側のガイド溝8前端から後端方
向に流れる導電性流体が上記磁路Aに直交して通
過する際に生ずる誘起電圧を両電極5によつて検
知し、流体の流速を測定することによつて、流量
を測定するのである。
Then, the induced voltage generated when the conductive fluid flowing from the front end to the rear end of the guide grooves 8 on both sides of the main body 1 passes orthogonally to the magnetic path A is detected by both electrodes 5, and the flow velocity of the fluid is measured. In particular, the flow rate is measured.

この場合磁路Aは、ヨーク4によつて磁極が小
さな幅で対向することになるので短い範囲で集中
して形成されて収束し、磁界が拡大してしまうこ
とはなく、管路10自体が磁性体製、非磁性体製
の如何を問わず磁路Aが影響を受けることは少な
く、極めて正確な測定が達成される。
In this case, since the magnetic poles of the magnetic path A face each other with a small width due to the yoke 4, the magnetic path A is formed and converged in a short range, and the magnetic field does not expand, and the conduit 10 itself Regardless of whether it is made of magnetic material or non-magnetic material, the magnetic path A is hardly affected, and extremely accurate measurements can be achieved.

更には、両磁極の先端であるヨーク4の先端
は、夫々ガイド溝8を挟んで対向し、流体は、こ
のガイド溝8の前端から後端にかけて流れるた
め、両磁極の直線的な最短距離間に直交する状態
で流れることになり、しかも前述したようにこの
ガイド溝8部分には両電極5が露出位置している
ので、小型で消費電力が少なくて済むにも拘ら
ず、しかも管路10の影響を受けることもなく、
高精度の検知を可能にできる。
Furthermore, the tips of the yokes 4, which are the tips of both magnetic poles, are opposed to each other across the guide groove 8, and the fluid flows from the front end to the rear end of the guide groove 8, so that the shortest linear distance between the two magnetic poles is Moreover, as mentioned above, since both electrodes 5 are exposed in the guide groove 8 portion, it is possible to reduce the size and consume less power. without being affected by
It enables highly accurate detection.

また第5図は本発明の精度を示すグラフであつ
て、ここでは内径100mmの磁性管内に於けるメー
トル単位の毎秒の流速結果であり、横軸に実速値
として実際の値をとり、縦軸に指示値として本体
1の示した値をとる。
Fig. 5 is a graph showing the accuracy of the present invention. Here, it shows the flow velocity results in meters per second in a magnetic tube with an inner diameter of 100 mm. The horizontal axis is the actual velocity value, and the vertical axis is the actual velocity value. The value indicated by the main body 1 is taken as the indicated value on the axis.

この試験データよりして、本体1の測定値が実
速に対して極めて直線的であることが理解されよ
う。第5図bは特に微流速部分の拡大であるが、
ここでの数値も極めてリニアであり、0.005m/
secの数値までデータを検証している。
From this test data, it will be understood that the measured value of the main body 1 is extremely linear with respect to the actual speed. Figure 5b is an enlargement of the part with particularly low flow velocity.
The numbers here are also extremely linear, 0.005m/
The data has been verified up to the sec value.

即ち本発明では、ヨーク4の付設によつて局部
的に磁路Aの密度を濃くしたことに加え、低周波
矩形波励磁方式を採用したが故に、流体の微流速
域での測定精度も、極めて高いのである。これ
は、前記第5図のデータが磁性体製管を用いての
ものであるにも拘らず、リニアであることからも
証明される。
That is, in the present invention, in addition to locally increasing the density of the magnetic path A by attaching the yoke 4, since a low frequency rectangular wave excitation method is adopted, the measurement accuracy in the small flow velocity region of the fluid is also improved. This is extremely high. This is evidenced by the fact that the data shown in FIG. 5 is linear even though it is based on a tube made of magnetic material.

そして構成が簡単であるので管路に容易に装着
できる効果も有する。
Further, since the structure is simple, it has the advantage that it can be easily attached to a conduit.

第4図の実施例では既設管路10への組付け状
態を示している。ここでは管路10の一部に仕切
弁11、グランドフランジ12等を介して本体1
を装着し、本体1上端を流れ方向指示ハンドル1
3に連結する。そして該ハンドル13を操作し
て、管路10内の流動方向に対応して本体1の姿
勢を制御するのである。
The embodiment shown in FIG. 4 shows a state in which it is assembled into an existing pipe line 10. Here, the main body 1 is connected to a part of the pipe line 10 via a gate valve 11, a gland flange 12, etc.
Attach the flow direction indicator handle 1 to the upper end of the main body 1.
Connect to 3. By operating the handle 13, the attitude of the main body 1 is controlled in accordance with the flow direction within the conduit 10.

