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JPS597931B2 - electromagnetic flow meter - Google Patents
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JPS597931B2 - electromagnetic flow meter - Google Patents

electromagnetic flow meter

Info

Publication number
JPS597931B2
JPS597931B2 JP3159679A JP3159679A JPS597931B2 JP S597931 B2 JPS597931 B2 JP S597931B2 JP 3159679 A JP3159679 A JP 3159679A JP 3159679 A JP3159679 A JP 3159679A JP S597931 B2 JPS597931 B2 JP S597931B2
Authority
JP
Japan
Prior art keywords
magnetic
magnetic flux
electrodes
magnetic circuit
excitation
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
JP3159679A
Other languages
Japanese (ja)
Other versions
JPS55124015A (en
Inventor
和雄 上野
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.)
Aichi Tokei Denki Co Ltd
Original Assignee
Aichi Tokei Denki Co Ltd
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 Aichi Tokei Denki Co Ltd filed Critical Aichi Tokei Denki Co Ltd
Priority to JP3159679A priority Critical patent/JPS597931B2/en
Priority to US06/175,611 priority patent/US4409846A/en
Publication of JPS55124015A publication Critical patent/JPS55124015A/en
Publication of JPS597931B2 publication Critical patent/JPS597931B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 この発明は、導電性の流体の少くとも部分を直接に挾ん
で相対する1対の電極と、両電極を通る直線と流れとの
両者に交叉する磁束を生ずる磁気回路と、この磁気回路
の磁束と流体の流れとに起因して両電極間に生ずる電圧
に基いて流速を算定する電磁流量計に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention comprises a pair of opposing electrodes that directly sandwich at least a portion of a conductive fluid, and a magnetic circuit that generates a magnetic flux that intersects both a straight line and a flow passing through both electrodes. The present invention relates to an electromagnetic flowmeter that calculates flow velocity based on the voltage generated between both electrodes due to the magnetic flux of the magnetic circuit and the flow of fluid.

この電磁流量計において、電極の電気化学的作用による
大幅な零点変動はなく、流体が流れつつある間でも零点
の確認が容易であるという条件を満足しつつ、しかも電
力消費を極めて少くする目的で、励磁線輪に流す励磁電
流を間欠的で毎回瞬間的でかつ交互に方向が反対のもの
とし、励磁電流が流れない間に磁気回路が保つ残留磁束
と流体の流れとに起因して両電極間に生ずる電圧に基き
流速を算定するようにした電磁流量計を、さきに本件出
願人は特許出願をした。
The purpose of this electromagnetic flowmeter is to satisfy the conditions that there is no significant zero point fluctuation due to the electrochemical action of the electrodes, and that the zero point can be easily checked even while the fluid is flowing, while also minimizing power consumption. , the excitation current applied to the excitation coil is intermittent, instantaneous, and alternately in opposite directions, and the magnetic circuit maintains a residual magnetic flux and fluid flow between the two electrodes while the excitation current does not flow. The applicant previously filed a patent application for an electromagnetic flowmeter that calculates the flow velocity based on the voltage generated between the two.

ところで、このものでは、環境温度の変化による励磁線
輪の抵抗値の変化が残留磁束の大きさに及ほす影響は、
励磁線輪と直列にそれよりも抵抗温度係数が小さく抵抗
値が大きい温度補償抵抗を接続することで極めて小さく
することができるが磁気回路の構成材料を適当に選ばな
いときは、励磁電流を一定化する手段を具えた場合でも
、環境5温度の変化により残留磁束が変動し、この結果
、測定流速に誤差を生ずる欠点があつた。
By the way, in this case, the effect that the change in the resistance value of the excitation wire ring due to the change in the environmental temperature has on the magnitude of the residual magnetic flux is as follows.
It can be made extremely small by connecting a temperature compensation resistor with a smaller resistance temperature coefficient and a larger resistance value in series with the excitation wire ring, but if the constituent material of the magnetic circuit is not selected appropriately, the excitation current cannot be kept constant. Even when equipped with a means for changing the temperature, the residual magnetic flux fluctuates due to changes in the environmental temperature, resulting in an error in the measured flow velocity.

