JP4844019B2 - Electromagnetic flow meter - Google Patents

Electromagnetic flow meter

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JP4844019B2
JP4844019B2 JP2005177211A JP2005177211A JP4844019B2 JP 4844019 B2 JP4844019 B2 JP 4844019B2 JP 2005177211 A JP2005177211 A JP 2005177211A JP 2005177211 A JP2005177211 A JP 2005177211A JP 4844019 B2 JP4844019 B2 JP 4844019B2
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magnetic pole
pole core
magnetic
hole
core
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JP2006349539A (en
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雄一 金子
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Yokogawa Electric Corp
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Yokogawa Electric Corp
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本発明は主として小口径の電磁流量計に関し、詳しくは磁極コア内部に発生する渦電流の影響を小さくし、磁気回路の周波数特性を改善した電磁流量計に関する。   The present invention mainly relates to a small-diameter electromagnetic flow meter, and more particularly to an electromagnetic flow meter in which the influence of eddy current generated inside a magnetic pole core is reduced and the frequency characteristics of a magnetic circuit are improved.

図9は、従来より一般に使用されている電磁流量計の原理構成説明図である。
図9に示すように、内径Dのパイプ内に磁束密度Bの一様な磁界が与えられている場合に、平均流速vの導電性液体が流れると、磁界および流れのおのおのの直角な方向に
E=D・v・B
の起電力Eが発生する。
FIG. 9 is a diagram illustrating the principle configuration of an electromagnetic flow meter that has been generally used.
As shown in FIG. 9, when a uniform magnetic field having a magnetic flux density B is applied to a pipe having an inner diameter D, when a conductive liquid having an average flow velocity v flows, the magnetic field and the flow are perpendicular to each other. E = D ・ v ・ B
Electromotive force E is generated.

体積流量Qは
Q=π・D/4・v=π/4・D/B・E
と表されるので、磁束密度Bが一定ならば、流量Qは起電力Eに比例する。電磁流量計はこの起電力Eを検出して、体積流量Qを計測する。
Volume flow Q is Q = π · D 2/4 · v = π / 4 · D / B · E
Therefore, if the magnetic flux density B is constant, the flow rate Q is proportional to the electromotive force E. The electromagnetic flow meter detects the electromotive force E and measures the volume flow rate Q.

図10はこのような電磁流量計の構成を示す断面図である。図において、1は測定すべき導電流体が流れる測定管、2a,2bは測定管の外周に対向して設けられた電極、3a,3bは同じく測定管の外周に電極の取付け方向とは90度回転した位置に対向して設けられた柱状の磁極コアである。この磁極コアの外周にはコイル4が巻きつけられたコイルボビン5が配置され、このコイルボビン5に磁極コア3が挿入された形状となっている。   FIG. 10 is a cross-sectional view showing the configuration of such an electromagnetic flow meter. In the figure, 1 is a measuring tube through which a conductive fluid to be measured flows, 2a and 2b are electrodes provided opposite to the outer periphery of the measuring tube, and 3a and 3b are also 90 ° at the outer periphery of the measuring tube. It is a columnar magnetic pole core provided facing the rotated position. A coil bobbin 5 around which a coil 4 is wound is disposed on the outer periphery of the magnetic pole core, and the magnetic pole core 3 is inserted into the coil bobbin 5.

6a,6bは電極2a,2bの先端に接続された信号線であり、図示の例では電極2bに接続された信号線6bが紙面に向かって下側に位置する磁極コア3bの底部(測定管寄り)に設けられた貫通孔7の中を通って電極2a側に引き出され、電極2aの先端に接続された信号線6aと撚り合わされて図示しない信号変換器に接続されている。8は磁極コア3a,3bとコイルボビン5の外側に取り付けられリターンコアであり磁場の帰還路として機能する。このような電磁流量計の先行技術としては下記の特許文献が知られている。   6a and 6b are signal lines connected to the tips of the electrodes 2a and 2b. In the illustrated example, the signal line 6b connected to the electrode 2b is located at the bottom (measurement tube) of the magnetic pole core 3b positioned on the lower side in the drawing. It passes through the through-hole 7 provided on the side of the electrode 2a, is drawn out to the electrode 2a side, is twisted with the signal line 6a connected to the tip of the electrode 2a, and is connected to a signal converter (not shown). A return core 8 is attached to the outside of the magnetic pole cores 3a and 3b and the coil bobbin 5, and functions as a return path for the magnetic field. The following patent documents are known as prior arts of such an electromagnetic flow meter.

