JPH01283911A - Power transformer - Google Patents

Power transformer

Info

Publication number
JPH01283911A
JPH01283911A JP11524588A JP11524588A JPH01283911A JP H01283911 A JPH01283911 A JP H01283911A JP 11524588 A JP11524588 A JP 11524588A JP 11524588 A JP11524588 A JP 11524588A JP H01283911 A JPH01283911 A JP H01283911A
Authority
JP
Japan
Prior art keywords
magnetic flux
superconductor
iron core
superconductors
outgoing
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
Application number
JP11524588A
Other languages
Japanese (ja)
Inventor
Shinichiro Hayashi
伸一郎 林
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 JP11524588A priority Critical patent/JPH01283911A/en
Publication of JPH01283911A publication Critical patent/JPH01283911A/en
Pending legal-status Critical Current

Links

Landscapes

  • Regulation Of General Use Transformers (AREA)

Abstract

PURPOSE:To ensure offset of penetrating magnetic flux with third harmonic wave current, by winding superconductors at the upper and the lower parts of an iron core having three legs in a three-phase transformer, or mounting the superconductors in a planar pattern. CONSTITUTION:Third harmonic waves are outputted from an iron core 1. A superconductor 2 is formed in one turn. The superconductors 1 are mounted on the surrounding part of the upper and the lower parts of the iron core 1. Or the superconductor is mounted on one part. Or the outgoing parts of the harmonic waves are covered with superconductive flat plates 6 and 7. When magnetic flux is going to pass through the superconductors 2, induced electromotive forces are generated and currents are made to flow. Thus, offsetting magnetic flux is generated. It is necessary to provide a conductor having the number of turns or the cross sectional area which is equal to ampere turns forming said magnetic flux in order to make the outgoing magnetic flux zero. When this is performed with the superconductor, the magnetic flux can be offset with the thin conductor.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は第3高調波電流を含有するインバータや整流
器に適用される[源変圧器に適用する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention is applied to inverters and rectifiers containing third harmonic current [applied to source transformers].

〔従来の技術〕[Conventional technology]

第2図は例えば電気書院発行[変圧器の設計工作法12
39頁、及び丸善発行「電気概論」123頁に示されて
いる3相内鉄形鉄心構造の電源変圧器を示す0図に於い
て鉄心(りの3脚に夫々U相用コイル(4)、V相用コ
イル(6)、W相用コイル(3)が巻回さnていること
を示す。こnら3相のコイルには夫々2π/ 3 (r
 a d)の位相差を持った磁束が発生しておりその代
数和は零である。従って磁束は鉄心の外へ出ることはな
い、また負荷電流として各相へ流れる電流も2π/3(
rad)の位相差のため各相のアンペアターンは打消す
のづ、それによる磁束は鉄心外へ出ることはない。とこ
ろがインバータや整流器の電源として使用した場合に第
3高調波を含む電流が流れる場合があり、この様な時は
各相鉄心の磁束−A、φB、及び−〇は同相となるため
打消し合わず鉄心の外、即ち上下に出てしまう。この様
な磁束は外部の機器に影響を及ぼし磁束変化のうず電流
による導体の過熱などの不具合を生じる。
For example, Figure 2 is published by Denki Shoin [Transformer Design and Construction Method 12]
In Figure 0, which shows a power transformer with a three-phase iron core structure shown on page 39 and page 123 of "Electrical Introduction" published by Maruzen, there are U-phase coils (4) on each of the three legs of the core. , a V-phase coil (6), and a W-phase coil (3).
Magnetic fluxes with a phase difference of a and d) are generated, and their algebraic sum is zero. Therefore, the magnetic flux does not go out of the iron core, and the current flowing to each phase as a load current is also 2π/3 (
The ampere turns of each phase are canceled due to the phase difference of rad), and the resulting magnetic flux does not exit the iron core. However, when used as a power source for an inverter or rectifier, current containing third harmonics may flow, and in such cases, the magnetic fluxes -A, φB, and -〇 of each phase core are in phase, so they cancel each other out. It comes out outside the iron core, that is, at the top and bottom. Such magnetic flux affects external equipment, causing problems such as overheating of conductors due to eddy currents caused by changes in magnetic flux.

