JPH0338705Y2 - - Google Patents

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Publication number
JPH0338705Y2
JPH0338705Y2 JP1982194776U JP19477682U JPH0338705Y2 JP H0338705 Y2 JPH0338705 Y2 JP H0338705Y2 JP 1982194776 U JP1982194776 U JP 1982194776U JP 19477682 U JP19477682 U JP 19477682U JP H0338705 Y2 JPH0338705 Y2 JP H0338705Y2
Authority
JP
Japan
Prior art keywords
conductor
conductors
current
magnetic sensor
groove
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
JP1982194776U
Other languages
Japanese (ja)
Other versions
JPS5997474U (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 JP19477682U priority Critical patent/JPS5997474U/en
Publication of JPS5997474U publication Critical patent/JPS5997474U/en
Application granted granted Critical
Publication of JPH0338705Y2 publication Critical patent/JPH0338705Y2/ja
Granted legal-status Critical Current

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Description

【考案の詳細な説明】 この考案は容器内に収納された導体の電流を測
定するようにした電流測定装置に関するものであ
る。
[Detailed Description of the Invention] This invention relates to a current measuring device that measures the current of a conductor housed in a container.

第1図及び第2図は従来の電流測定装置であ
る。図において、容器1,2,3内には絶縁ガス
が所定の圧力で充填され、高電圧が印加される導
体4,5,6を絶縁している。
1 and 2 show conventional current measuring devices. In the figure, containers 1, 2, and 3 are filled with insulating gas at a predetermined pressure to insulate conductors 4, 5, and 6 to which high voltage is applied.

このような構成においては、導体4,5,6を
流れる電流によつて発生する磁界が他相の容器
1,2,3内に入り、磁気センサー10,11,
12に影響を与え、磁気センサー10,11,1
2による電流測定精度を低下させるという欠点が
あつた。
In such a configuration, the magnetic field generated by the current flowing through the conductors 4, 5, 6 enters the containers 1, 2, 3 of the other phase, and the magnetic sensors 10, 11,
12, magnetic sensors 10, 11, 1
2 had the disadvantage of lowering the accuracy of current measurement.

この考案は上記欠点を解消するためになされた
もので、磁気センサーによる電流測定精度が良好
な電流測定装置を提供する。
This invention was made to eliminate the above-mentioned drawbacks, and provides a current measuring device with good current measurement accuracy using a magnetic sensor.

以下、図について説明する。第3図及び第4図
において、1,2,3は同一平面上にほぼ平行に
配置された3相の各相の円筒状の容器で、絶縁ガ
スが封入されている。4,5,6は各容器1,
2,3を同軸で貫通した各相の導体で、外周に環
状の溝4a,5a,6aが設けてある。そして、
導体4にU相、導体5にV相及び導体6にW相の
三相交流が流れている。7,8,9は各溝4a,
5a,6aに配置された円形状の鉄心で、各導体
4,5,6を横切る直線に対して各導体4,5,
6の中心を通るほぼ垂直な垂直線上に、それぞれ
空〓7a,8a,9aが形成されている。10,
11,12は空〓7a,8a,9aに配置された
磁気センサーで、自相の導体4,5,6の周方向
に磁界で作動するように構成されている。
The figures will be explained below. In FIGS. 3 and 4, numerals 1, 2, and 3 are cylindrical containers for each of the three phases arranged substantially parallel on the same plane and filled with insulating gas. 4, 5, 6 are each container 1,
2 and 3 coaxially pass through each phase, and annular grooves 4a, 5a, and 6a are provided on the outer periphery. and,
A three-phase alternating current flows through the conductor 4 in the U phase, the conductor 5 in the V phase, and the conductor 6 in the W phase. 7, 8, 9 are each groove 4a,
5a, 6a, each conductor 4, 5, 6 is connected to a straight line that crosses each conductor 4, 5, 6.
Sky spaces 7a, 8a, and 9a are formed on substantially perpendicular lines passing through the center of the space 6, respectively. 10,
Magnetic sensors 11 and 12 are arranged in the air 7a, 8a, and 9a, and are configured to operate by a magnetic field in the circumferential direction of the conductors 4, 5, and 6 of the self-phase.