特開2004−294176JP 2004-294176 A

上記特許文献では柱状の磁極コアとして、筒状のフェライト系ステンレス材を用い、筒の内部に電磁純鉄材を挿入することにより高周波励磁を可能とし高い磁束密度をはかっている。
しかしながら、上記従来例においては磁極コアに発生する渦電流で磁束密度の立ち上がりが遅くなり、磁気回路の周波数特性が良くないという問題があり、また、信号線6bが磁極コアを貫通しているため、信号線6bのみに鎖交面積分の微分ノイズが発生し、磁極コア内の微分ノイズの収束が遅くなるという問題があった。更に、信号サンプリング時にも微分ノイズが十分に収束しない場合は、信号線6bに微分ノイズが残ってしまう。信号線6aと信号線6bのノイズ量に差があると、差動増幅後もノイズ成分は残ってしまい、結果としてゼロシフト量が大きくなるという問題があった。
In the above-mentioned patent document, a cylindrical ferritic stainless steel material is used as the columnar magnetic pole core, and an electromagnetic pure iron material is inserted into the cylinder, thereby enabling high-frequency excitation and a high magnetic flux density.
However, in the above conventional example, the rise of the magnetic flux density is delayed by the eddy current generated in the magnetic pole core, the frequency characteristics of the magnetic circuit are not good, and the signal line 6b penetrates the magnetic pole core. The differential noise corresponding to the interlinkage area is generated only in the signal line 6b, and the convergence of the differential noise in the magnetic pole core is slow. Furthermore, if the differential noise does not sufficiently converge even during signal sampling, the differential noise remains on the signal line 6b. If there is a difference in the amount of noise between the signal line 6a and the signal line 6b, the noise component remains even after differential amplification, resulting in a problem that the zero shift amount increases.

本発明は上述の問題点を解決するためになされたもので、磁極コアに発生する渦電流の影響を小さくし、磁気回路の周波数特性を改善すると共に、信号線6bへの微分ノイズの影響を小さくし、ゼロシフト量を小さくした電磁流量計を実現することを目的とする。   The present invention has been made to solve the above-described problems. The influence of eddy current generated in the magnetic pole core is reduced, the frequency characteristic of the magnetic circuit is improved, and the influence of differential noise on the signal line 6b is reduced. The purpose is to realize an electromagnetic flow meter that is small and has a small zero shift amount.

本発明は上記問題点を解決するためになされたもので、請求項1の電磁流量計においては、
一対の流量検出用電極と、一端が測定管の外周に固定され前記電極の取付け方向とは90度回転した位置に対向して配置された一対の円柱状の磁極コアと、この磁極コアが挿入され前記磁極コアの長さより短く形成されたコイルボビンと、を有する磁気回路を備え、前記測定管内を流れる導電性流体に対して磁界を印加し、前記流量検出用電極に生じた起電力に基づいて発生した流量信号を出力する電磁流量計において、前記一対の円柱状の磁極コアの他端側の中心から前記測定管側に向かって測定管には達しない程度の深さに形成された穴と、前記一対の円柱状の磁極コアの一方であって前記コイルボビンの一端と前記磁極コアの他端を面一としたときに露出する前記磁極コアが固定された側であって、前記一対の流量検出用電極に接続された信号線の一方が他方の信号線側と同じ側に引き出せるように前記磁極コアの軸方向に対して直角方向に前記磁極コア及び穴を貫通する信号線貫通孔を設けたことを特徴とする。
The present invention has been made to solve the above problems, and in the electromagnetic flow meter according to claim 1,
A pair of flow rate detection electrodes, a pair of cylindrical magnetic pole cores , one end of which is fixed to the outer periphery of the measuring tube and opposed to a position rotated 90 degrees with respect to the mounting direction of the electrodes, and this magnetic pole core is inserted And a coil bobbin formed shorter than the length of the magnetic pole core, applying a magnetic field to the conductive fluid flowing in the measurement tube, and based on the electromotive force generated in the flow rate detection electrode In the electromagnetic flow meter that outputs the generated flow rate signal, a hole formed to a depth that does not reach the measurement tube from the center on the other end side of the pair of cylindrical magnetic cores toward the measurement tube side; , One of the pair of columnar magnetic pole cores, the side of the magnetic pole core that is exposed when one end of the coil bobbin and the other end of the magnetic pole core are flush with each other , and the pair of flow rates Connected to detection electrode A signal line through hole penetrating the magnetic pole core and the hole in a direction perpendicular to the axial direction of the magnetic pole core is provided so that one of the signal lines can be drawn to the same side as the other signal line side. .

