JPS6027864A - Magnetic field measurement for compressed gas insulated cable - Google Patents
Magnetic field measurement for compressed gas insulated cableInfo
- Publication number
- JPS6027864A JPS6027864A JP58136072A JP13607283A JPS6027864A JP S6027864 A JPS6027864 A JP S6027864A JP 58136072 A JP58136072 A JP 58136072A JP 13607283 A JP13607283 A JP 13607283A JP S6027864 A JPS6027864 A JP S6027864A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- sheath
- measuring
- phase
- bonding bars
- 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.)
- Pending
Links
Landscapes
- Measuring Magnetic Variables (AREA)
- Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
Abstract
Description
【発明の詳細な説明】
この発明はガス絶縁機器あるいは管′路気中ケーブルに
おける磁界測定方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring magnetic fields in gas-insulated equipment or pipes and aerial cables.
この発明t−実施する管路気中ケーブルは図に示すよう
に例えば人相、B相、C相の3相の導体1,2,8をシ
ース4.5.6内に通し、この各シースをシースボンド
パー7.8で一体に連結したものである。As shown in the figure, for example, conductors 1, 2, and 8 of three phases, ie, human phase, B phase, and C phase, are passed through a sheath 4, 5, and 6, and each of these sheaths is are connected together with a sheath bond par 7.8.
このような管路気中ケーブルにおいて、各相を電流が第
1図、第3図の矢印aのように流れると、ファラデーの
法則によυ矢印すのような右回9の磁界が生じる。In such a conduit air cable, when current flows through each phase as shown by arrow a in FIGS. 1 and 3, a clockwise magnetic field 9 as shown by arrow υ is generated according to Faraday's law.
このような磁界の強さは各相の導体1,2.8を流れる
電流の強さに比例するので、各磁界の強さを測定すれば
導体を流れる電流の強さが分ることになる。The strength of such a magnetic field is proportional to the strength of the current flowing through the conductors 1, 2.8 of each phase, so measuring the strength of each magnetic field will tell you the strength of the current flowing through the conductor. .
しかし、図に示しであるように導体1,2.8を電流が
流れると、シースポンドパー7.8にも矢印Cのように
磁界が生じ、これが各導体1,2゜8に生じる磁界に影
響を与える。However, when current flows through the conductors 1 and 2.8 as shown in the figure, a magnetic field is also generated in the sheath pump 7.8 as shown by arrow C, and this causes the magnetic field generated in each conductor 1 and 2. influence
従って独立した導体に電流を通じた場合の磁界測定方法
をそのま一シースボンドによりシースを連結した8相な
どの管路気中ケープJvK応用すると測定誤差を生じる
。Therefore, if the method for measuring magnetic fields when current is passed through independent conductors is applied to an 8-phase pipe air cape JvK in which sheaths are connected by sheath bonds, measurement errors will occur.
この発明は上記のようなシースポンドパーに生じる磁界
の影響を受けることなく各相に編じる磁界を正確に測定
する方法を提供することを目的とする。An object of the present invention is to provide a method for accurately measuring the magnetic field created in each phase without being affected by the magnetic field generated in the sheath pumper as described above.
以下、この発明の測定方法の一実施例を添付図面にもと
づいて説明する。An embodiment of the measuring method of the present invention will be described below with reference to the accompanying drawings.
図に示すように、各シース4,5.6にその中心線がシ
ースポントノ<−r、sの中心線と直角をなすように測
定用の孔9をそれぞれ設ける。As shown in the figure, each sheath 4, 5.6 is provided with a measuring hole 9 such that its center line is perpendicular to the center line of the sheath pontoon <-r, s.
ついで、この孔9にi界測定素子10を挿入するがこの
素子10としてフラデー効果を利用した素子を用い、こ
の素子10を第2図のようにシースポンドパー7の中心
線と直角となるように配置して素子10に流れる電流を
測定することにより磁界の強さが測定できる。Next, an i-field measuring element 10 is inserted into this hole 9. An element that utilizes the Fraday effect is used as this element 10, and this element 10 is inserted so that it is perpendicular to the center line of the sheath pounder 7 as shown in FIG. The strength of the magnetic field can be measured by measuring the current flowing through the element 10.
このように素子10をポンドパー7.8の中心線と直角
になるように配置することによって例えば図のようにA
相を測定する場合、人相の導体lに流れる電流により生
じる磁界を該素子10が垂直に受けるので、人相電流を
測定できるのであるが、このときポンドパー7に流れる
電流による磁界は矢印CのようにA相に装着した素子1
0と平行になっているから、この素子10はポンドパー
7に流れる電流の影響は受けない。By arranging the element 10 so as to be perpendicular to the center line of the pond par 7.8, for example, as shown in the figure,
When measuring the phase, the element 10 vertically receives the magnetic field generated by the current flowing through the conductor l of the human phase, so the human phase current can be measured. At this time, the magnetic field due to the current flowing through the pounder 7 is Element 1 installed on the A phase as shown below.
