JPS6226407B2 - - Google Patents
Info
- Publication number
- JPS6226407B2 JPS6226407B2 JP54073291A JP7329179A JPS6226407B2 JP S6226407 B2 JPS6226407 B2 JP S6226407B2 JP 54073291 A JP54073291 A JP 54073291A JP 7329179 A JP7329179 A JP 7329179A JP S6226407 B2 JPS6226407 B2 JP S6226407B2
- Authority
- JP
- Japan
- Prior art keywords
- float
- flow rate
- pipe
- flow
- electromagnetic coil
- 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
【発明の詳細な説明】
本発明は浮子を管路に内蔵浮遊させ流体の流れ
による浮子の変位量で流量を測定する方法を改良
し、浮子の変位を磁界の強さに変換して流量を測
定する方法に関するものである。[Detailed Description of the Invention] The present invention improves the method of floating a float inside a pipe and measuring the flow rate based on the amount of displacement of the float caused by the flow of fluid, and converts the displacement of the float into the strength of a magnetic field to measure the flow rate. It concerns the method of measurement.
浮子式の流量計は浮子の変位量を管路壁に設け
た目盛によつて読取る方式であるため目測に個人
差を生じやすい、概算値の測定しかできない等の
問題点があり、簡便ではあるが正確な測定は期待
できない。 Float-type flowmeters are simple, but they have problems such as the amount of displacement of the float being read using a scale installed on the pipe wall, which tends to cause individual differences in visual measurements and can only measure approximate values. However, accurate measurements cannot be expected.
そこで、差動トランスの原理を利用して流体管
路に磁性を有する浮子を内蔵すると共にこの流体
管路を囲んで吸引用の励磁コイルを設け、且つそ
の前後に差動トランスを形成するコイルを配置し
た流量計が実公昭49−41329号公報に開示されて
いる。この公報に開示のものは、流速零のとき励
磁コイルの中央に置かれている浮子が流れによつ
て移動する変位量を差動トランスの起電力変化で
読取るので、管路壁の目盛によつて読取るものに
比べて正確であるが、三組のコイルを用いている
ため構成が複雑であり、また励磁コイルの磁力に
よる復元力を超えて浮子が移動するとそのまま流
失するという不都合がある。 Therefore, by utilizing the principle of a differential transformer, a magnetic float is built into the fluid pipe, an excitation coil for attraction is provided surrounding the fluid pipe, and coils forming a differential transformer are installed before and after the excitation coil. The arranged flowmeter is disclosed in Japanese Utility Model Publication No. 49-41329. The system disclosed in this publication uses the scale on the pipe wall to read the displacement of the float placed in the center of the excitation coil due to the flow when the flow velocity is zero, based on changes in the electromotive force of the differential transformer. Although this method is more accurate than one that is read by hand, it has a complicated structure because it uses three sets of coils, and it also has the disadvantage that if the float moves beyond the restoring force of the excitation coil's magnetic force, it will be washed away.
本発明は一個の電磁コイルを用いた簡単な構成
で浮子を流失させる心配なく正確な流量測定を電
気的に行うことができる方法を提供するものであ
つて、流体が流れる管路を鉛直に配置し、この管
路を囲んで電磁コイルを設置すると共にこの電磁
コイルが作る磁界に反発する浮子を管路に内蔵し
て浮遊させ、管路内の流れにより浮子が変位した
とき電磁コイルに供給する電流を変え磁界の強さ
を変化させることによつて浮子を流量零の位置へ
戻し、この電流変化量により流体の流量を測定す
ることを特徴とするものである。 The present invention provides a method that can electrically measure the flow rate accurately without worrying about the float being washed away with a simple configuration using a single electromagnetic coil, and in which the pipe line through which the fluid flows is arranged vertically. Then, an electromagnetic coil is installed surrounding this pipe, and a float that repels the magnetic field created by this electromagnetic coil is built into the pipe and floats, and when the float is displaced by the flow in the pipe, it is supplied to the electromagnetic coil. The feature is that the float is returned to the zero flow position by changing the current and the strength of the magnetic field, and the flow rate of the fluid is measured based on the amount of change in current.