請求項においては、請求項1に記載の電磁流量計において、
前記穴の入り口にねじを形成したことを特徴とする。
In claim 2 , in the electromagnetic flowmeter according to claim 1 ,
A screw is formed at the entrance of the hole.

請求項においては、請求項1または2に記載の電磁流量計において、
前記穴を設けた磁極コアにスリットを設けたことを特徴とする。
In claim 3 , in the electromagnetic flowmeter according to claim 1 or 2 ,
A slit is provided in the magnetic pole core provided with the hole.

請求項においては、請求項1乃至3に記載の電磁流量計において、
前記磁極コアの穴に軟磁性金属の粉体を混入した絶縁性のペースト又は軟磁性金属の粉体を混入した樹脂を充填したことを特徴とする。
In claim 4 , in the electromagnetic flowmeter according to claims 1 to 3,
The hole of the magnetic pole core is filled with an insulating paste mixed with a soft magnetic metal powder or a resin mixed with a soft magnetic metal powder.

請求項においては、請求項に記載の電磁流量計において、
前記軟磁性金属粉体を混入したペースト又は樹脂の充填に先立って絶縁性部材により前記磁極コアの穴の内面に絶縁層を設けたことを特徴とする。
In claim 5 , in the electromagnetic flowmeter according to claim 4 ,
Prior to filling of the paste or resin mixed with the soft magnetic metal powder, an insulating layer is provided on the inner surface of the hole of the magnetic pole core by an insulating member.

請求項6においては、請求項4又は5に記載の電磁流量計において、
前記磁極コアの途中に磁極コアの軸心に対して直角方向に軸心貫通孔を設けると共に前記軟磁性金属の粉体を混入するペースト又は樹脂として接着効果のあるものを使用したことを特徴とする。
In claim 6, in the electromagnetic flowmeter according to claim 4 or 5 ,
In the middle of the magnetic pole core, an axial center through hole is provided in a direction perpendicular to the axial center of the magnetic pole core, and a paste or resin mixed with the soft magnetic metal powder is used. To do.

以上説明したことから明らかなように請求項1の発明によれば次のような効果がある。
流量検出用電極に生じた起電力に基づいて発生した流量信号を出力する電磁流量計にお
いて、一対の円柱状の磁極コアの他端側の中心から前記測定管側に向かって測定管には達しない程度の深さに形成された穴と、前記一対の円柱状の磁極コアの一方であって前記コイルボビンの一端と前記磁極コアの他端を面一としたときに露出する前記磁極コアが固定された側であって、前記一対の流量検出用電極に接続された信号線の一方が他方の信号線側と同じ側に引き出せるように前記磁極コアの軸方向に対して直角方向に前記磁極コア及び穴を貫通する信号線貫通孔を設けたので、磁極コア中心部には渦電流が発生しない。
As is apparent from the above description, the invention of claim 1 has the following effects.
In an electromagnetic flowmeter that outputs a flow rate signal generated based on an electromotive force generated in a flow rate detection electrode, the measurement tube reaches the measurement tube side from the center of the other end of the pair of cylindrical magnetic cores. A hole formed to a depth not to be fixed, and the magnetic pole core that is one of the pair of columnar magnetic pole cores and is exposed when one end of the coil bobbin and the other end of the magnetic pole core are flush with each other is fixed The magnetic pole core in a direction perpendicular to the axial direction of the magnetic pole core so that one of the signal lines connected to the pair of flow rate detection electrodes can be drawn to the same side as the other signal line side. And since the signal line through-hole penetrating the hole is provided, no eddy current is generated in the central part of the magnetic pole core.

また渦電流の流れる経路が、磁極コア外周部に限定され、磁極コア内に信号線6bを通した時、信号線に接する磁極コアの面積が小さくなる。また渦電流の流れる経路が、磁極コア外周部に限定され、長い経路を取ることから、渦電流の収束が早くなり、磁気回路の周波数特性が向上する。   Further, the path through which the eddy current flows is limited to the outer periphery of the magnetic pole core, and when the signal line 6b is passed through the magnetic pole core, the area of the magnetic pole core in contact with the signal line is reduced. Further, the path through which the eddy current flows is limited to the outer periphery of the magnetic pole core and takes a long path, so the convergence of the eddy current is accelerated and the frequency characteristics of the magnetic circuit are improved.