これにかんがみ、この発明は、前記の間欠反転瞬間励磁
的の電磁流量計において上記の欠点のないものの実現を
目的とするもので、後に実施例について説明するように
、磁気回路を、透磁率が高く残留磁束が小さい高透磁率
材料よりなる継鉄と永久磁石材料よりなる磁石体とを直
列に連結して構成したことを特徴とする電磁流量計であ
る。
In view of this, it is an object of the present invention to realize an intermittent reversal instantaneous excitation electromagnetic flowmeter that does not have the above-mentioned drawbacks. This electromagnetic flowmeter is characterized in that it is configured by connecting in series a yoke made of a high permeability material with a high residual magnetic flux and a magnet body made of a permanent magnet material.

第1図は、この発明の一実施例について導電性5の流体
の流れに直交する断面を示している。流体の管路1は、
この断面の近辺の長手方向の相当の範囲に亘り、非磁性
かつ非導電性である。管路1の内側に露出して、流体の
流れの少くとも部分を直接に挾んで相対する1対の電極
2a、2bがある。各電極2a、2bは管路1の壁を水
密的に貫通する導体部分を介して、両電極2a、2b間
の電圧に基いて流速を算定する流速算定装置3に接続し
てある。管路1を挾んで磁極4a、4bをもつ継鉄5a
!55bを、透磁率が高く残留磁束が小さい高透磁率材
料、例えば電磁軟鉄やけい素鋼板で構成し、電極4a、
4b間に生じた磁束が、両磁極2a、2bを通る直線と
流体の流れとの両者に交叉するようにしてある。
FIG. 1 shows a cross section perpendicular to the flow of a conductive 5 fluid for one embodiment of the invention. The fluid conduit 1 is
It is non-magnetic and non-conductive over a considerable range in the longitudinal direction near this cross section. There is a pair of electrodes 2a, 2b exposed inside the conduit 1 and facing each other so as to directly sandwich at least a portion of the fluid flow. Each electrode 2a, 2b is connected via a conductor portion that penetrates the wall of the conduit 1 in a watertight manner to a flow rate calculation device 3 that calculates the flow rate based on the voltage between the electrodes 2a, 2b. A yoke 5a with magnetic poles 4a and 4b sandwiching the pipe 1
! 55b is made of a high magnetic permeability material with high magnetic permeability and low residual magnetic flux, such as electromagnetic soft iron or silicon steel plate, and the electrodes 4a,
The magnetic flux generated between the magnetic poles 2a and 2b intersects both the straight line passing through the magnetic poles 2a and 2b and the fluid flow.

継鉄5a,5bは磁極4a,4bとは反対の端に、保持
力はそれ程大きくなく磁束の立上Dが急で飽和が速い永
久磁石材料、例えば鋳造したアルニコ1で構成した磁石
体6を挾持し、全体で1の磁気回路4を構成している。
磁石体6の外周には磁気回路4を励磁するための励磁線
輪7を巻きけけ、その線径を太く全抵抗値を小さくして
ある。
The yokes 5a and 5b have a magnet body 6 at the end opposite to the magnetic poles 4a and 4b made of a permanent magnet material such as cast Alnico 1, which does not have a very large holding force but has a rapid rise D of magnetic flux and is quick to saturate. They are sandwiched together to form one magnetic circuit 4 as a whole.
An excitation wire ring 7 for exciting the magnetic circuit 4 is wound around the outer periphery of the magnet body 6, and the wire diameter is made thick and the total resistance value is made small.