以下本発明の実施の態様を図面に就いて説明す
ると、第1図および第2図において1は鉛直に配
置された管路、2は磁石で作られたまたは磁石を
一部に有する或いは磁性材料で作られた円錐形の
浮子、3は管路1を囲んで設置された電磁コイ
ル、4は電源、5は電流を無段階に変化させる可
変抵抗器のような電流調整器、6は電流を流体の
流量に換算して表示する流量表示計を示してい
る。 Embodiments of the present invention will be described below with reference to the drawings. In FIGS. 1 and 2, 1 is a pipe line arranged vertically, and 2 is a pipe made of a magnet, has a magnet in a part, or is made of a magnetic material. A conical float made of A flow rate display meter that converts and displays the flow rate of fluid is shown.
第1図は管路1に内蔵した浮子2の重量が浮力
より大きい場合であつて、電磁コイル3が作る磁
界に反発して流れのないとき重量Fg浮力Fb、磁
力Fnの平衡した位置即ち電磁コイル3の上方に
浮子2が浮遊して静止している。この状態で浮子
2の受ける力Fは
F=Fg+Fb+Fn=0
となつている。管路1に矢印Aで示すように上向
きの流れを生じたとき浮子2はこの流れによつて
上向きの力Ffを受け、
F=Ff=Fg+Fb+Fn(但しFf<F)
となつた位置まで移動し停止する。ここで電流調
整器5を操作して△F=Fn−Ffなる力△Fを電
磁コイル3による磁界の強さを変えることによつ
て附加すると浮子2は流量零の位置へ戻され、従
つてこの力△Fを作り出すに要した電流即ち流量
零のときの電流からの電流変化量に相当する流量
の値を流量表示計6によつて読取り或いは記録し
て流量を知るのである。浮子2が流量零の位置よ
り降下してもF>0となるためF=0の位置に引
き戻される。この実施例では流れを生じたときF
<0となり浮子2は電磁コイル1から遠ざかるの
で電流を減少させFnを小さくしてF=0とする
のである。 Figure 1 shows the case where the weight of the float 2 built into the pipe 1 is greater than the buoyant force, and when there is no flow due to repulsion to the magnetic field created by the electromagnetic coil 3, the weight F g buoyant force F b and the magnetic force F n are balanced. The float 2 is floating and stationary above the electromagnetic coil 3. In this state, the force F that the float 2 receives is F=F g +F b +F n =0. When an upward flow is generated in the pipe 1 as shown by arrow A, the float 2 receives an upward force F f due to this flow, F=F f =F g +F b +F n (however, F f <F ) and stops. When the current regulator 5 is operated to apply a force ΔF of ΔF=F n −F f by changing the strength of the magnetic field by the electromagnetic coil 3, the float 2 is returned to the zero flow position. Therefore, the flow rate is determined by reading or recording the flow rate value corresponding to the current required to create this force ΔF, that is, the amount of change in current from the current when the flow rate is zero, using the flow rate indicator 6. Even if the float 2 descends from the zero flow rate position, F>0, so it is pulled back to the F=0 position. In this example, when a flow is generated, F
<0, and the float 2 moves away from the electromagnetic coil 1, so the current is decreased and F n is made smaller, so that F=0.