また、信号線に接する磁極コアの面積が減少するため、信号線6bに発生する微分ノイズが減少する。その結果、信号線6aと信号線6bのノイズ量のアンバランスさが小さくなり、ゼロシフト量が小さくなる。   In addition, since the area of the magnetic pole core in contact with the signal line is reduced, the differential noise generated in the signal line 6b is reduced. As a result, the noise amount unbalance between the signal line 6a and the signal line 6b is reduced, and the zero shift amount is reduced.

請求項2の発明によれば、穴の入り口にねじを形成したので、リターンコアを磁極にねじ止めすることができる。
請求項3の発明によれば、穴を設けた磁極コアにスリットを設けたので、渦電流の収束
をさらに早め、磁気回路の周波数特性を改善することができる。
According to the invention of claim 2, since the screw is formed at the entrance of the hole, the return core can be screwed to the magnetic pole.
According to the invention of claim 3, since the slit is provided in the magnetic pole core provided with the hole, the convergence of the eddy current can be further accelerated, and the frequency characteristic of the magnetic circuit can be improved.

請求項4の発明によれば、磁極コアの穴に軟磁性金属の粉体を混入した絶縁性のペースト又は軟磁性金属の粉体を混入した樹脂を充填したので、磁極中心部の渦電流の収束が早くなり、磁場の立ち上がりへの影響が小さくなる。
また、ペースト又は樹脂は軟磁性金属の粉体が混入されているため、単に磁極の中心部に穴をあけた場合に比較して、中心磁束密度減少の影響を小さくでき、最大透磁率を高めることができる。
According to the invention of claim 4, since the insulating paste in which the soft magnetic metal powder is mixed or the resin in which the soft magnetic metal powder is mixed is filled in the hole of the magnetic pole core, Convergence is faster and the effect on the rise of the magnetic field is reduced.
Also, since the paste or resin is mixed with soft magnetic metal powder, the influence of the decrease in the center magnetic flux density can be reduced and the maximum magnetic permeability can be increased as compared with the case where a hole is simply made in the center of the magnetic pole. be able to.

請求項5の発明によれば、
前記軟磁性金属粉体を混入したペースト又は樹脂の充填に先立って絶縁性部材により前記磁極コアの穴の内面に絶縁層を設けたので、渦電流の収束をさらに早めることができる
According to the invention of claim 5 ,
Prior to filling with the paste or resin mixed with the soft magnetic metal powder, an insulating layer is provided on the inner surface of the hole of the magnetic pole core by an insulating member, so that convergence of eddy current can be further accelerated.

請求項6の発明によれば、
磁極コアの途中に磁極コアの軸心に対して直角方向に軸心貫通孔を設けると共に前記軟磁性金属の粉体を混入するペースト又は樹脂として接着効果のあるものを使用したのでねじを用いることなくシートコアを固定することができ、また、コイルボビンの固定部材として機能させることができる。
According to the invention of claim 6 ,
Use a screw because a paste or resin that has an axial through hole in the middle of the magnetic pole core in a direction perpendicular to the axis of the magnetic core and mixed with the soft magnetic metal powder is used. The seat core can be fixed without any problem, and can function as a fixing member for the coil bobbin.

図1は本発明の電磁流量計の一実施例を示す断面図である。図において、図6に示す従来例と同一要素には同一符号を付して重複する説明は省略する。
図において、1は測定管、2a,2bは電極、3は磁極コアである。磁極コア3はコイルボビン5に挿入されている。6a,6bは信号線、8は磁場の帰還路として機能するリターンコアで磁極コア3とコイル4の外側に取り付けられている。
FIG. 1 is a sectional view showing an embodiment of the electromagnetic flowmeter of the present invention. In the figure, the same elements as those of the conventional example shown in FIG.
In the figure, 1 is a measuring tube, 2a and 2b are electrodes, and 3 is a magnetic pole core. The magnetic pole core 3 is inserted into the coil bobbin 5. Reference numerals 6a and 6b denote signal lines, and reference numeral 8 denotes a return core that functions as a magnetic field return path, and is attached to the outside of the magnetic pole core 3 and the coil 4.

10a,10bは柱状の磁極コア3a,3bの中心に設けられた穴で、この穴は磁極コア3bの底部(測定管寄り)に設けられた貫通孔(信号線通し穴)7を突き抜けるとともに、測定管1には達しない程度の深さまで形成されており、この貫通穴7の周辺部の磁極コアの面積が小さくなるように形成されている。   10a and 10b are holes provided at the centers of the columnar magnetic pole cores 3a and 3b, and these holes penetrate through a through hole (signal line through hole) 7 provided at the bottom (near the measuring tube) of the magnetic pole core 3b. It is formed to a depth that does not reach the measurement tube 1, and is formed so that the area of the magnetic pole core around the through hole 7 is small.

