JPH0228408Y2 - - Google Patents

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Publication number
JPH0228408Y2
JPH0228408Y2 JP8461783U JP8461783U JPH0228408Y2 JP H0228408 Y2 JPH0228408 Y2 JP H0228408Y2 JP 8461783 U JP8461783 U JP 8461783U JP 8461783 U JP8461783 U JP 8461783U JP H0228408 Y2 JPH0228408 Y2 JP H0228408Y2
Authority
JP
Japan
Prior art keywords
conduit
transmitter
signal detection
detection electrode
force
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
JP8461783U
Other languages
Japanese (ja)
Other versions
JPS59189116U (en
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 filed Critical
Priority to JP8461783U priority Critical patent/JPS59189116U/en
Publication of JPS59189116U publication Critical patent/JPS59189116U/en
Application granted granted Critical
Publication of JPH0228408Y2 publication Critical patent/JPH0228408Y2/ja
Granted legal-status Critical Current

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Description

【考案の詳細な説明】 〈産業上の利用分野〉 本考案は電磁流量計発信器(以下、必要に応じ
て発信器と略称する)に関し、特に発信器の面間
距離を短かくしたときに生ずる問題点を除去する
ように改良したものである。
[Detailed description of the invention] <Industrial field of application> The present invention relates to an electromagnetic flowmeter transmitter (hereinafter abbreviated as a transmitter when necessary), and is particularly useful when the distance between the surfaces of the transmitter is shortened. This has been improved to eliminate the problems that arise.

〈従来技術〉 発信器の導管内部の任意の点に単位の電圧が与
えられたときに信号検出電極に寄与する割合を示
す指標としていわゆる重み関数がある。この重み
関数は信号検出電極を含む導管断面で最大値をと
り、これから導管の管軸方向に離れるにしたがつ
て急激に減少する傾向がある。そして信号検出電
極にほとんど寄与しなくなる管軸方向の長さは導
管の内径をDとすれば信号検出電極を含む導管断
面を中心として上下流にほぼ0.75Dである。した
がつて、従来の発信器の管軸方向の長さ、つまり
面間距離は1.5D程度のものとなつている。
<Prior Art> There is a so-called weighting function as an index that indicates the proportion of voltage that is contributed to the signal detection electrode when a unit voltage is applied to an arbitrary point inside the conduit of the transmitter. This weighting function has a maximum value at the cross section of the conduit that includes the signal detection electrode, and tends to decrease sharply as it moves away from this in the axial direction of the conduit. The length in the axial direction of the tube that hardly contributes to the signal detection electrode is approximately 0.75D upstream and downstream from the conduit cross section including the signal detection electrode, where D is the inner diameter of the conduit. Therefore, the length of the conventional transmitter in the tube axis direction, that is, the distance between the surfaces, is about 1.5D.