鉄心7,8,9を設けることによつて、空〓7
a,8a,9aおける自相導体4,5,6の電流
による周方向の磁界は大きくなる。一方、他相の
導体4,5,6を流れる電流による磁界は鉄心
7,8,9を通り、空隙7a,8a,9aを通り
にくい。このようなことから、磁気センサー1
0,11,12による各導体4,5,6の電流検
出精度が向上する。
By providing the iron cores 7, 8, and 9, the air
The magnetic field in the circumferential direction due to the current in the self-phase conductors 4, 5, and 6 in a, 8a, and 9a increases. On the other hand, the magnetic field caused by the current flowing through the conductors 4, 5, and 6 of the other phases passes through the iron cores 7, 8, and 9, and hardly passes through the gaps 7a, 8a, and 9a. For this reason, magnetic sensor 1
The current detection accuracy of each conductor 4, 5, 6 by 0, 11, 12 is improved.

導体4,5,6を流れる電流による磁界は、他
相の鉄心7,8,9の各導体4,5,6を結ぶ線
上にある部分に大きな影響を与えることから、こ
の部分から90°離れた位置、すなわち、導体4,
5,6を通り各導体4,5,6間を結ぶ直線に対
してほぼ垂直な垂線上の位置に磁気センサー1
0,11,12を設け、他相の磁界の影響を小さ
くしている。
The magnetic field caused by the current flowing through the conductors 4, 5, and 6 has a large effect on the part of the iron cores 7, 8, and 9 of the other phases that are on the line connecting each conductor 4, 5, and 6, so position, i.e., conductor 4,
Magnetic sensor 1 is placed at a position on a perpendicular line passing through conductors 4, 6 and almost perpendicular to the straight line connecting between each conductor 4, 5, and 6.
0, 11, and 12 are provided to reduce the influence of magnetic fields of other phases.

また、鉄心7,8,9を溝4a,5a,6aに
埋め込むことによつて電界が集中するのを防いで
いる。
Further, by embedding the iron cores 7, 8, and 9 in the grooves 4a, 5a, and 6a, concentration of the electric field is prevented.

即ち、容器1,2,3は接地されて導体4,
5,6に高電圧が印加されていることから、導体
4,5.6の表面には(1)式の電界Eがかかる。
That is, the containers 1, 2, and 3 are grounded and the conductors 4,
Since a high voltage is applied to conductors 5 and 6, an electric field E of equation (1) is applied to the surfaces of conductors 4 and 5.6.

E=V/a・1/logb/a(V/m)……(1) ここで、Vは導体4,5,6に印加される電
圧、aは導体4,5,6の半径、bは容器1,
2,3の内径である。
E=V/a・1/logb/a (V/m)...(1) Here, V is the voltage applied to conductors 4, 5, and 6, a is the radius of conductors 4, 5, and 6, and b is container 1,
The inner diameter is 2 or 3.

上記(1)式は表面が滑らかな場合であつて、表面
に突起物があると電界が強くなることは知られて
いる。
Equation (1) above applies when the surface is smooth, and it is known that the electric field becomes stronger if there are protrusions on the surface.

例えば、一方が接地された平行平板の間隔がd
で平行平板のどちらかに半球状の突起物がある場
合、最大電界強度は(2)式で示されることが知られ
ている。
For example, the distance between parallel plates with one side grounded is d
It is known that when there is a hemispherical protrusion on either side of parallel plates, the maximum electric field strength is expressed by equation (2).

Emax=V/d×3 ……(2) このように平行平板に突起物があると、突起物
がない場合の3倍の電界の強さとなる。しかも上
記実施例の場合は同軸に配置されているので、電
界の上昇が3倍にもならないが、上記(1)式から算
出される値より大きくなる。
Emax=V/d×3...(2) If there is a protrusion on a parallel plate like this, the electric field will be three times stronger than when there is no protrusion. Moreover, in the case of the above embodiment, since they are arranged coaxially, the rise in the electric field does not increase three times, but it becomes larger than the value calculated from the above equation (1).

