JP3015580B2 - Electromagnetic flow meter - Google Patents
Electromagnetic flow meterInfo
- Publication number
- JP3015580B2 JP3015580B2 JP4058516A JP5851692A JP3015580B2 JP 3015580 B2 JP3015580 B2 JP 3015580B2 JP 4058516 A JP4058516 A JP 4058516A JP 5851692 A JP5851692 A JP 5851692A JP 3015580 B2 JP3015580 B2 JP 3015580B2
- Authority
- JP
- Japan
- Prior art keywords
- fluid
- electromagnetic flowmeter
- flow meter
- full
- electromagnetic
- 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 - Fee Related
Links
Landscapes
- Measuring Volume Flow (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、電磁流量計の非満管流
の測定に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to the measurement of non-full flow of an electromagnetic flowmeter.
【0002】[0002]
【従来の技術】従来の電磁流量計では、図2(a)、
(b)に示すように、測定流体が流れる測定管22にお
いて流体が満水状態であるときのみ本来の測定性能を発
揮する。もし、流体が満水でない状態の場合、例えば、
満水水位Aから電極23が流体に接液する限界水位Bの
間では、電極23が流体に接液する限界水位Bに下がる
に従って、電磁流量計21の指示が実際の流量に比べて
大きく出ることが一般に知られている。2. Description of the Related Art In a conventional electromagnetic flow meter, FIG.
As shown in (b), the original measurement performance is exhibited only when the fluid is full in the measurement tube 22 through which the measurement fluid flows. If the fluid is not full, for example,
Between the full water level A and the limit water level B at which the electrode 23 comes into contact with the fluid, the indication of the electromagnetic flowmeter 21 becomes larger than the actual flow rate as the electrode 23 comes down to the limit water level B at which it comes into contact with the fluid. Is generally known.
【0003】また、限界水位Bよりも更に下がり、電極
23が流体に接液しなくなると、もはや流量を測定する
ことは困難となる。[0003] Further, when the water level falls further below the limit water level B and the electrode 23 does not come into contact with the fluid, it is no longer possible to measure the flow rate.
【0004】実際に電磁流量計を設置する場所の配管状
態から満水状態にすることができない場合や、また、満
水状態にはできるがそれを実現するための配管に多大の
費用を要するといった場合には、電磁流量計本来の性能
の特徴である高精度な測定を行えなかったり、水位によ
っては測定不能になることがあった。[0004] When it is not possible to make a pipe full at the place where the electromagnetic flowmeter is actually installed, or when it is possible to make the pipe full but the pipe for realizing it is very expensive. May not be able to perform high-precision measurement, which is a characteristic feature of the performance of the electromagnetic flowmeter, or may be impossible to measure depending on the water level.
【0005】[0005]
【発明が解決しようとする課題】上記のように従来の技
術では、電磁流量計21の測定管22内の流体が満管状
態でない場合には、正確な流量測定が不可能であった。
そこで本発明は、たとえ測定管22内の流体が満水状態
でなくても問題なく流量を正確に測定できる電磁流量計
を実現することを目的とする。As described above, in the prior art, accurate measurement of the flow rate was impossible if the fluid in the measuring pipe 22 of the electromagnetic flow meter 21 was not full.
Therefore, an object of the present invention is to realize an electromagnetic flowmeter that can accurately measure a flow rate without any problem even if the fluid in the measurement tube 22 is not full.
【0006】[0006]
【課題を解決するための手段】本発明の電磁流量計は、
測定管内に、測定する流体とほぼ同等の電気伝導度の材
料から成り測定管の軸線方向に複数の貫通穴が穿設され
た円柱体を電極と接触するように配置したことを特徴と
する。The electromagnetic flow meter according to the present invention comprises:
A cylindrical body made of a material having substantially the same electrical conductivity as the fluid to be measured and having a plurality of through holes formed in the axial direction of the measuring tube is arranged in the measuring tube so as to be in contact with the electrode.