励磁線輪7には間欠的で毎回瞬間的でかつ交互に方向が
反対の励磁電流を流す励磁装置8を接続してある。磁石
体6を構成する永久磁石材料を十分な強さの幅を以て往
復変化する磁界に置くとき生ずる磁束との関係が、第2
図に実線で示す線図のように変化するものとする。
An excitation device 8 is connected to the excitation wire ring 7, which supplies excitation current intermittently, instantaneously each time, and alternately in opposite directions. The relationship with the magnetic flux generated when the permanent magnet material constituting the magnet body 6 is placed in a magnetic field that changes back and forth with a sufficient strength width is the second
It is assumed that the change occurs as shown in the solid line diagram in the figure.

次に、第1図の実施例の磁気回路4において継鉄5a,
5bの透磁率は磁極4a,4b間の空隙の透磁率に比べ
て8000〜12000倍と高いので、励磁線輪7の電
流によつてこの空隙に発生する起磁力は磁石体6の端面
間にか\るものと実用上等しい。
Next, in the magnetic circuit 4 of the embodiment shown in FIG.
Since the magnetic permeability of 5b is 8,000 to 12,000 times higher than that of the gap between the magnetic poles 4a and 4b, the magnetomotive force generated in this gap by the current of the excitation wire ring 7 is generated between the end faces of the magnet body 6. It is practically equivalent to

従つて、磁石体6の磁束とそれに起因する磁界との関係
は、磁極4a,4b間のバーシアンス(Pg)を例えば
Pm=Pg><1m/Sm、(ただし1m,Smは磁石
体6の長さ、断面積)なる関係式を使用して、磁石体6
のパーシアソス係数(Pm)に換算した値によつて決ま
る。磁極4a,4b間のパーシアンスは幾何学的に決ま
るから、磁石体6の磁束とそれに起因する磁界との関係
は一定であり、第2図における傾斜線P−ピで表わすこ
とができる。励磁装置8によつて励磁線輪7に流れる電
流によつて磁石体6に生ずる磁界Hの変化が、第2図に
おいて(+h〜−hl)の範囲にとどまるときはその磁
界Hと磁石体6の磁束との関係は第2図にさ線で示す線
図Q−qに沿つて変化するが、その範囲を超えた(+H
〜−Hl)の範囲で変化させるときは、破線で示す線図
R−P−k−ピに沿つて変化させる。
Therefore, the relationship between the magnetic flux of the magnet 6 and the magnetic field caused by it is such that the versiance (Pg) between the magnetic poles 4a and 4b is, for example, Pm=Pg><1m/Sm (where 1m, Sm is the length of the magnet 6). Using the relational expression (S, cross-sectional area), the magnetic body 6
It is determined by the value converted to the Persiassian coefficient (Pm). Since the perceance between the magnetic poles 4a and 4b is determined geometrically, the relationship between the magnetic flux of the magnet body 6 and the magnetic field caused by it is constant, and can be represented by the slope line P--P in FIG. When the change in the magnetic field H generated in the magnet body 6 by the current flowing through the excitation wire ring 7 by the excitation device 8 remains within the range (+h to -hl) in FIG. 2, the magnetic field H and the magnet body 6 change. The relationship with the magnetic flux changes along the diagram Q-q shown by the horizontal line in Figure 2, but beyond that range (+H
-Hl), the change is made along the broken line R-P-k-pi.

このため励磁線輪7の励磁電流がなくなるときは、線図
R−P−k−Yと傾斜線P一?との交点であるP又はν
で安定し、残留磁束はB又は−B′となる。両方向の励
磁電流を等大にすればB=Wとなる。又、前記関係式P
m=Pg>(1m/Smから明一らかなように、磁石体
6の断面積Smを小さく選ぶほどパーシアンスPm力吠
きく、傾斜線P−νは急傾斜し、残留磁気B,B′の絶
対値が大きくなる。
Therefore, when the excitation current of the excitation wire ring 7 disappears, the line diagram R-P-k-Y and the slope line P1? P or ν, which is the intersection with
The residual magnetic flux becomes B or -B'. If the excitation currents in both directions are made equal in magnitude, B=W. Also, the above relational expression P
m=Pg>(1m/Sm As is clear from The absolute value becomes larger.

