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JPH07104736B2 - DC bias magnetism detection method for transformer - Google Patents
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JPH07104736B2 - DC bias magnetism detection method for transformer - Google Patents

DC bias magnetism detection method for transformer

Info

Publication number
JPH07104736B2
JPH07104736B2 JP1004373A JP437389A JPH07104736B2 JP H07104736 B2 JPH07104736 B2 JP H07104736B2 JP 1004373 A JP1004373 A JP 1004373A JP 437389 A JP437389 A JP 437389A JP H07104736 B2 JPH07104736 B2 JP H07104736B2
Authority
JP
Japan
Prior art keywords
transformer
bias
search coil
magnetic
peak value
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 - Lifetime
Application number
JP1004373A
Other languages
Japanese (ja)
Other versions
JPH02183816A (en
Inventor
賢次 桐畑
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP1004373A priority Critical patent/JPH07104736B2/en
Publication of JPH02183816A publication Critical patent/JPH02183816A/en
Publication of JPH07104736B2 publication Critical patent/JPH07104736B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Testing Electric Properties And Detecting Electric Faults (AREA)
  • Housings And Mounting Of Transformers (AREA)
  • Control Of Electrical Variables (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は変圧器の直流偏磁を検出する方法に関するも
のである。
The present invention relates to a method for detecting DC bias magnetism in a transformer.

〔従来の技術〕 例えば、トランジスタを用いたインバータでは、インバ
ータ回路の各アームの電圧降下のばらつきやトランジス
タの導通期間のばらつきなどにより、出力交流電圧に直
流成分が含まれる。この直流成分によってインバータの
主回路の出力に接続される負荷の変圧器が直流偏磁を生
じて鉄損、励磁電流、騒音が増大するなど特性の悪化を
来すので、直流偏磁は防止しなければならない。
[Prior Art] For example, in an inverter using a transistor, a DC component is included in an output AC voltage due to variations in voltage drop of each arm of an inverter circuit, variations in conduction period of a transistor, and the like. Due to this DC component, the transformer of the load connected to the output of the main circuit of the inverter causes DC bias magnetization, which causes deterioration of characteristics such as increase in iron loss, exciting current, and noise. There must be.

従来、この種の変圧器の直流偏磁を検出する方法として
は、例えば、特願昭62−28353号のようにインバータの
主回路に並列に可飽和リアクトルを接続し、可飽和リア
クトルによって電流を検出する電流検出手段とこの電流
検出手段によって検出されたリアクトルの電流極性をフ
ォトカプラによって判別する極性判別手段と用いるよう
な方法がある。
Conventionally, as a method for detecting the DC bias magnetism of this type of transformer, for example, as in Japanese Patent Application No. 62-28353, a saturable reactor is connected in parallel to the main circuit of an inverter, and a current is supplied by the saturable reactor. There is a method of using the current detecting means for detecting and the polarity determining means for determining the current polarity of the reactor detected by the current detecting means by a photo coupler.

〔発明が解決しようとする課題〕 しかしながら、上記のような従来の変圧器の直流偏磁検
出方法では、可飽和リアクトルという別の装置を必要と
するので、設置スペースを余計に必要とし、又、可飽和
リアクトルそのものが損失や騒音を発生する、あるい
は、運転中には可飽和リアクトルの保守が難しいなどの
問題点があった。
[Problems to be Solved by the Invention] However, in the conventional DC bias magnetic field detection method for a transformer as described above, since another device called a saturable reactor is required, an extra installation space is required, and There are problems that the saturable reactor itself causes loss and noise, or that the saturable reactor is difficult to maintain during operation.

この発明は上記のような問題点を解決するためになされ
たもので、余計なスペースを必要とせず、又、損失及び
騒音が発生することのない変圧器の直流偏磁検出方法を
得ることを目的とする。
The present invention has been made to solve the above problems, and an object of the present invention is to provide a method for detecting a DC bias magnetic field in a transformer that does not require extra space and does not cause loss or noise. To aim.