【0007】[0007]
【作用】本発明の電磁流量計においては、測定管内に、
流体とほぼ同等の電気伝導度の材料から成り測定管の軸
線方向に複数の貫通穴が明いた円柱体を電極と接触する
ように配置したため、あたかも満水状態であるような条
件を作り出すことができる。したがって、水位によって
流体が通過する貫通穴は変るが、各穴を通過する流量
は、電磁流量計の重み関数磁束分布により正確に電極間
起電力として発生し、その結果、測定管内が満水状態で
なくても正確な流量指示が得られる。In the electromagnetic flow meter according to the present invention, the inside of the measuring tube is
A cylindrical body made of a material with almost the same electrical conductivity as the fluid and having multiple through holes in the axial direction of the measurement tube is arranged so as to be in contact with the electrodes, so that conditions can be created as if the water were full. . Therefore, the through hole through which the fluid passes varies depending on the water level, but the flow rate passing through each hole is accurately generated as an interelectrode electromotive force due to the weight function magnetic flux distribution of the electromagnetic flowmeter, and as a result, the measurement pipe is filled with water. Accurate flow indication can be obtained without it.
【0008】[0008]
【実施例】以下、図面に示した実施例に基づいて本発明
を詳細に説明する。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, the present invention will be described in detail based on embodiments shown in the drawings.
【0009】図1(a)、(b)に本発明一実施例の電
磁流量計を示す。図示のように、従来と同様な電磁流量
計11の測定管12内に、測定する流体とほぼ同等の電
気伝導度の材料、例えば、導電性プラスチックス、導電
性セラミックス、または流体が浸み込むような多孔性材
料等から成り測定管12の軸線方向に複数の貫通穴14
が穿設された円柱体15が、一対の電極13と接触する
ように、測定管12の全長にわたって配置されている。FIGS. 1A and 1B show an electromagnetic flow meter according to an embodiment of the present invention. As shown in the drawing, a material having substantially the same electrical conductivity as the fluid to be measured, for example, conductive plastics, conductive ceramics, or fluid permeates into the measuring tube 12 of the electromagnetic flow meter 11 similar to the conventional one. A plurality of through-holes 14 are formed in the axial direction of the measuring tube 12 made of such a porous material.
Is arranged over the entire length of the measuring tube 12 so as to contact the pair of electrodes 13.
【0010】上記のように構成された本発明一実施例の
電磁流量計の作用を以下に説明する。従来の電磁流量計
の磁束分布は、満水状態において測定管断面の各位置で
の流体の微小要素について電極間に発生する起電力に対
する寄与がその微小要素の断面積にほぼ比例するような
分布、すなわち、測定管中央部が強く、電極近辺が弱い
磁束分布を実現していて、いわゆる重み関数磁束分布と
なっている。すなわち、従来の電磁流量計は、測定管内
の流体が満水状態ならば、一部の断面要素の流体のみが
流れ、他の流体が停止していても、その断面要素の流量
を正確に測定することができる。The operation of the electromagnetic flow meter according to the embodiment of the present invention configured as described above will be described below. The magnetic flux distribution of the conventional electromagnetic flowmeter is such that the contribution to the electromotive force generated between the electrodes with respect to the microelements of the fluid at each position of the cross section of the measurement tube in a full state is substantially proportional to the cross-sectional area of the microelements, That is, a strong magnetic flux distribution is realized in the central part of the measuring tube and weak in the vicinity of the electrode, which is a so-called weight function magnetic flux distribution. That is, when the fluid in the measuring tube is full, the conventional electromagnetic flowmeter accurately measures the flow rate of the cross-sectional element even when other fluids are stopped and only the fluid of the cross-sectional element is stopped. be able to.
【0011】本発明一実施例の電磁流量計11において
は、測定管12内に、流体とほぼ同等の電気伝導度の材
料から成り測定管12の軸線方向に複数の貫通穴14が
明いた円柱体15を電極13と接触するように配置した
ため、あたかも満水状態であるような条件を作り出すこ
とができる。したがって、水位によって流体が通過する
貫通穴14は変るが、各貫通穴14を通過する流量は、
電磁流量計11の重み関数磁束分布により正確に電極間
起電力として発生し、その結果、測定管12内が満水状
態でなくても正確な流量指示を得ることができる。In the electromagnetic flow meter 11 according to one embodiment of the present invention, a cylinder formed of a material having substantially the same electrical conductivity as a fluid and having a plurality of through holes 14 in the axial direction of the measurement tube 12 is provided in the measurement tube 12. Since the body 15 is arranged so as to be in contact with the electrode 13, it is possible to create a condition as if the body is full. Therefore, the through holes 14 through which the fluid passes vary depending on the water level, but the flow rate through each through hole 14 is
The interelectrode electromotive force is accurately generated by the weight function magnetic flux distribution of the electromagnetic flowmeter 11, and as a result, an accurate flow rate instruction can be obtained even when the inside of the measurement tube 12 is not full.
