JPH0222700Y2 - - Google Patents
Info
- Publication number
- JPH0222700Y2 JPH0222700Y2 JP17701982U JP17701982U JPH0222700Y2 JP H0222700 Y2 JPH0222700 Y2 JP H0222700Y2 JP 17701982 U JP17701982 U JP 17701982U JP 17701982 U JP17701982 U JP 17701982U JP H0222700 Y2 JPH0222700 Y2 JP H0222700Y2
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- electrical resistance
- resistance value
- current
- containers
- 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
Links
- 239000004020 conductor Substances 0.000 claims description 15
- 238000005259 measurement Methods 0.000 description 3
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 230000000149 penetrating effect Effects 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
Landscapes
- Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
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図に示す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。他相の導体4,
5,6を流れる電流によつて発生する磁界が、容
器1,2,3内に入り、磁気センサー7,8,9
に影響を与え、磁気センサー7,8,9による導
体4,5,6を流れる電流の測定精度が低下する
という欠点があつた。 This is a conventional current measuring device shown in FIGS. 1 and 2. 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. Conductor 4 of other phase,
The magnetic field generated by the current flowing through the containers 1, 2, 3 enters the containers 1, 2, 3 and the magnetic sensors 7, 8, 9
This has the disadvantage that the measurement accuracy of the current flowing through the conductors 4, 5, 6 by the magnetic sensors 7, 8, 9 is reduced.
この考案は上記欠点を解消するためになされた
もので、円筒状の第1〜第3の筒体を順次同一軸
線上で直列になるように連結して容器を構成し、
容器を貫通した導体を配置し、第2の筒体内に導
体と所定の距離をあけて磁気センサーを配置し、
第2の筒体の電気抵抗値を第1及び第3の筒体の
電気抵抗値よりも小さくなるように構成すること
によつて、電気測定精度を向上させた電流測定装
置を提供する。 This invention was made in order to eliminate the above-mentioned drawbacks, and a container is constructed by sequentially connecting first to third cylindrical bodies in series on the same axis.
A conductor is placed through the container, and a magnetic sensor is placed within the second cylinder at a predetermined distance from the conductor.
A current measuring device is provided in which electrical measurement accuracy is improved by configuring the electrical resistance value of the second cylindrical body to be smaller than the electrical resistance values of the first and third cylindrical bodies.
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はほぼ平行に配置された第
1〜第3の容器で、順次同一軸線上で直列になる
ように連結された断面形状が等しい円筒状の第1
の筒体1a,2a,3aと第2の筒体1b,2
b,3bと第3の筒体1c,2c,3cとによつ
て構成されている。第2の筒体1b,2b,3b
は第1の筒体1a,2b,3b及び第3の筒体1
c,2c,3cよりも電気抵抗が小さくなるよう
に構成されている。例えば、第1の筒体1a,2
a,3aと第3の箇体1c,2c,3cとをステ
ンレスやアルミニユームで構成した場合は、第2
の筒体1b,2b,3bを銅で構成する。4,
5,6は容器1,2,3を貫通した導体、7,
8,9は容器1,2,3の周方向の磁界によつて
作動するように、第2の箇体1b,2b,3b内
に導体4,5,6から所定の距離をあけて配置さ
れた磁気センサーで、サーチコイル、ホール素
子、磁気光学センサーなどで構成されている。磁
気センサー7,8,9は他相の導体4,5,6を
流れる電流の影響を受けにくくするために、導体
4,5,6から各導体4,5,6を含む平面に対
して直角方向に配置されている。 The figures will be explained below. In FIGS. 3 and 4, 1, 2, and 3 are first to third containers arranged approximately parallel to each other, which are cylindrical containers with the same cross-sectional shape and connected in series on the same axis. 1st
cylinders 1a, 2a, 3a and second cylinders 1b, 2
b, 3b and third cylindrical bodies 1c, 2c, 3c. Second cylindrical body 1b, 2b, 3b
are the first cylindrical bodies 1a, 2b, 3b and the third cylindrical body 1
It is constructed so that the electrical resistance is smaller than that of c, 2c, and 3c. For example, the first cylindrical bodies 1a, 2
When a, 3a and the third bodies 1c, 2c, 3c are made of stainless steel or aluminum, the second
The cylindrical bodies 1b, 2b, and 3b are made of copper. 4,
5 and 6 are conductors that penetrated the containers 1, 2, and 3, 7,
8 and 9 are arranged at a predetermined distance from the conductors 4, 5 and 6 in the second bodies 1b, 2b and 3b so as to be operated by the magnetic field in the circumferential direction of the containers 1, 2 and 3. It is a magnetic sensor that consists of a search coil, a Hall element, a magneto-optical sensor, etc. The magnetic sensors 7, 8, 9 are arranged at right angles from the conductors 4, 5, 6 to the plane containing each conductor 4, 5, 6 in order to be less susceptible to the influence of the current flowing through the conductors 4, 5, 6 of other phases. placed in the direction.