〔課題を解決するための手段〕[Means for Solving the Problems]

この発明に係る変圧器の直流偏磁検出方法は、変圧器の
鉄心が直流偏磁を生じると鉄心の磁化力が正負非対称に
なることに着目し、鉄心で構成される磁気回路の近傍に
近接したタンクの高抵抗非磁性部分の外面にサーチコイ
ルを設けて鉄心の磁化力をタンク外から直接監視して変
圧器の直流偏磁を検出するようにしたものである。
The direct current bias magnetic detection method for a transformer according to the present invention focuses on the fact that the magnetizing force of the iron core becomes positive and negative asymmetric when the direct current bias of the iron core of the transformer is generated, and the proximity of the magnetic circuit composed of the iron core is considered. A search coil is provided on the outer surface of the high resistance non-magnetic portion of the tank to detect the DC bias of the transformer by directly monitoring the magnetizing force of the iron core from outside the tank.

〔作用〕[Action]

この発明においては、サーチコイルの出力電圧を積分し
た波形の正・負ピーク値の大小を比較することにより鉄
心の磁化力の変化を検出し、直流偏磁の有無を判別す
る。
In the present invention, the change in the magnetizing force of the iron core is detected by comparing the magnitudes of the positive and negative peak values of the waveform obtained by integrating the output voltage of the search coil, and the presence or absence of DC bias magnetization is determined.

〔実施例〕〔Example〕

以下、この発明の一実施例を図について説明する。第1
図はこの発明の一実施例を説明するための変圧器を示す
水平断面図であり、ここでは外鉄形の変圧器を例にとっ
ている。第2図(a)(b)は第1図の変圧器を正面及
び側面からみた場合の構成図であり、第1図は第2図の
A−A′断面を示している。第3図はこの発明の一実施
例に用いられる直流偏磁検出回路を示すブロック図であ
る。第4図(a)(b)及び第5図(a)(b)は第3
図の直流偏磁検出回路で得られる磁界Hを磁束φと共に
示す特性図であり、第4図は直流偏磁が生じていない場
合、第5図は直流偏磁が生じている場合を示している。
An embodiment of the present invention will be described below with reference to the drawings. First
FIG. 1 is a horizontal sectional view showing a transformer for explaining an embodiment of the present invention, and here, an outer iron type transformer is taken as an example. 2 (a) and 2 (b) are configuration diagrams of the transformer of FIG. 1 when viewed from the front and side surfaces, and FIG. 1 shows a cross section taken along the line AA ′ of FIG. FIG. 3 is a block diagram showing a DC bias magnetic detection circuit used in an embodiment of the present invention. 4 (a) (b) and 5 (a) (b) are the third
FIG. 4 is a characteristic diagram showing a magnetic field H obtained by the DC bias magnetic detection circuit in the figure together with a magnetic flux φ. FIG. 4 shows a case where DC bias is not occurring, and FIG. 5 is a case where DC bias is occurring. There is.

第1図において、1−1、1−2は高圧コイル2および
低圧コイル3が巻かれている変圧器の鉄心、4は変圧鉄
心1−1、1−2に近接したタンク5の高抵抗非磁性部
分15(例えばステンレス製)の外面に設けられているサ
ーチコイルであり、サーチコイル取付箱8およびカバー
9内に収納されており、タンク5内の変圧器鉄1−1、
1−2から漏れる磁束の一部はタンクの高抵抗非磁性部
分15を通過しタンク5の外面に設置したサーチコイル4
に鎖交する。サーチコイル4には出力端子7が設けら
れ、サーチコイル取付箱8から引き出されている。ま
た、第1図に示されているiL,φ,Hなる記号は、それぞ
れに、この変圧器が低圧側からの無負荷励磁状態にある
ときの励磁電流,磁束,磁界(鉄心の磁化力に対応す
る)を示している。
In FIG. 1, 1-1 and 1-2 are iron cores of a transformer around which a high voltage coil 2 and a low voltage coil 3 are wound, and 4 is a high resistance non-contact of a tank 5 close to the transformer iron cores 1-1 and 1-2. A search coil provided on the outer surface of the magnetic part 15 (for example, made of stainless steel), which is housed in the search coil mounting box 8 and the cover 9, and is the transformer iron 1-1 in the tank 5.
A part of the magnetic flux leaking from 1-2 passes through the high resistance non-magnetic portion 15 of the tank and is mounted on the outer surface of the tank 5 in the search coil 4
Link to. An output terminal 7 is provided on the search coil 4 and is drawn out from the search coil mounting box 8. The symbols i L , φ, and H shown in Fig. 1 respectively indicate the exciting current, magnetic flux, and magnetic field (magnetizing force of the iron core) when this transformer is in the unloaded excitation state from the low voltage side. (Corresponding to).