0, this element 10 is not affected by the current flowing through the pounder 7.
また、他相の導体2,8を流れる電流による磁界も人相
の素子10と平行になるため、影響は受けない。Further, the magnetic field caused by the current flowing through the conductors 2 and 8 of the other phases is also parallel to the human phase element 10, so that it is not affected.
結局人相に配置された素子10は人相に流れる電流のみ
を正確に測定できることになる。In the end, the element 10 placed on the human body can accurately measure only the current flowing through the human body.
また、A相以外のB相、C相の導体2.8に流れる電流
の測定も前記同様の測定方法によって正確に知ることが
できる。Further, the current flowing through the conductors 2.8 of the B phase and C phase other than the A phase can also be accurately determined by the same measuring method as described above.
なお第1図、第8図の実施例はシースポンドパー7の取
付は位置より若干ずれた位置に孔9を形成しであるが、
第1図の鎖線のように孔9をボンドパー7の取付位置と
同じ位置にしてもよく、また第2図のように人相の孔9
に対してC相やB相が180°の位置となった場合も同
様の効果が得られる。In addition, in the embodiments shown in FIGS. 1 and 8, the hole 9 is formed at a position slightly shifted from the mounting position of the sheath pounder 7.
The hole 9 may be located at the same position as the bond par 7, as shown by the chain line in FIG.
A similar effect can be obtained when the C phase or B phase is at a position of 180° with respect to the above.
この発明は上記のようにシースポンドが−と90″離れ
た場所を磁界測定場所としてここに磁界測定素子を配置
するととによって、シースパーや他の導体に流れる電流
による磁界が素子と平行になる。In the present invention, as described above, the magnetic field measuring element is arranged at a place where the sheath pond is -90'' away from the magnetic field measuring place, so that the magnetic field due to the current flowing through the sheath spar or other conductor becomes parallel to the element.
従ってこれらの磁界の影響を受けることなく被測定導体
を流れる電流が正確に測定できる効果がある。Therefore, there is an effect that the current flowing through the conductor to be measured can be accurately measured without being affected by these magnetic fields.
第1図はこの発明の実施状態を示す一部切欠平面図、第
2図は同上の横断正面図、第8図は一部切欠斜視図であ
る。
1.2.8・・・・・・導 体 4,5.6・・・・・
・シース9・・・・・・測定用の孔 10・・・・・・
磁界測定素子特許出願人 住友電気工業株式会社
代理人 弁理士和1)唱FIG. 1 is a partially cutaway plan view showing the state of implementation of the present invention, FIG. 2 is a cross-sectional front view of the same, and FIG. 8 is a partially cutaway perspective view. 1.2.8...Conductor 4,5.6...
・Sheath 9...Measurement hole 10...
Magnetic field measurement element patent applicant Sumitomo Electric Industries Co., Ltd. agent Patent attorney Kazu1) Sho
Claims (2)
り連結した管路気中ケーブルにおいて、シースポンドパ
ーと90°離れた場所を磁界測定場所としてここに磁界
測定素子を配置して磁界を測定することを特徴とする管
路気中ケーブルにおける磁界測定方法。(1) In a conduit aerial cable in which multiple sheaths covering a conductor are connected by a sheath pumper, the magnetic field is measured at a location 90° away from the sheath pumper, and a magnetic field measuring element is placed here to measure the magnetic field. A method for measuring a magnetic field in a conduit aerial cable.
素子を用いることを特徴とする特許請求の1範囲第1項
記載の管路気中ケーブルにおけ6磁界測定方法。(2) A method for measuring a magnetic field in a conduit aerial cable according to claim 1, characterized in that an element utilizing the Faraday effect is used as the a-field measuring element.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58136072A JPS6027864A (en) | 1983-07-25 | 1983-07-25 | Magnetic field measurement for compressed gas insulated cable |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58136072A JPS6027864A (en) | 1983-07-25 | 1983-07-25 | Magnetic field measurement for compressed gas insulated cable |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6027864A true JPS6027864A (en) | 1985-02-12 |
Family
ID=15166566
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP58136072A Pending JPS6027864A (en) | 1983-07-25 | 1983-07-25 | Magnetic field measurement for compressed gas insulated cable |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6027864A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6363974A (en) * | 1986-09-04 | 1988-03-22 | Honda Motor Co Ltd | Apparatus for detecting current in electric wire |
-
1983
- 1983-07-25 JP JP58136072A patent/JPS6027864A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6363974A (en) * | 1986-09-04 | 1988-03-22 | Honda Motor Co Ltd | Apparatus for detecting current in electric wire |
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