第2図は浮子2の浮力が重量より大きい場合で
あつて、電磁コイル3の下方に浮子2が浮遊して
静止している。管路1に矢印Aで示す上向きの流
れを生じたとき浮子2はこの流れによつて前記同
様上向きの力Fを受けてF=Ffとなる位置まで
上昇して電磁コイル3に接近して停止するので、
△F=Fn−Ffなる力△Fを附加して浮子2を流
量零の位置へ戻す。この実施例では流れを生じた
ときF>0となり電流を増加させてFnを大きく
してF=0とするもので、この力△Fを作り出す
に要した電流値に相当する流量の値を流量表示計
6によつて読取り或いは記録して流量を知るので
ある。 FIG. 2 shows a case where the buoyancy of the float 2 is greater than its weight, and the float 2 is floating and stationary below the electromagnetic coil 3. When an upward flow is generated in the pipe line 1 as indicated by the arrow A, the float 2 receives an upward force F due to this flow and rises to a position where F=F f and approaches the electromagnetic coil 3. Because it stops,
A force ΔF of ΔF=F n −F f is applied to return the float 2 to the position of zero flow rate. In this example, when a flow is generated, F > 0, the current is increased, F n is increased, and F = 0.The value of the flow rate corresponding to the current value required to create this force △F is The flow rate is known by reading or recording it with the flow rate indicator 6.
ここで、Fg,Fbは浮子2の体積、重量および
流体の比重によつて初期条件として与えられるも
ので流体の流れが一様であれば一定値を示すた
め、△Fなる力を作るように磁界の強さを変化さ
せるに要した電流値を測定することによりFfの
大きさを知り最終的に流量が正確に判明する。 Here, F g and F b are given as initial conditions by the volume and weight of the float 2 and the specific gravity of the fluid, and if the fluid flow is uniform, they show constant values, so a force of △F is created. By measuring the current value required to change the strength of the magnetic field, the magnitude of F f can be determined, and ultimately the flow rate can be determined accurately.
尚、脈流等の瞬間的な流量変化に対しては管路
壁に目盛を設け浮子2の瞬間的な変位を目測によ
り測定して流量を知るようにすることもある。 For instantaneous flow rate changes such as pulsating flow, a scale may be provided on the pipe wall and the instantaneous displacement of the float 2 may be visually measured to determine the flow rate.
また、本発明では電磁コイル3に与える電流を
決定すると磁力Fnが決定され流量零のときの浮
子2の位置が定まるので、流量変化に伴う浮子2
の上限、下限を設定しておき浮子2が上限、下限
に変位したときこれを感知しポンプ、流量制御弁
にフイードバツクすることにより一定範囲内の流
量に制御することができる。また流量表示計6の
代りに電流計を用い電流を流量に換算表によつて
換算することもある。更にまた管路1の浮子2が
浮遊する部分は直管に限らず上方へ拡大するテー
パ管であつてもよい。 Furthermore, in the present invention, when the current applied to the electromagnetic coil 3 is determined, the magnetic force F n is determined, and the position of the float 2 when the flow rate is zero is determined.
The flow rate can be controlled within a certain range by setting the upper and lower limits of the flow rate, sensing when the float 2 moves to the upper and lower limits, and providing feedback to the pump and flow control valve. Further, an ammeter may be used instead of the flow rate indicator 6, and the current may be converted into a flow rate using a conversion table. Furthermore, the portion of the pipe line 1 on which the float 2 floats is not limited to a straight pipe, but may be a tapered pipe that expands upward.