第2図において、タンク5は鉄1−1,1−2、高圧コイ
ル2及び低圧コイル3を収納しており、変圧器を構成し
ている。高圧コイル2にはプッシング6−1及び6−2
が接続され、タンク5との絶縁を確保している。
In FIG. 2, a tank 5 accommodates irons 1-1 and 1-2, a high-voltage coil 2 and a low-voltage coil 3, and constitutes a transformer. The high voltage coil 2 has pushers 6-1 and 6-2.
Are connected to secure insulation from the tank 5.

第3図において、10は第1図、第2図に示された変圧器
を示しており、該変圧器10の高圧コイル2にはインバー
タ11が接続されている。
In FIG. 3, reference numeral 10 denotes the transformer shown in FIGS. 1 and 2, and an inverter 11 is connected to the high voltage coil 2 of the transformer 10.

サーチコイル4の出力端子から得られる出力電圧Eは積
分器12により積分され、積分された出力電圧EHは正側ピ
ーク値検出器13−1及び負側ピーク値検出器13−2に入
力される。
The output voltage E obtained from the output terminal of the search coil 4 is integrated by the integrator 12, and the integrated output voltage E H is input to the positive side peak value detector 13-1 and the negative side peak value detector 13-2. It

各ピーク値検出器13−1及び13−2により検出された正
側ピーク値H+P及び負側ピーク値H-Pは比較器14に入力さ
れ、この比較器14からは、 ΔH=H+P−H-P で与えられるピーク差ΔHが出力される。
The positive side peak value H + P and the negative side peak value H- P detected by the respective peak value detectors 13-1 and 13-2 are input to the comparator 14, and from this comparator 14, ΔH = H + The peak difference ΔH given by P− H− P is output.

次に、第4図及び第5図の特性波形図を参照しながら、
正側ピーク値H+P及び負側ピーク値H-Pの大小を比較して
直流偏磁を検出するこの発明の一実施例について説明す
る。サーチコイル4の出力電圧Eはサーチコイル4が設
置されている空間の磁界の時間微分、即ち(1)式で与
えられる。
Next, referring to the characteristic waveform diagrams of FIGS. 4 and 5,
An embodiment of the present invention for detecting a DC bias by comparing the positive peak value H + P and the negative peak value H -P with each other will be described. The output voltage E of the search coil 4 is given by the time derivative of the magnetic field of the space where the search coil 4 is installed, that is, the equation (1).

E=N・S・μdH/dt ……(1) ここで、E:サーチコイル出力[V] N:サーチコイル巻線[ターン] S:サーチコイル断面積[m2] μ:サーチコイルの磁心の透磁率[H/m] H:磁界[A] 又、積分器12の出力EHはサーチコイル出力Eの時間積分
であり、元の磁界Hに対応している。
E = N ・ S ・ μdH / dt (1) where E: Search coil output [V] N: Search coil winding [Turn] S: Search coil cross-sectional area [m 2 ] μ: Search coil magnetic core Permeability [H / m] H: magnetic field [A] The output E H of the integrator 12 is the time integration of the search coil output E and corresponds to the original magnetic field H.

即ち、(2)式の関係にある。That is, there is a relationship of the formula (2).

EH=A∫Edt =AH/N・S・μ ……(2) ここで、A:積分器の積分定数 第3図の正側ピーク値検出器13−1と負側ピーク値検出
器13−2は第4図,第5図に示す磁界のそれぞれ正側ピ
ーク値H+Pと負側ピーク値H-Pを検出する。
E H = A∫Edt = AH / N · S · μ (2) where A: integration constant of integrator The positive peak value detector 13-1 and the negative side peak value detector 13 in FIG. -2 detects the positive side peak value H + P and the negative side peak value H -P of the magnetic field shown in FIGS. 4 and 5, respectively.