発明者らは口径が2.5mm,5mm,10mmの測定管について実験を行った。
磁極コアの直径は口径にかかわらず同じ10mmで、長さは40mm程度。磁極コア3bに設けられた貫通孔7は磁極コア3bの端部から30mm程度の深さの位置の直径方向に形成されている。なお、口径が2.5mm,5mmの測定管の磁極コアにはφ4.2mmで深さ33mmの孔を形成し、口径10mmの測定管の磁極コア3a,3bにはφ5mmで深さ33mmの穴を形成して実験を行った。
The inventors conducted experiments on measuring tubes having diameters of 2.5 mm, 5 mm, and 10 mm.
The diameter of the magnetic core is the same 10 mm regardless of the diameter, and the length is about 40 mm. The through-hole 7 provided in the magnetic pole core 3b is formed in the diameter direction at a position about 30 mm deep from the end of the magnetic pole core 3b. In addition, a hole having a diameter of 2.5 mm and a depth of 33 mm is formed in a magnetic core of a measuring tube having a diameter of 2.5 mm and 5 mm, and a hole having a diameter of 5 mm and a depth of 33 mm is formed in the magnetic core 3a and 3b of the measuring pipe having a diameter of 10 mm. The experiment was conducted.

図2は上述の口径の測定管に対し穴10を設けない無対策の磁極コアと、穴10a,10bを設けた場合の比較例を示す実験結果である。




実験によれば、
インダクタンスのコーナー周波数は
口径2.5mmのものは無対策磁極コアでは195Hz
対策磁極コアでは 250Hz
口径5mmのものは無対策磁極コアでは 230Hz
対策磁極コアでは 310Hz
口径10mmのものは無対策磁極コアでは 260Hz
対策磁極コアでは 320Hz
FIG. 2 is an experimental result showing a comparative example in the case where a measureless magnetic core having no hole 10 and holes 10a and 10b are provided in the above-described measurement tube having a diameter.




According to the experiment
The corner frequency of the inductance is
The one with a diameter of 2.5mm is 195Hz for the non-countermeasure core
250Hz for magnetic pole core
230mm for 5mm diameter magnetic core
310Hz for magnetic pole core
The thing of 10mm in diameter is 260Hz in the magnetic pole core without countermeasures
320Hz for magnetic pole core

ゼロシフト量は
口径2.5mmのものは無対策磁極コアでは−6.76cm/s
対策磁極コアでは −1.07cm/s
口径5mmのものは無対策磁極コアでは −16.08cm/s
対策磁極コアでは −7.42cm/s
口径10mmのものは無対策磁極コアでは −10.12cm/s
対策磁極コアでは −1.81cm/s
Zero shift amount is
The diameter of 2.5mm is -6.76cm / s for the non-countermeasured magnetic core.
-1.07 cm / s for magnetic pole core
The one with a diameter of 5 mm is -16.08 cm / s for the countermeasureless magnetic core.
-7.42 cm / s for magnetic pole core
10mm diameter is -10.12cm / s for magnetic core without countermeasures
-1.81 cm / s for magnetic pole core

中心磁束密度は260mAの直流電流をコイルに流した場合
口径2.5mmのものは無対策磁極コアでは107.6ミリテスラ(mT)
対策磁極コアでは 95.4(mT)
口径5mmのものは無対策磁極コアでは 59.3(mT)
対策磁極コアでは 51.8(mT)
口径10mmのものは無対策磁極コアでは 32.4(mT)
対策磁極コアでは 29.8(mT)
The center magnetic flux density is 260 mA when direct current is passed through the coil.
The diameter of 2.5mm is 107.6milli-Tesla (mT) for the non-countermeasured magnetic core.
95.4 (mT) for magnetic pole core
59.3 (mT) for 5mm diameter core with no countermeasure magnetic core
51.8 (mT) for magnetic pole core
The diameter of 10 mm is 32.4 (mT) for the non-countermeasured magnetic core.
29.8 (mT) for magnetic pole core