このような第3高調波を含む電流は商用周波の電源にお
いても電源投入時の突入電流においても鉄心の飽和特性
により生じる。
A current including such a third harmonic is generated due to the saturation characteristics of the iron core both in a commercial frequency power supply and in an inrush current when the power is turned on.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

また外出する磁束は変圧器の近くに実装されている電子
機器などの電子回路にノイズを与え誤動作の原因となる
In addition, the magnetic flux that goes out causes noise in electronic circuits such as electronic devices installed near the transformer, causing malfunctions.

以下のように従来のWl電源変圧器3脚構造のため第3
高調波電流による磁束を鉄心外へ出し導体の過熱とか電
子機器の誤動作を生じるなどの課題があった。
Due to the conventional Wl power transformer three-legged structure as shown below, the third
There were problems such as the magnetic flux caused by harmonic currents flowing outside the core, causing overheating of conductors and malfunction of electronic equipment.

この発明は上記のような課題を解消するためになされた
ものでF@3高調波を有する電流を生じても鉄心内に生
じる磁束を鉄心外へ出さない様にすることを目的とする
This invention was made to solve the above-mentioned problems, and an object thereof is to prevent the magnetic flux generated within the iron core from flowing out of the iron core even if a current having F@3 harmonics is generated.

〔課題を解決するための手段〕[Means to solve the problem]

この発明は第3高調波が鉄心より外出する周囲を超電導
体で1ターンを形成したものを鉄心の上下又は一方に装
着するか、又は該高調波の外出部を超電導の平板でおお
うものである。
In this invention, one turn of a superconductor is formed around the area where the third harmonic goes out from the iron core, and one turn is attached to the top and bottom or one side of the iron core, or the part where the third harmonic goes out is covered with a superconducting flat plate. .

〔作用〕[Effect]

この発明における超電導体は外出する磁束と交叉するた
め、それを打消すべく超電力を生じ、その超m力による
電流は外出する磁束を打消すため外部に磁束は出ない。
Since the superconductor in this invention intersects with the outgoing magnetic flux, it generates superpower to cancel it, and the current due to the superm force cancels out the outgoing magnetic flux, so no magnetic flux exits to the outside.

〔発明の実施例〕[Embodiments of the invention]

以下、この発明の一実施例を図について説明する。第1
図において鉄心(りの3脚部に夫々U相コイル(4)、
V相コイル+5)、W相コイル(3)が巻回さnている
。これらの各コイルに第3高調波電流が流nると第2図
で説明したように同相となって外部へ出る。ここで本発
明は超電導体(2)を鉄心(1)の上下の全周に巻くも
のである。この様な構造のものにおいて該超電導体(2
)の中を磁束が通過しようとするとそれに誘起々電力を
生じて電流を流し打消す磁束を生ずる。この様な作用は
常電導体でも同じように行なうが超電導体は電気抵抗が
零のため作用する効果は大となり且つ損失もない、また
外出する磁束を零にするためには、それを作っているア
ンペアターンに等しい量の巻数又は導体断面積を有する
導体が必要であるが、こfを超電導体で行なうと細い導
体で可能でありコンパクトで且つ!電気抵抗が零のため
磁束を打ける作用の大きなものを達成することができる
An embodiment of the present invention will be described below with reference to the drawings. 1st
In the figure, there are U-phase coils (4) on each of the three legs of the iron core.
A V-phase coil +5) and a W-phase coil (3) are wound. When the third harmonic current flows through each of these coils, it becomes the same phase as explained in FIG. 2 and goes out to the outside. Here, in the present invention, the superconductor (2) is wound all around the top and bottom of the iron core (1). In such a structure, the superconductor (2
) When a magnetic flux tries to pass through it, it generates an induced electric power, which causes a current to flow and cancel out the magnetic flux. This kind of action occurs in the same way with normal conductors, but since the electrical resistance of superconductors is zero, the effect is greater and there is no loss.In addition, in order to reduce the outgoing magnetic flux to zero, it is necessary to create a superconductor. A conductor with the number of turns or conductor cross-sectional area equal to the number of ampere turns is required, but if this is done with a superconductor, it can be done with a thin conductor, compact and! Since the electrical resistance is zero, it is possible to achieve a large effect of applying magnetic flux.