このとき、直流偏磁が生じていなければ、鉄心1の磁化
力は正負対称であるから、磁界Hの正側ピーク値H+P
び負側ピーク値H-Pは第4図のように対称になり、ピー
ク差ΔHは零となる。
At this time, if the DC bias is not generated, the magnetizing force of the iron core 1 is positive and negative symmetrical, so the positive peak value H + P and the negative peak value H -P of the magnetic field H are symmetrical as shown in FIG. And the peak difference ΔH becomes zero.

一方、直流偏磁が生じると、鉄心1の磁化力が正負非対
称となるため、第4図と同様の磁束φに対して、各ピー
ク値H+P及びH-Pは第5図のように非対称となり、例え
ば、負側ピーク値H-Pが小さくなる。従って、比較器14
から出力されるピーク差ΔHによって、直流偏磁が生じ
ていることが分かる。
On the other hand, when DC bias is generated, the magnetizing force of the iron core 1 becomes positive and negative asymmetrical. Therefore, for the magnetic flux φ similar to that in FIG. 4, the peak values H + P and H -P are as shown in FIG. It becomes asymmetric, and for example, the negative peak value H −P becomes smaller. Therefore, the comparator 14
It can be seen that the DC bias magnetism occurs due to the peak difference ΔH output from.

サーチコイル4の出力電圧波形をフーリエ級数展開する
か、又は積分後にフーリエ級数展開するかによって直流
偏磁を検出することも可能である。直流偏磁が生じてい
る場合にはE及びEHの波形には正側と負側が非対称にな
るために、偶数調波が含まれる。従って、フーリエ級数
展開して偶数調破の有無によって直流偏磁が生じている
ことを判断できる。
It is also possible to detect the DC bias magnetism by performing the Fourier series expansion of the output voltage waveform of the search coil 4 or the Fourier series expansion after integration. When DC bias is generated, the waveforms of E and E H include even harmonics because the positive and negative sides are asymmetrical. Therefore, it is possible to determine that the DC bias is generated depending on whether or not there is an even number breakdown by performing Fourier series expansion.

ところで、サーチコイルによる直流偏磁検出方法とし
て、変圧器のタンク内鉄心の近傍、例えば鉄心1−1,1
−2のほぼ中央に配置することも考えられるが、サーチ
コイルが故障した場合の取り替えが困難である。
By the way, as a method for detecting a DC bias magnetic field using a search coil, a method for detecting a DC bias magnetic field in the vicinity of an iron core in a tank of a transformer,
Although it may be possible to arrange it at approximately the center of -2, it is difficult to replace it when the search coil fails.

これに対し、第1図,第2図に示したように構成された
ものにおいては、例えばサーチコイル4が故障した場
合、カバー9を取り外しサーチコイル4を点検し故障箇
所の修理あるいは全体交換するなどの状況に応じた処置
を行う。それが終わればカバー9を取り付け作業は完了
する。このように、変圧器の外部より直流偏磁が検出で
きるので、サーチコイルが故障しても取り替えが容易で
ある。
On the other hand, in the configuration as shown in FIG. 1 and FIG. 2, for example, when the search coil 4 fails, the cover 9 is removed and the search coil 4 is inspected to repair or replace the failed part entirely. Take appropriate action depending on the situation. After that, the cover 9 is attached and the work is completed. In this way, since the DC bias magnetism can be detected from the outside of the transformer, it is easy to replace it even if the search coil fails.

[発明の効果] 以上のように、この発明によれば、磁性体からなるタン
ク外壁の変圧器鉄心に近接した一部分を高抵抗非磁性部
分で構成し、この高抵抗非磁性部分の外面に、変圧器鉄
心の偏磁状態を検出するサーチコイルを設置したので、
変圧器の直流偏磁をタンクの外部に設けたサーチコイル
で容易に検出でき、変圧器の運転中にもサーチコイルの
交換や保守を容易に行なうことができるという効果があ
る。
[Effects of the Invention] As described above, according to the present invention, a portion of the tank outer wall made of a magnetic material, which is close to the transformer iron core, is configured by a high resistance non-magnetic portion, and the outer surface of the high resistance non-magnetic portion is Since we installed a search coil to detect the biased state of the transformer core,
The DC bias magnetism of the transformer can be easily detected by the search coil provided outside the tank, and the search coil can be easily replaced and maintained even during operation of the transformer.