第2の箇体1b,2b,3bは第1の筒体1
a,2a,3a及び第3の筒体1c,2c,3c
よりも電気抵抗値が小さくなつている。第2の筒
体1b,2b,3bに加わる他相の磁界により、
第2の筒体1b,2b,3b内にはそれを打ち消
すための誘導電流が流れる。第2の筒体1b,2
b,3bの電気抵抗値が小さいために、誘導電流
値が大きく、壁面を貫通して第2の筒体1b,2
b,3b内に漏洩する他相の磁界は、第1の筒体
1a,2a,3a及び第3の筒体1c,2c,3
c内に漏洩する他相の磁界より少ない。このた
め、磁気センサー7,8,9による他相の磁界の
影響が極めてなくなり、磁気センサー7,8,9
による電流測定精度が向上する。 The second bodies 1b, 2b, 3b are the first cylindrical body 1
a, 2a, 3a and third cylinder 1c, 2c, 3c
The electrical resistance value is smaller than that of . Due to the magnetic field of other phases applied to the second cylinders 1b, 2b, 3b,
An induced current flows in the second cylindrical bodies 1b, 2b, 3b to cancel the current. Second cylindrical body 1b, 2
Since the electric resistance value of cylindrical bodies 1b and 3b is small, the induced current value is large, penetrating the wall surface and flowing into the second cylindrical bodies 1b and 2.
The other phase magnetic fields leaking into the first cylinders 1a, 2a, 3a and the third cylinders 1c, 2c, 3b
The amount of magnetic field leaking into c is smaller than that of other phases. Therefore, the influence of magnetic fields of other phases by the magnetic sensors 7, 8, and 9 is extremely reduced, and the magnetic sensors 7, 8, and 9
Improves current measurement accuracy.
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
の斜視図、第4図は第3図の断面図である。図
中、1,2,3は容器、1a,2a,3aは第1
の筒体、1b,2b,3bは第2の筒体、1c,
2c,3cは第3の筒体、4,5,6は導体であ
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 perspective view of an embodiment of this invention, and Fig. 4 is a sectional view of Fig. 3. . In the figure, 1, 2, 3 are containers, 1a, 2a, 3a are first
1b, 2b, 3b are the second cylinders, 1c,
2c and 3c are third cylindrical bodies, and 4, 5, and 6 are conductors. Note that the same reference numerals in each figure indicate the same or equivalent parts.
Claims (1)
直列になるように連結して容器を構成し、上記容
器を複数個ほぼ平行に配置して上記各容器内に導
体を配置し、上記第2の筒体内に上記導体と所定
の距離をあけて上記導体の電流を測定する磁気セ
ンサーを配置し、上記第2の筒体の電気抵抗値を
上記第1及び上記第3の筒体の電気抵抗値より小
さくなるように構成したことを特徴とする電流測
定装置。 A container is constructed by sequentially connecting first to third cylindrical bodies in series on the same axis, a plurality of the containers are arranged substantially in parallel, and a conductor is arranged in each container. , a magnetic sensor for measuring the current of the conductor is disposed within the second cylinder at a predetermined distance from the conductor, and the electrical resistance value of the second cylinder is measured between the first and third cylinders. A current measuring device characterized in that the current measuring device is configured so that the electrical resistance value is smaller than the electrical resistance value of the body.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17701982U JPS5980760U (en) | 1982-11-20 | 1982-11-20 | current measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17701982U JPS5980760U (en) | 1982-11-20 | 1982-11-20 | current measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5980760U JPS5980760U (en) | 1984-05-31 |
| JPH0222700Y2 true JPH0222700Y2 (en) | 1990-06-19 |
Family
ID=30384692
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17701982U Granted JPS5980760U (en) | 1982-11-20 | 1982-11-20 | current measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5980760U (en) |
-
1982
- 1982-11-20 JP JP17701982U patent/JPS5980760U/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5980760U (en) | 1984-05-31 |
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