このように、この発明の電磁流量計では、磁気回路4を
、透磁率が高く残留磁束が小さい高透磁率材料よりなる
継鉄5a,5bと、永久磁石材料よりなる磁石体6とを
直列に連結して構成したから、残留磁束に対する環境温
度の変化の影響は、実質上磁石体6のみによつて定まり
、かつ、磁石体6の材料である永久磁石材料では、その
残留磁束が環境温度の変化に起因して受ける変動が、例
えば一(0.06〜0.02)′F6/℃というように
極めて小さいので、当然、磁極4a,4bの間隙での磁
束の変動も殆んどなくなり、環境温度の変化が測定流速
に誤差を及ぽすという先記の欠点を除去することができ
る。
In this way, in the electromagnetic flowmeter of the present invention, the magnetic circuit 4 is constructed by connecting in series the yokes 5a and 5b made of a high magnetic permeability material with high magnetic permeability and low residual magnetic flux, and the magnet body 6 made of a permanent magnetic material. Because of the connected structure, the influence of changes in the environmental temperature on the residual magnetic flux is substantially determined only by the magnet body 6, and in the permanent magnet material that is the material of the magnet body 6, the residual magnetic flux changes depending on the environmental temperature. Since the fluctuation caused by the change is extremely small, for example, 1 (0.06 to 0.02)'F6/°C, there is naturally almost no fluctuation in the magnetic flux in the gap between the magnetic poles 4a and 4b. The above-mentioned disadvantage that changes in environmental temperature cause errors in the measured flow rate can be eliminated.

なお、第3図に縦断面、第4図に横断面を示す別の実施
例では、管路1の流体の通路断面を局部的に扁平にして
電極4a,4b間の空隙を狭くしその結果磁気回路4の
パーシアンスを高くし、2個の磁石体6a,6b及び2
個の励磁線輪7a,7bを設け、継鉄を、電極4a,4
bと磁石体6a,6bの一端とそれぞれの間の部分5a
,5bと、磁石体6a,6bの他端間の部分5から構成
してある。
In another embodiment, whose longitudinal section is shown in FIG. 3 and whose cross section is shown in FIG. The perseverance of the magnetic circuit 4 is increased, and the two magnet bodies 6a, 6b and 2
Excitation wire rings 7a, 7b are provided, and the yoke is connected to the electrodes 4a, 4.
b and one end of the magnet bodies 6a, 6b and the portion 5a between each
, 5b, and a portion 5 between the other ends of the magnet bodies 6a, 6b.

そしてこれらの部分は、励磁線輪7a97bのリード線
及び電極2a,2bとともに、管路1をプラスチツクで
成形するとき同時にいぐるみによつて関係位置に保持さ
れている。管路1の上側には、励磁線輪7a,7bと接
続した励磁装置8、電極2a,2bと接続した流速算定
装置3、電源電池、及び発信装置等を収納した処理装置
9を取り付けてある。管路1は、両端に金属製の口金1
0を気密的に固くねじこんで、口金10のねじによつて
配管と結合するようにし、かつ、設置状態での長手方向
の引張力に耐える程度の強度をもつている。
These parts, together with the leads of the excitation coil 7a97b and the electrodes 2a, 2b, are held in position by the stuffed toy at the same time as the conduit 1 is molded of plastic. An excitation device 8 connected to excitation wire rings 7a and 7b, a flow rate calculation device 3 connected to electrodes 2a and 2b, a processing device 9 containing a power source battery, a transmitting device, etc. are attached to the upper side of the conduit 1. . The conduit 1 has metal caps 1 on both ends.
0 is tightly screwed in in an airtight manner so as to be connected to the piping by the screw of the base 10, and has enough strength to withstand longitudinal tensile force in the installed state.