となった。ここで、口径2.5mmのものに注目すると磁極コア内部をくり抜き、磁極コア内部を貫通する信号線に接する磁極コア材を減少させることによって、インダクタンスのコーナー周波数は無対策磁極コアでは195Hzであったものが対策後は250Hzとなり、30%程度向上させることができた。
また、ゼロシフト量は対策前は−6.76cm/sであったのが、対策後は
−1.07cm/sとなり、実施した場合ゼロシフト量が約1/5の大きさになった。
It became. Here, focusing on the 2.5 mm diameter, by cutting out the inside of the magnetic core and reducing the magnetic core material in contact with the signal line penetrating the inside of the magnetic core, the corner frequency of the inductance is 195 Hz in the non-magnetic pole core. After the measures were taken, the frequency became 250 Hz, which was improved by about 30%.
Further, the zero shift amount was −6.76 cm / s before the countermeasure, but became −1.07 cm / s after the countermeasure, and when implemented, the zero shift amount was about 1/5.

図3は口径2.5mmの電磁流量計において磁極コアに対策を施した(穴をあけたもの)と無対策(穴をあけないもの)の磁極コアで微分ノイズのピークの絶対値を比較した信号波形を示すものである。対策前は33.8mVであったが、対策後は32.0mVにテール分の収束が改善されていることがわかる。
図4は同じく口径10mmのものについて比較したもので、対策を施したものは微分ノイズのピーク値が25mVから17.4mVにテール分の収束が改善されていることがわかる。
Fig. 3 compares the absolute value of the peak of differential noise between a magnetic core with a 2.5mm caliber magnetic pole core with countermeasures (with holes) and no countermeasures (without holes). A signal waveform is shown. Although it was 33.8 mV before the countermeasure, it can be seen that the tail convergence is improved to 32.0 mV after the countermeasure.
FIG. 4 shows a comparison with a 10 mm aperture, and it can be seen that the tail of the peak of the differential noise is improved from 25 mV to 17.4 mV when the countermeasure is taken.

図5は磁極コアに開けた丸穴をメネジの下穴として利用して、ネジもしくはボルトを使用して、リターンコアと磁極コアを結合した例を示している。
なお、メネジは切らず、ピン等の圧入によってリターンコアと磁極コアを結合してもよい。
また、A−A断面図のように、丸穴に加えてスリットを入れることで、過電流の発生する部位を細分化し過電流を小さくする。その結果、渦電流の発生部位を細分化し過電流を小さくすることで渦電流の収束を更に早めて、磁気回路の周波数特性を改善することもできる。
FIG. 5 shows an example in which a return hole and a magnetic pole core are coupled using screws or bolts using a round hole opened in the magnetic pole core as a pilot hole for a female screw.
The return core and the magnetic pole core may be coupled by press-fitting a pin or the like without cutting the female screw.
Moreover, as shown in the A-A cross-sectional view, by adding a slit in addition to the round hole, the portion where the overcurrent is generated is subdivided to reduce the overcurrent. As a result, the frequency characteristics of the magnetic circuit can be improved by further accelerating the convergence of the eddy current by subdividing the eddy current generation site and reducing the overcurrent.

図6は図1で示した磁極コアの穴の中に軟磁性金属の粉体を混入した絶縁性ペースト又は絶縁性樹脂を注入した例を示す断面図である。この場合、軟磁性金属の混入量は必要とする中心磁束密度によって決定されるが、混入後もできるだけペースト又は樹脂の固有抵抗値が高くなるように調整する。   6 is a cross-sectional view showing an example in which an insulating paste or an insulating resin mixed with a soft magnetic metal powder is injected into the hole of the magnetic pole core shown in FIG. In this case, the mixing amount of the soft magnetic metal is determined by the required center magnetic flux density, but is adjusted so that the specific resistance value of the paste or resin is as high as possible even after mixing.

図6の構成によれば磁極コア中心部に渦電流の収束が早くなり、磁場の立ち上がりへの影響が小さくなる。また、大部分の渦電流の流れる経路が磁極外周部に限定され、長い経路を取ることから渦電流の収束が早くなり磁気回路の周波数特性を向上させることができる。   According to the configuration of FIG. 6, the convergence of the eddy current is accelerated in the central part of the magnetic pole core, and the influence on the rise of the magnetic field is reduced. Further, the path through which most of the eddy current flows is limited to the outer periphery of the magnetic pole, and since a long path is taken, the convergence of the eddy current is accelerated and the frequency characteristics of the magnetic circuit can be improved.