以上のように本発明によると鉛直に配置した管
路を囲んで電磁コイルを設置してこの電磁コイル
が作る磁界に浮子を反発させ、流体の流量零のと
きの位置から流れによつて浮子が変位したとき磁
界の強さを変化させて浮子を流量零の位置へ戻
し、このとき電磁コイルへ与える電流の変化量に
よつて流量を測定するものであるから、管路壁に
目盛を設け浮子の変位を直接読取る通常の浮子式
流量計のように個人差が生じ正確に測定できない
等の欠点を伴わないものである。また、管路にオ
リフイス、羽根等を設けるという特別の加工を施
す必要がなく、磁性の浮子を内蔵させ且つ外側に
一個の電磁コイルを設置するだけでよいため構成
がきわめて簡単であり、しかも初期条件で与えら
れる浮子の重量と浮力とは鉛直管路において流れ
が一様であれば一定値で与えられるので、流れに
よる浮子の変位に対抗して磁界の強さを変えると
いう簡単な操作で正確な流量測定ができるばかり
か、浮子を流量零の位置へ戻すように磁界の強さ
を変化させているので大流量でも浮子を流失させ
る心配なく取扱えるのである。更に、本発明は電
磁コイルへ与える電流を変化させるためそのまま
流量を記録し或いは流量制御を行わせることがで
きる等利用範囲の広いものである。 As described above, according to the present invention, an electromagnetic coil is installed surrounding a vertically arranged pipe line, and the float is repelled by the magnetic field created by this electromagnetic coil, and the float is moved by the flow from the position when the fluid flow rate is zero. When the float is displaced, the strength of the magnetic field is changed to return the float to the zero flow position, and the flow rate is measured by the amount of change in the current applied to the electromagnetic coil at this time, so a scale is provided on the pipe wall and the float It does not have the drawbacks of a conventional rotary flowmeter that directly reads the displacement of the flowmeter, such as the inability to measure accurately due to individual differences. In addition, there is no need to perform special processing such as installing orifices or blades in the conduit, and it is only necessary to incorporate a magnetic float and install one electromagnetic coil on the outside, making the configuration extremely simple. The weight and buoyancy of the float given by the conditions are given as constant values if the flow is uniform in a vertical pipe, so they can be accurately determined by a simple operation of changing the strength of the magnetic field to counteract the displacement of the float due to the flow. Not only is it possible to measure the flow rate, but because the strength of the magnetic field is changed to return the float to the zero flow position, it can be handled even at large flow rates without worrying about the float being washed away. Furthermore, the present invention has a wide range of applications, such as being able to record the flow rate or control the flow rate by changing the current applied to the electromagnetic coil.
第1図および第2図は本発明の異なる実施の態
様を示す説明図である。
1……管路、2……浮子、3……電磁コイル、
4……電源、5……電流調整器、6……流量表示
計。
FIGS. 1 and 2 are explanatory diagrams showing different embodiments of the present invention. 1... Pipeline, 2... Float, 3... Electromagnetic coil,
4...Power supply, 5...Current regulator, 6...Flow rate display meter.
Claims (1)
を囲んで電磁コイルを設置すると共にこの電磁コ
イルが作る磁界に反発する浮子を管路に内蔵して
浮遊させ、管路内の流れにより浮子が変位したと
き電磁コイルに供給する電流を変え磁界の強さを
変化させることによつて浮子を流量零の位置へ戻
し、この電流変化量により流体の流量を測定する
ことを特徴とする流量測定方法。1 A pipe through which fluid flows is arranged vertically, an electromagnetic coil is installed surrounding this pipe, and a float that repels the magnetic field created by this electromagnetic coil is built into the pipe and floated, and the flow inside the pipe is A flow rate characterized in that when the float is displaced, the current supplied to the electromagnetic coil is changed to change the strength of the magnetic field to return the float to the zero flow position, and the flow rate of the fluid is measured based on the amount of change in current. Measuring method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7329179A JPS55164311A (en) | 1979-06-11 | 1979-06-11 | Flow rate measuring method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7329179A JPS55164311A (en) | 1979-06-11 | 1979-06-11 | Flow rate measuring method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS55164311A JPS55164311A (en) | 1980-12-22 |
| JPS6226407B2 true JPS6226407B2 (en) | 1987-06-09 |
Family
ID=13513897
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7329179A Granted JPS55164311A (en) | 1979-06-11 | 1979-06-11 | Flow rate measuring method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS55164311A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN100469413C (en) * | 2003-05-13 | 2009-03-18 | A.L.哈达斯技术有限公司 | Device for measuring the volumetric or mass flow rate of a fluid |
| JP2009287992A (en) * | 2008-05-28 | 2009-12-10 | Kondo Kogyo Kk | Float type minute pressure difference display device |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4941329U (en) * | 1972-07-13 | 1974-04-11 |
-
1979
- 1979-06-11 JP JP7329179A patent/JPS55164311A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS55164311A (en) | 1980-12-22 |
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