【0012】[0012]
【発明の効果】以上詳述したように本発明によれば、測
定管内に、測定する流体とほぼ同等の電気伝導度の材料
から成り測定管の軸線方向に複数の貫通穴が穿設された
円柱体を電極と接触するように配置したことを特徴とす
る電磁流量計を実現したことにより、測定管内があたか
も満水状態であるような条件を作り出すことができるた
め、水位によって流体が通過する貫通穴は変るが、各貫
通穴を通過する流量は、電磁流量計の重み関数磁束分布
により正確に電極間起電力として発生し、その結果、測
定管内が満水状態でない場合も正確に流量を測定でき
る。また、従来の電磁流量計に本発明にかかる円柱体を
測定管内に配置することで簡単に実現することができ、
既設の電磁流量計の活用が可能であるため、簡単且つ安
価に実現できる。As described above in detail, according to the present invention, a plurality of through-holes are formed in the measuring tube in the axial direction of the measuring tube made of a material having substantially the same electrical conductivity as the fluid to be measured. By realizing an electromagnetic flowmeter characterized by arranging a cylindrical body so as to be in contact with the electrodes, it is possible to create a condition where the inside of the measurement pipe is full, so that the fluid level allows the fluid to pass through. Although the hole changes, the flow rate passing through each through-hole is accurately generated as an interelectrode electromotive force due to the weight function magnetic flux distribution of the electromagnetic flowmeter, and as a result, the flow rate can be accurately measured even when the inside of the measurement pipe is not full. . Further, it can be easily realized by arranging the cylindrical body according to the present invention in a conventional electromagnetic flowmeter in a measurement tube,
Since the existing electromagnetic flowmeter can be used, it can be realized simply and inexpensively.
【図1】本発明一実施例の電磁流量計を示し、図1
(a)は測定管軸を含む断面図であり、図1(b)は電
極を含み測定管軸に直角な断面図である。FIG. 1 shows an electromagnetic flow meter according to an embodiment of the present invention.
FIG. 1A is a cross-sectional view including a measurement tube axis, and FIG. 1B is a cross-sectional view including electrodes and perpendicular to the measurement tube axis.
【図2】従来の電磁流量計を示し、図2(a)は測定管
軸を含む断面図であり、図2(b)は電極を含み測定管
軸に直角な断面図である。FIG. 2 shows a conventional electromagnetic flowmeter, FIG. 2 (a) is a cross-sectional view including a measuring pipe axis, and FIG. 2 (b) is a cross-sectional view including electrodes and perpendicular to the measuring pipe axis.
11…電磁流量計 12…測定管 13…電極 14…貫通穴 15…円柱体 DESCRIPTION OF SYMBOLS 11 ... Electromagnetic flowmeter 12 ... Measuring tube 13 ... Electrode 14 ... Through-hole 15 ... Cylindrical body
Claims (4)
電気伝導度の材料から成り測定管の軸線方向に複数の貫
通穴が穿設された円柱体を電極と接触するように配置し
たことを特徴とする電磁流量計。1. A cylindrical body made of a material having substantially the same electrical conductivity as a fluid to be measured and having a plurality of through holes formed in an axial direction of the measuring tube is disposed in the measuring tube so as to contact the electrode. An electromagnetic flowmeter characterized by the following.
ことを特徴とする請求項1記載の電磁流量計。2. The electromagnetic flow meter according to claim 1, wherein the cylindrical body is made of conductive plastics.
とを特徴とする請求項1記載の電磁流量計。3. The electromagnetic flowmeter according to claim 1, wherein the cylinder is made of a conductive ceramic.
とする請求項1記載の電磁流量計。4. The electromagnetic flowmeter according to claim 1, wherein the column is made of a porous material.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4058516A JP3015580B2 (en) | 1992-03-17 | 1992-03-17 | Electromagnetic flow meter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4058516A JP3015580B2 (en) | 1992-03-17 | 1992-03-17 | Electromagnetic flow meter |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH05264307A JPH05264307A (en) | 1993-10-12 |
JP3015580B2 true JP3015580B2 (en) | 2000-03-06 |
Family
ID=13086595
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4058516A Expired - Fee Related JP3015580B2 (en) | 1992-03-17 | 1992-03-17 | Electromagnetic flow meter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP3015580B2 (en) |
-
1992
- 1992-03-17 JP JP4058516A patent/JP3015580B2/en not_active Expired - Fee Related
Also Published As
Publication number | Publication date |
---|---|
JPH05264307A (en) | 1993-10-12 |
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