その結果、信号線6bに発生する微分ノイズが減少し、信号線6aと6bのノイズ量の不均衡が小さくなるのでゼロ点のシフト量を小さくすることができる。
更に、絶縁性ペースト又は絶縁性樹脂には軟磁性金属粉体が混入されているため磁極として機能する。その結果、単に穴をあけた場合に比較して中心磁束密度減少の影響を小さくでき最大透磁率を高めることができる。
As a result, the differential noise generated in the signal line 6b is reduced, and the noise amount imbalance between the signal lines 6a and 6b is reduced, so that the shift amount of the zero point can be reduced.
Furthermore, since soft magnetic metal powder is mixed in the insulating paste or the insulating resin, it functions as a magnetic pole. As a result, it is possible to reduce the influence of the decrease in the central magnetic flux density and increase the maximum magnetic permeability as compared with the case where the holes are simply drilled.

図7は他の実施例を示すもので、この例においては軟磁性金属の粉体を混入したペース
と又は樹脂を磁極コアの穴に注入する前に、絶縁性ワニスやシリコン樹脂などを注入し磁
極コア本体との間に絶縁層を作ったものである。このような構成によれば渦電流の収束を
更に高めることができる。
FIG. 7 shows another embodiment. In this example, an insulating varnish, silicon resin, or the like is injected before the soft magnetic metal powder is mixed in or before the resin is injected into the hole of the magnetic pole core. An insulating layer is formed between the magnetic pole core body and the magnetic pole core body. According to such a configuration, the convergence of eddy current can be further enhanced.

図8は更に他の実施例を示すもので、この例においては磁極コアに穴10を形成すると
共に穴の途中から直径方向に貫通孔14を形成したものである。このような構成として、
穴に注入する軟磁性金属の粉体を混入する樹脂として接着効果のあるものを使用してシー
トコア8を接着により固定し、合わせてコイルボビン5も固定するようにしたものである
。上述の構成によれば、シートコアの固定が簡単に行うことができ、また、コイルボビン
5の振動による悪影響をなくし測定値を安定化することができる。
FIG. 8 shows still another embodiment. In this example, the hole 10 is formed in the magnetic pole core and the through hole 14 is formed in the diameter direction from the middle of the hole. As such a configuration,
A resin having a bonding effect is used as a resin mixed with soft magnetic metal powder to be injected into the hole, and the sheet core 8 is fixed by adhesion, and the coil bobbin 5 is also fixed together. According to the above-described configuration, the seat core can be easily fixed, and the adverse effect due to the vibration of the coil bobbin 5 can be eliminated and the measurement value can be stabilized.

なお、以上の説明は、本発明の説明および例示を目的として特定の好適な実施例を示したに過ぎない。したがって本発明は、上記実施例に限定されることなく、その本質から逸脱しない範囲で更に多くの変更、変形を含むものである。   The above description merely shows a specific preferred embodiment for the purpose of explanation and illustration of the present invention. Therefore, the present invention is not limited to the above-described embodiments, and includes many changes and modifications without departing from the essence thereof.

本発明の実施形態の一例を示す電磁流量計の断面図である。It is sectional drawing of the electromagnetic flowmeter which shows an example of embodiment of this invention. 穴を設けない無対策の磁極コアと、穴を設けた場合の比較例を示す実験結果である。It is an experimental result which shows the comparative example at the time of providing a countermeasure magnetic pole core which does not provide a hole, and a hole. 磁極コアに対策を施したものと無対策の磁極コアで微分ノイズのピーク値を比較した信号波形を示すものである。The signal waveform which compared the peak value of a differential noise with what took the countermeasure to the magnetic pole core, and the magnetic core with no countermeasure is shown. 磁極コアに対策を施したものと無対策の磁極コアで微分ノイズのピーク値を比較した信号波形を示すものである。The signal waveform which compared the peak value of a differential noise with what took the countermeasure to the magnetic pole core, and the magnetic core with no countermeasure is shown. 他の実施例を示す電磁流量計の断面図である。It is sectional drawing of the electromagnetic flowmeter which shows another Example. 他の実施例を示す電磁流量計の断面図である。It is sectional drawing of the electromagnetic flowmeter which shows another Example. 他の実施例を示す電磁流量計の断面図である。It is sectional drawing of the electromagnetic flowmeter which shows another Example. 他の実施例を示す電磁流量計の断面図である。It is sectional drawing of the electromagnetic flowmeter which shows another Example. 電磁流量計の原理構成説明図である。It is a principle structure explanatory drawing of an electromagnetic flowmeter. 従来例を示す断面図である。It is sectional drawing which shows a prior art example.