しかしながら、近年電磁流量計は経済性の追求
や軽量化を目ざして小形化される傾向となつてお
り、同時に高精度をも要求されている。小形化を
実現するためには発信器の面間距離Lを内径Dに
比べて短かくする必要がある。第1図は従来の発
信器の面間距離を単に短かくしたときの導管内の
電気力線の分布を示したものである。第1図では
励磁コイルなどの磁界発生手段は省略してある。
1は発信器の導管であり、その内面にはライニン
グ2が施されている。3a,3bは流体が流れる
ことにより生ずる信号電圧を検出する信号検出電
極である。4a,4bは発信器が挿入される相
手の配管であり、それぞれGで接地されている。
被測定流体6に磁界が与えられ矢印Fの方向に被
測定流体が流れると検出電極3a,3bに流量に
応じた信号電圧が発生し変換器(図示せず)で検
出される。この場合に被測定流体6中に生ずる電
気力線は検出電極3aから直接検出電極3bに向
かう電気力線群である7,7a1,7a2…7ao、7
b1,7b2…7boと、相手の配管4a,4bを経由
して信号検出電極3a,3bに流出入する電気力
線群である8a1,…8a4、8b1,8b4とがある。
発信器の面間距離Lが内径Dに比べて長い場合
には、電気力線群8a1,…8a4、8b1,8b4は存
在せず、電気力線群7,7a1,7a2…7ao、7
b1,7b2…7boのみである。しかし、面間距離L
が内径Dに比べて短かくなると相手配管4a,4
bを経由して信号検出電極3a,3bに流出入す
る電気力線群8a1,…8a4、8b1,8b4が生じ
る。面間距離Lが内径Dに比べて短かくなるほど
この電気力線の本数が増加する。電気力線群8
a1,…8a4、8b1,8b4は信号検出電極3a,3
bに流出入するので、これが変動するとスパン誤
差を生じる。具体的には相手配管4a,4bの材
質が異なつたり、相手配管の内面の導電性が変化
すると前記電気力線群8a1,…8a4、8b1,8b4
の短絡状態が変わるのでスパン変動を生じさせ
る。この短絡効果は被測定流体6の導電率が小さ
い程導電性の配管4a,4bの内面に短絡する電
気力線の数は多くなり、信号電圧は大きく減少し
誤差を増大させる。
However, in recent years, electromagnetic flowmeters have tended to be made smaller in pursuit of economic efficiency and weight reduction, and at the same time, high accuracy is also required. In order to achieve miniaturization, it is necessary to make the distance L between the surfaces of the transmitter shorter than the inner diameter D. FIG. 1 shows the distribution of electric lines of force within a conduit when the distance between the surfaces of a conventional transmitter is simply shortened. In FIG. 1, magnetic field generating means such as excitation coils are omitted.
Reference numeral 1 denotes a transmitter conduit, the inner surface of which is lined with a lining 2. 3a and 3b are signal detection electrodes that detect signal voltages generated by flowing fluid. 4a and 4b are pipes into which the transmitter 5 is inserted, and each is grounded at G.
When a magnetic field is applied to the fluid to be measured 6 and the fluid to be measured flows in the direction of arrow F, a signal voltage corresponding to the flow rate is generated at the detection electrodes 3a and 3b and detected by a converter (not shown). In this case, the electric lines of force generated in the fluid to be measured 6 are a group of electric lines of force 7, 7a 1 , 7a 2 . . . 7a o , 7 that go directly from the detection electrode 3a to the detection electrode 3b.
b 1 , 7b 2 . . . 7b o and 8a 1 , . be.
When the inter-plane distance L of the transmitter 5 is longer than the inner diameter D, the electric force line groups 8a 1 ,...8a 4 , 8b 1 , 8b 4 do not exist, and the electric force line groups 7, 7a 1 , 7a 2 ...7a o , 7
b 1 , 7b 2 ... only 7b o . However, the distance L between the surfaces
becomes shorter than the inner diameter D, the mating pipes 4a, 4
Groups of electric lines of force 8a 1 , . As the inter-plane distance L becomes shorter than the inner diameter D, the number of electric lines of force increases. Electric field lines group 8
a 1 ,...8a 4 , 8b 1 , 8b 4 are signal detection electrodes 3a, 3
Since it flows into and out of b, fluctuations in this will cause a span error. Specifically, if the materials of the mating pipes 4a and 4b are different or the conductivity of the inner surface of the mating pipes changes, the electric force line groups 8a 1 , ... 8a 4 , 8b 1 , 8b 4
The short-circuit condition changes, causing span fluctuations. This short-circuit effect is such that the lower the conductivity of the fluid 6 to be measured, the more lines of electric force short-circuit to the inner surfaces of the conductive pipes 4a and 4b, which greatly reduces the signal voltage and increases errors.

〈考案の目的〉 本考案は、前記の従来技術に鑑み、小形化に伴
つて生ずる相手配管の種類および被測定流体の導
電率の変化に起因するスパン誤差を除去すること
を目的とする。
<Purpose of the invention> In view of the above-mentioned prior art, the present invention aims to eliminate span errors caused by changes in the type of mating piping and changes in the conductivity of the fluid to be measured, which occur with downsizing.