また、例えば橋梁側に露出した既設管路10の
エア抜きに本体1を装着し、従来の既設流速計の
精度チエツクの為に本発明の装置を利用すること
も可能となり、或いは組付け固定自体を上記エア
抜きを利用して行なつてもよい。即ち、ここでの
装置は固定的にも臨時的にも実施できるのであ
る。
Furthermore, it is also possible to use the device of the present invention to check the accuracy of a conventional existing current meter by attaching the main body 1 to the air vent of the existing conduit 10 exposed on the bridge side, or by simply assembling and fixing the device itself. This may be done using the air bleed mentioned above. That is, the device here can be implemented either permanently or temporarily.

よつて本発明の電磁式流速測定装置によれば、
材質の如何を問わず既設の管路内に簡単に装着で
き、精度が極めて高く、可動部分がないので、流
体による摩耗、故障等の支障がなく、長期にわた
つて安定した測定ができ、構成が簡単であつて、
小型であり、作業性が高く低廉である等、多くの
優れた作用効果を有する。
Therefore, according to the electromagnetic flow rate measuring device of the present invention,
It can be easily installed into existing pipes regardless of the material, has extremely high accuracy, and has no moving parts, so there is no problem such as wear due to fluids or failures, and stable measurement can be performed over a long period of time. is easy and
It has many excellent functions and effects, such as being small, highly workable, and inexpensive.

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

第1図は本発明の流速計本体の一実施例を示す
側面図、第2図は側面断面図、第3図は正面断面
図、第4図は管路に装着した状態の断面図、第5
図は本発明に於ける本体の精度を示すグラフであ
る。 符号の説明、1……流速計本体、2……電磁コ
イル、3……コア、4……ヨーク、5,6……電
極、A……磁路。
Fig. 1 is a side view showing one embodiment of the current meter main body of the present invention, Fig. 2 is a side sectional view, Fig. 3 is a front sectional view, Fig. 4 is a sectional view of the flowmeter installed in a pipe, and 5
The figure is a graph showing the accuracy of the main body in the present invention. Explanation of symbols: 1... current meter body, 2... electromagnetic coil, 3... core, 4... yoke, 5, 6... electrode, A... magnetic path.

Claims (1)

【特許請求の範囲】[Claims] 1 樹脂モールド成形される流速計本体の両側面
に、液体の流路に沿つてガイド溝を設け、前記流
速計本体の内部に、電磁コイルが巻回されたコア
の両磁極を、ヨークを介して近接対向位置させて
ることにより、流体の流路であるガイド溝に直交
する一対の磁路を形成し、更に該一対の磁路内
に、流路と磁路とに直交する姿勢の一対の電極
を、前記ガイド溝部分に露出配置させて電磁流速
計を構成し、該電磁流速計を流体管路内に配置し
て成る電磁式流速測定装置。
1 Guide grooves are provided along the liquid flow path on both sides of the resin-molded current meter body, and both magnetic poles of the core around which the electromagnetic coil is wound are inserted into the inside of the current meter body through a yoke. By arranging them in close and opposing positions, a pair of magnetic paths orthogonal to the guide groove, which is a fluid flow path, is formed, and furthermore, within the pair of magnetic paths, a pair of magnetic paths are placed in positions perpendicular to the flow path and the magnetic path. An electromagnetic current velocity measuring device comprising: an electromagnetic current meter having an electrode exposed in the guide groove portion; and an electromagnetic current meter disposed within a fluid conduit.
JP3541384A 1984-02-28 1984-02-28 Electromagnetic flow rate measuring instrument Granted JPS60179613A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3541384A JPS60179613A (en) 1984-02-28 1984-02-28 Electromagnetic flow rate measuring instrument

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3541384A JPS60179613A (en) 1984-02-28 1984-02-28 Electromagnetic flow rate measuring instrument

Publications (2)

Publication Number Publication Date
JPS60179613A JPS60179613A (en) 1985-09-13
JPH0530203B2 true JPH0530203B2 (en) 1993-05-07

Family

ID=12441190

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3541384A Granted JPS60179613A (en) 1984-02-28 1984-02-28 Electromagnetic flow rate measuring instrument

Country Status (1)

Country Link
JP (1) JPS60179613A (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54123768U (en) * 1978-02-16 1979-08-29
JPS57156563A (en) * 1981-03-20 1982-09-27 Morioka Keiki Seisakusho:Kk Electromagnetic current meter

Also Published As

Publication number Publication date
JPS60179613A (en) 1985-09-13

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