このように、磁気回路4の磁石体6a,6b及び継鉄5
,5a,5bを適当に設計することによつて、十分の残
留磁束を得つつ全体を小形にすることができるから、全
体の価格を低く抑えることができる。
In this way, the magnet bodies 6a, 6b of the magnetic circuit 4 and the yoke 5
, 5a, 5b, the overall size can be reduced while obtaining sufficient residual magnetic flux, so the overall price can be kept low.

【図面の簡単な説明】 第1図はこの発明の一実施例の横断面図、第2図は第1
図の実施例における磁石体の残留磁気を説明するための
線図、第3図と第4図とは別の実施例のそれぞれA−A
縦断面図及びB−B横断面図である。 2a,2b・・・電極、4・・・磁気回路、7,7a,
7b・・・励磁線輪、5,5a,5b・・・継鉄、6,
6a,6b・・・磁石体。
[Brief Description of the Drawings] Fig. 1 is a cross-sectional view of one embodiment of the present invention, and Fig. 2 is a cross-sectional view of an embodiment of the present invention.
Diagrams for explaining the residual magnetism of the magnet body in the embodiment shown in the figure, A-A of embodiments different from those in FIGS. 3 and 4, respectively.
They are a longitudinal cross-sectional view and a BB transverse cross-sectional view. 2a, 2b... Electrode, 4... Magnetic circuit, 7, 7a,
7b... Excitation wire ring, 5, 5a, 5b... Yoke, 6,
6a, 6b... magnet bodies.

Claims (1)

【特許請求の範囲】[Claims] 1 導電性の流体の流れの少くとも部分を直接に挾んで
相対する1対の電極と、両電極を通る直線と流れとの両
者に交叉する磁束を生ずる磁気回路と、この磁気回路を
励磁する励磁線輪とをもち、励磁線輪に間欠的で毎回瞬
間的でかつ交互に方向が反対の励磁電流を流し、励磁電
流が流れない間に磁気回路が保つ残留磁束と流体の流れ
とに起因して両電極間に生ずる電圧に基き流速を算定す
るようにした電磁流量計において、磁気回路を、透磁率
が高く残留磁束が小さい高透磁率材料よりなる継鉄と永
久磁石材料よりなる磁石体とを直列に連結して構成した
ことを特徴とする電磁流量計。
1. A pair of opposing electrodes that directly sandwich at least a portion of the flow of a conductive fluid, a magnetic circuit that generates a magnetic flux that crosses both the straight line passing through the electrodes and the flow, and exciting this magnetic circuit. This is caused by the residual magnetic flux and fluid flow maintained by the magnetic circuit when the excitation current is not flowing, and the excitation current is passed through the excitation wire intermittently, instantaneously, and alternately in opposite directions. In an electromagnetic flowmeter that calculates the flow velocity based on the voltage generated between both electrodes, the magnetic circuit is composed of a yoke made of a high permeability material with high magnetic permeability and low residual magnetic flux, and a magnet body made of a permanent magnet material. An electromagnetic flowmeter characterized by being configured by connecting in series.
JP3159679A 1979-02-08 1979-03-16 electromagnetic flow meter Expired JPS597931B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP3159679A JPS597931B2 (en) 1979-03-16 1979-03-16 electromagnetic flow meter
US06/175,611 US4409846A (en) 1979-02-08 1980-08-06 Electromagnetic flow meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3159679A JPS597931B2 (en) 1979-03-16 1979-03-16 electromagnetic flow meter

Publications (2)

Publication Number Publication Date
JPS55124015A JPS55124015A (en) 1980-09-24
JPS597931B2 true JPS597931B2 (en) 1984-02-21

Family

ID=12335569

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3159679A Expired JPS597931B2 (en) 1979-02-08 1979-03-16 electromagnetic flow meter

Country Status (1)

Country Link
JP (1) JPS597931B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH038985Y2 (en) * 1985-08-16 1991-03-06

Also Published As

Publication number Publication date
JPS55124015A (en) 1980-09-24

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