符号の説明Explanation of symbols

1 測定管
2 電極
3 磁極コア
4 コイル
5 コイルボビン
6 信号線
7 貫通孔
8 シートコア(リターンコア)
10 穴
11 軟磁性金属粉体を混入したペースト又は樹脂
12 絶縁性部材
13 接着性効果部材
DESCRIPTION OF SYMBOLS 1 Measuring tube 2 Electrode 3 Magnetic pole core 4 Coil 5 Coil bobbin 6 Signal line 7 Through-hole 8 Sheet core (return core)
10 Hole 11 Paste or resin mixed with soft magnetic metal powder 12 Insulating member 13 Adhesive effect member

Claims (6)

一対の流量検出用電極と、一端が測定管の外周に固定され前記電極の取付け方向とは90度回転した位置に対向して配置された一対の円柱状の磁極コアと、この磁極コアが挿入され前記磁極コアの長さより短く形成されたコイルボビンと、を有する磁気回路を備え、前記測定管内を流れる導電性流体に対して磁界を印加し、前記流量検出用電極に生じた起電力に基づいて発生した流量信号を出力する電磁流量計において、前記一対の円柱状の磁極コアの他端側の中心から前記測定管側に向かって測定管には達しない程度の深さに形成された穴と、前記一対の円柱状の磁極コアの一方であって前記コイルボビンの一端と前記磁極コアの他端を面一としたときに露出する前記磁極コアが固定された側であって、前記一対の流量検出用電極に接続された信号線の一方が他方の信号線側と同じ側に引き出せるように前記磁極コアの軸方向に対して直角方向に前記磁極コア及び穴を貫通する信号線貫通孔を設けたことを特徴とする電磁流量計。 A pair of flow rate detection electrodes, a pair of cylindrical magnetic pole cores , one end of which is fixed to the outer periphery of the measuring tube and opposed to a position rotated 90 degrees with respect to the mounting direction of the electrodes, and this magnetic pole core is inserted And a coil bobbin formed shorter than the length of the magnetic pole core, applying a magnetic field to the conductive fluid flowing in the measurement tube, and based on the electromotive force generated in the flow rate detection electrode In the electromagnetic flow meter that outputs the generated flow rate signal, a hole formed to a depth that does not reach the measurement tube from the center on the other end side of the pair of cylindrical magnetic cores toward the measurement tube side; , One of the pair of columnar magnetic pole cores, the side of the magnetic pole core that is exposed when one end of the coil bobbin and the other end of the magnetic pole core are flush with each other , and the pair of flow rates Connected to detection electrode A signal line through hole penetrating the magnetic pole core and the hole in a direction perpendicular to the axial direction of the magnetic pole core is provided so that one of the signal lines can be drawn to the same side as the other signal line side. Electromagnetic flow meter. 前記穴の入り口にねじを形成したことを特徴とする請求項1に記載の電磁流量計。   The electromagnetic flowmeter according to claim 1, wherein a screw is formed at an entrance of the hole. 前記穴を設けた磁極コアにスリットを設けたことを特徴とする請求項1又は2に記載の電磁流量計。 Electromagnetic flow meter according to claim 1 or 2, characterized in that the slits in pole core provided with said hole. 前記磁極コアの穴に軟磁性金属の粉体を混入した絶縁性のペースト又は軟磁性金属の粉体を混入した樹脂を充填したことを特徴とする請求項1乃至3に記載の電磁流量計。   4. The electromagnetic flowmeter according to claim 1, wherein the magnetic core is filled with an insulating paste mixed with a soft magnetic metal powder or a resin mixed with a soft magnetic metal powder. 前記軟磁性金属粉体を混入したペースト又は樹脂の充填に先立って絶縁性部材により前記磁極コアに形成した穴の内面に絶縁層を設けたことを特徴とする請求項4に記載の電磁流量計。   5. The electromagnetic flowmeter according to claim 4, wherein an insulating layer is provided on an inner surface of a hole formed in the magnetic pole core by an insulating member prior to filling of the paste or resin mixed with the soft magnetic metal powder. . 前記磁極コアの途中に磁極コアの軸心に対して直角方向に軸心貫通孔を設けると共に前記軟磁性金属の粉体を混入するペースト又は樹脂として接着効果のあるものを使用したことを特徴とする請求項4又は5に記載の電磁流量計。 In the middle of the magnetic pole core, an axial center through hole is provided in a direction perpendicular to the axial center of the magnetic pole core, and a paste or resin mixed with the soft magnetic metal powder is used. The electromagnetic flowmeter according to claim 4 or 5 .
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