なお、上記実施例は各鉄心7,8,9の2個所
に間隙7a,8a,9aを設けたものについて説
明したが、1個所のみ間隙7a,8a,9aを設
けて電流検出器10,11,12を配置しても効
果がある。
In the above embodiment, the gaps 7a, 8a, 9a are provided at two locations in each of the iron cores 7, 8, 9. , 12 is also effective.

以上のようにこの考案によると、導体の外周に
設けた溝内に空隙が導体の中心を通る垂線上にく
るように鉄心を配置し、鉄心の空隙内に磁気セン
サーを配置したので、磁気センサーを作動させる
自相の電流による磁気を強くし、他相の電流によ
る磁界の影響を少なくでき、測定精度の向上が図
れる。
As described above, according to this invention, the iron core is placed in the groove provided on the outer periphery of the conductor so that the air gap is on a perpendicular line passing through the center of the conductor, and the magnetic sensor is placed within the air gap of the iron core, so the magnetic sensor It is possible to strengthen the magnetism caused by the current in the current phase that operates the current, reduce the influence of the magnetic field caused by the current in other phases, and improve measurement accuracy.

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

第1図は従来の電流測定装置の斜視図、第2図
は第1図の断面図、第3図はこの考案の一実施例
の断面図、第4図はこの考案の一実施例の要部の
断面図である。図において、1,2,3は容器、
4,5,6は導体、7,8,9は鉄心、7a,8
a,9aは間隙、10,11,12は磁気センサ
ーである。なお各図中同一符号は同一又は相当部
分を示す。
Fig. 1 is a perspective view of a conventional current measuring device, Fig. 2 is a sectional view of Fig. 1, Fig. 3 is a sectional view of an embodiment of this invention, and Fig. 4 is a summary of an embodiment of this invention. FIG. In the figure, 1, 2, 3 are containers,
4, 5, 6 are conductors, 7, 8, 9 are iron cores, 7a, 8
A and 9a are gaps, and 10, 11, and 12 are magnetic sensors. Note that the same reference numerals in each figure indicate the same or equivalent parts.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 導電性を有する筒状の容器を複数個ほぼ平行に
配置して上記容器内に上記各容器と同軸に導体を
配置し、上記各導体を横切る直線に対して上記各
導体の中心を通るほぼ垂直な垂直線上に上記各導
体の主電流を測定する磁気センサーを配置したも
のにおいて、上記導体の外周に環状の溝を設け
て、空〓を有する環状の鉄心の上記空〓が上記導
体の中心を通る垂線上にくるように上記鉄心を上
記溝内に配置し、上記磁気センサーを上記空〓内
に配置したことを特徴とする電流測定装置。
A plurality of conductive cylindrical containers are arranged approximately in parallel, and a conductor is arranged within the container coaxially with each of the containers, and a line passing through the center of each conductor is approximately perpendicular to a straight line that crosses each of the conductors. A magnetic sensor for measuring the main current of each conductor is arranged on a perpendicular line, and an annular groove is provided on the outer periphery of the conductor, so that the hollow of the annular iron core has a hollow that extends from the center of the conductor. A current measuring device characterized in that the iron core is disposed in the groove so as to be on a perpendicular line passing through the groove, and the magnetic sensor is disposed within the space.
JP19477682U 1982-12-20 1982-12-20 current measuring device Granted JPS5997474U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19477682U JPS5997474U (en) 1982-12-20 1982-12-20 current measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19477682U JPS5997474U (en) 1982-12-20 1982-12-20 current measuring device

Publications (2)

Publication Number Publication Date
JPS5997474U JPS5997474U (en) 1984-07-02
JPH0338705Y2 true JPH0338705Y2 (en) 1991-08-15

Family

ID=30418550

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19477682U Granted JPS5997474U (en) 1982-12-20 1982-12-20 current measuring device

Country Status (1)

Country Link
JP (1) JPS5997474U (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5499479A (en) * 1978-01-23 1979-08-06 Toshiba Corp Direct current measuring apparatus

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5499479A (en) * 1978-01-23 1979-08-06 Toshiba Corp Direct current measuring apparatus

Also Published As

Publication number Publication date
JPS5997474U (en) 1984-07-02

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