〈考案の構成〉 この目的を達成する本考案の構成は、内面が絶
縁物でライニングされた導管と、この導管の軸と
垂直な方向に磁界を発生する手段と、前記導管の
軸と前記磁界とのそれぞれに垂直な方向に対向し
て導管に配設された信号検出電極とを有する電磁
流量計発信器において、前記信号検出電極を含む
前記導管の軸に直交する断面と前記電磁流量計発
信器の端面との間の前記ライニング内壁に環状の
導電体を配設したことを特徴とするものである。
<Structure of the invention> The structure of the invention that achieves this object includes a conduit whose inner surface is lined with an insulating material, a means for generating a magnetic field in a direction perpendicular to the axis of the conduit, and a means for generating a magnetic field between the axis of the conduit and the magnetic field. an electromagnetic flowmeter transmitter having a cross section perpendicular to the axis of the conduit including the signal detection electrode and a signal detection electrode disposed in a conduit so as to face each other in a direction perpendicular to the electromagnetic flowmeter transmitter; It is characterized in that an annular conductor is disposed on the inner wall of the lining between the end surface of the container and the inner wall of the lining.

〈実施例〉 以下、本考案の実施例について図面に基づき詳
細に説明する。なお、第1図と同一機能を有する
部分には同一の符号を付し、重複する説明を省略
する。
<Example> Hereinafter, an example of the present invention will be described in detail based on the drawings. Note that parts having the same functions as those in FIG. 1 are denoted by the same reference numerals, and redundant explanations will be omitted.

第2図は本考案の1実施例を示す発信器の断面
図である。発信器の導管部分およびこれと結合さ
れる配管部分のみ示す。第2図においては、信号
検出電極3a,3bを含む導管断面に対して左右
対称なライニング2の内面上の位置に環状の導電
体9a,9bが配設されている。この導電体9
a,9bは接地されておらず導管から絶縁されて
いる。この様な構成にすると、被測定流体の流れ
に起因して生じた電気力線の大部分は信号検出電
極3aから3bに向かう電気力線群10a1…10
ao,10b1…10boとなるが、一部の電気力線1
1a1,11b1は導電体9a,9bに入り込みこの
中を通つた後電気力線11a2,11b2として信号
検出電極3bに流入する。この導電体9a,9b
は接地されていないのでここに入り込む電流は導
管1または配管4a,4bに流出しない。したが
つて短絡効果による信号電圧の減少もない。換言
すれば、従来の発信器の面間距離を単に短かくし
た第1図において従来ならば相手配管へ流入した
電気力線群8a1,…8a4、8b1,8b4が本実施例
では導電体9a,9bで吸収されるので相手配管
4a,4bの影響を受けることがない。
FIG. 2 is a sectional view of a transmitter showing one embodiment of the present invention. Only the conduit section of the transmitter and the piping section connected thereto are shown. In FIG. 2, annular conductors 9a and 9b are arranged on the inner surface of the lining 2, which is symmetrical with respect to the cross section of the conduit including the signal detection electrodes 3a and 3b. This conductor 9
a, 9b are not grounded and are insulated from the conduit. With this configuration, most of the electric lines of force generated due to the flow of the fluid to be measured are directed from the signal detection electrodes 3a to 3b in the group of electric lines of force 10a 1 ...10
a o , 10b 1 ...10b o , but some electric lines of force 1
1a 1 and 11b 1 enter the conductors 9a and 9b, pass through them, and then flow into the signal detection electrode 3b as electric lines of force 11a 2 and 11b 2 . These conductors 9a, 9b
Since this is not grounded, the current that enters here does not flow into the conduit 1 or the pipes 4a and 4b. Therefore, there is no reduction in signal voltage due to short circuit effects. In other words, in FIG. 1, where the distance between the surfaces of the conventional transmitter is simply shortened, the electric force line groups 8a 1 , ... 8a 4 , 8b 1 , 8b 4 that would have conventionally flowed into the mating pipes are changed in this embodiment. Since it is absorbed by the conductors 9a and 9b, it is not affected by the mating pipes 4a and 4b.

第2図の実施例では信号検出電極を含む導管断
面と発信器の端面との間に1つの導電体のリング
を装着した例を示したが、2個以上の導電体のリ
ングを配設しても良い。
In the embodiment shown in Fig. 2, one conductor ring is installed between the conduit cross section including the signal detection electrode and the end face of the transmitter, but two or more conductor rings may be installed. It's okay.