【図面の簡単な説明】[Brief description of drawings]

第1図はこの発明の一実施例を説明するための外鉄形の
変圧器の水平断面図、第2図(a)(b)は第1図の変
圧器を正面及び側面からみた構成図、第3図はこの発明
の一実施例に用いられる直流偏磁検出回路を示すブロッ
ク図、第4図(a)(b)及び第5図(a)(b)はこ
の発明の一実施例を説明するための磁界と磁束の特性を
示す各種波形図である。 1−1,1−2……鉄心、4……サーチコイル 5……タンク、12……積分器 13−1……正側ピーク値検出器 13−1……負側ピーク値検出器 14……比較器、15……タンクの高抵抗非磁性部分 尚、図中、同一符号は同一又は相当部分を示す。
FIG. 1 is a horizontal cross-sectional view of an outer iron type transformer for explaining an embodiment of the present invention, and FIGS. 2 (a) and 2 (b) are configuration diagrams of the transformer of FIG. 1 viewed from the front and side. FIG. 3 is a block diagram showing a DC bias magnetic detection circuit used in an embodiment of the present invention, and FIGS. 4 (a) (b) and 5 (a) (b) are embodiments of the present invention. FIG. 7 is various waveform diagrams showing characteristics of a magnetic field and a magnetic flux for explaining the above. 1-1, 1-2 ... iron core, 4 ... search coil 5 ... tank, 12 ... integrator 13-1 ... positive side peak value detector 13-1 ... negative side peak value detector 14 ... Comparator, 15 ... High resistance non-magnetic part of tank Incidentally, in the drawings, the same reference numerals indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】磁気回路を構成する変圧器鉄心の近傍にサ
ーチコイルを設け、このサーチコイルの出力電圧を積分
し、積分後の波形の正側ピーク値と負側ピーク値との大
小を比較することによって直流偏磁を検出する変圧器の
直流偏磁検出方法に於て、 前記変圧器鉄心を収容する磁性体からなるタンクの外壁
の一部を高抵抗非磁性部分で構成し、この高抵抗非磁性
部分の外面に前記サーチコイルを設けることを特徴とす
る変圧器の直流偏磁検出方法。
1. A search coil is provided in the vicinity of a transformer core that constitutes a magnetic circuit, the output voltage of the search coil is integrated, and the magnitudes of the positive side peak value and the negative side peak value of the waveform after integration are compared. In the method of detecting a DC bias magnetic field of a transformer for detecting a DC bias magnetic field, a part of the outer wall of the tank made of a magnetic material that houses the transformer core is composed of a high resistance non-magnetic part, A method for detecting a DC bias in a transformer, characterized in that the search coil is provided on an outer surface of a resistance non-magnetic portion.
JP1004373A 1989-01-10 1989-01-10 DC bias magnetism detection method for transformer Expired - Lifetime JPH07104736B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1004373A JPH07104736B2 (en) 1989-01-10 1989-01-10 DC bias magnetism detection method for transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1004373A JPH07104736B2 (en) 1989-01-10 1989-01-10 DC bias magnetism detection method for transformer

Publications (2)

Publication Number Publication Date
JPH02183816A JPH02183816A (en) 1990-07-18
JPH07104736B2 true JPH07104736B2 (en) 1995-11-13

Family

ID=11582563

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1004373A Expired - Lifetime JPH07104736B2 (en) 1989-01-10 1989-01-10 DC bias magnetism detection method for transformer

Country Status (1)

Country Link
JP (1) JPH07104736B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112415300B (en) * 2020-10-25 2021-12-31 国网湖北省电力有限公司电力科学研究院 Rail transit and transformer direct-current magnetic bias correlation analysis method
CN113836718B (en) * 2021-09-23 2023-12-29 中铁第四勘察设计院集团有限公司 A DC bias calculation method for high-speed maglev main substation transformer
CN114994443B (en) * 2022-06-07 2024-11-12 国网江西省电力有限公司电力科学研究院 A transformer neutral point DC bias current measuring instrument
CN119959603B (en) * 2025-02-17 2025-10-03 西安西电变压器有限责任公司 A method for determining DC bias current of a transformer and related device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2635714B2 (en) * 1988-09-14 1997-07-30 株式会社東芝 DC bias detection method for transformer core

Also Published As

Publication number Publication date
JPH02183816A (en) 1990-07-18

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