また、第2図の導電体は金属体に限らず電気的
に導電性があるものであれば良い。例えば、絶縁
ライニングの一部に導電性物質を混合し、環状部
分のみを導電性プラスチツクとしても同等の効果
がある。
Further, the conductor shown in FIG. 2 is not limited to a metal body, and may be any electrically conductive body. For example, the same effect can be obtained by mixing a conductive substance into a part of the insulating lining and making only the annular part a conductive plastic.

〈考案の効果〉 以上、実施例とともに具体的に記載したように
本考案によれば、絶縁ライニングの内面に単に非
接地の円環状の導電体を配設する簡単な構成で相
手配管による短絡効果を受けることの少ない短面
間の発信器が安価に得られる効果がある。
<Effects of the Invention> As described above in detail along with the embodiments, according to the present invention, the short circuit effect caused by the mating piping can be reduced by simply arranging a non-grounded annular conductor on the inner surface of the insulating lining. This has the effect of making it possible to obtain a transmitter between short surfaces at a low cost, which is less susceptible to radiation.

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

第1図は従来の発信器の実施例を示す断面図、
第2図は本考案の実施例を示す断面図である。 1……導管、2……ライニング、3a,3b…
…信号検出電極、4a,4b……配管、……発
信器、7,7a1…7ao、7b1…7bo……電気力
線、8a1,…8a4、8b1,8b4……電気力線、9
a,9b……導電体、10,10a1…10ao、1
0b1…10bo……電気力線、11a1,11a2,1
1b1,11b2……電気力線。
FIG. 1 is a sectional view showing an example of a conventional transmitter;
FIG. 2 is a sectional view showing an embodiment of the present invention. 1... Conduit, 2... Lining, 3a, 3b...
... Signal detection electrode, 4a, 4b ... Piping, 5 ... Transmitter, 7, 7a 1 ... 7a o , 7b 1 ... 7b o ... Line of electric force, 8a 1 , ... 8a 4 , 8b 1 , 8b 4 ... …Electric lines of force, 9
a, 9b...conductor, 10,10a 1 ...10a o , 1
0b 1 ...10b o ...Electric field lines, 11a 1 , 11a 2 , 1
1b 1 , 11b 2 ... Lines of electric force.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 内面が絶縁物でライニングされた導管と、この
導管の軸と垂直な方向に磁界を発生する手段と、
前記導管の軸と前記磁界とのそれぞれに垂直な方
向に対向して導管に配設された信号検出電極とを
有する電磁流量計発信器において、前記信号検出
電極を含む前記導管の軸に直交する断面と前記電
磁流量計発信器の端面との間の前記ライニング内
壁に環状の導電体を配設したことを特徴とする電
磁流量計発信器。
a conduit whose inner surface is lined with an insulating material, and means for generating a magnetic field in a direction perpendicular to the axis of the conduit;
In an electromagnetic flowmeter transmitter having a signal detection electrode disposed in a conduit facing each other in a direction perpendicular to the axis of the conduit and the magnetic field, the signal detection electrode is perpendicular to the axis of the conduit including the signal detection electrode. An electromagnetic flowmeter transmitter, characterized in that an annular conductor is disposed on the inner wall of the lining between the cross section and the end face of the electromagnetic flowmeter transmitter.
JP8461783U 1983-06-03 1983-06-03 electromagnetic flowmeter transmitter Granted JPS59189116U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8461783U JPS59189116U (en) 1983-06-03 1983-06-03 electromagnetic flowmeter transmitter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8461783U JPS59189116U (en) 1983-06-03 1983-06-03 electromagnetic flowmeter transmitter

Publications (2)

Publication Number Publication Date
JPS59189116U JPS59189116U (en) 1984-12-15
JPH0228408Y2 true JPH0228408Y2 (en) 1990-07-31

Family

ID=30214577

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8461783U Granted JPS59189116U (en) 1983-06-03 1983-06-03 electromagnetic flowmeter transmitter

Country Status (1)

Country Link
JP (1) JPS59189116U (en)

Also Published As

Publication number Publication date
JPS59189116U (en) 1984-12-15

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