第3図は本発明の他の実施例であII)i1図と同様に
鉄心(1)の各脚に夫々U相コイル(4)、v相コイル
(5)、W相コイル(3)が巻回されているのは同じで
あるが、鉄心+1)の上下に超電導体の平板(6)を装
着するものである。平板(6)の作用は第1図で説明し
た超電導体(2)と同じ作用をするものである。
Fig. 3 shows another embodiment of the present invention, and similarly to Fig. II)i1, a U-phase coil (4), a V-phase coil (5), and a W-phase coil (3) are installed on each leg of the iron core (1), respectively. The winding is the same, but superconductor flat plates (6) are attached above and below the iron core +1). The function of the flat plate (6) is the same as that of the superconductor (2) explained in FIG.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明によれば3相変圧器の3脚の鉄
心の上下部に超電導体を巻回、又は平板状に装着したの
で第3高調波電流によって貫通しようとする磁束を打消
す作用をコンパクトに且つ確実に行えることを特徴とす
るものである。
As described above, according to the present invention, the superconductor is wound or attached in a flat plate shape to the upper and lower parts of the iron core of the three legs of the three-phase transformer, so that the magnetic flux that attempts to penetrate by the third harmonic current is canceled out. It is characterized by being able to perform its functions compactly and reliably.

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

第1図は本発明の一実施例による電源変圧器の斜視図。 第2図は従来の変圧器の正面図。 第3図は本発明の他の実施例による電源変圧器の斜視図
である。 なお、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 power transformer according to an embodiment of the present invention. Figure 2 is a front view of a conventional transformer. FIG. 3 is a perspective view of a power transformer according to another embodiment of the invention. In addition, in the figures, the same reference numerals indicate the same or equivalent parts.

Claims (2)

【特許請求の範囲】[Claims] (1)電源変圧器において、主脚鉄心を貫通する磁束の
方向と直角に上記主脚鉄心の上下方部全体もしくはその
一方を超電導体でおおうことを特徴とする電源変圧器。
(1) A power transformer characterized in that the whole or one of the upper and lower parts of the main landing gear core is covered with a superconductor at right angles to the direction of magnetic flux passing through the main landing gear core.
(2)鉄心脚をおおう超電導体の形状を環状もしくは板
状にしたことを特徴とする特許請求の範囲第1項記載の
電源変圧器。
(2) The power transformer according to claim 1, wherein the superconductor covering the core legs has a ring-like or plate-like shape.
JP11524588A 1988-05-11 1988-05-11 Power transformer Pending JPH01283911A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11524588A JPH01283911A (en) 1988-05-11 1988-05-11 Power transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11524588A JPH01283911A (en) 1988-05-11 1988-05-11 Power transformer

Publications (1)

Publication Number Publication Date
JPH01283911A true JPH01283911A (en) 1989-11-15

Family

ID=14657935

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11524588A Pending JPH01283911A (en) 1988-05-11 1988-05-11 Power transformer

Country Status (1)

Country Link
JP (1) JPH01283911A (en)

Similar Documents

Publication Publication Date Title
JPS5998510A (en) Transformer for rectifier
JPH0691335B2 (en) Shield of electromagnetic equipment
US20210383961A1 (en) Transformer
JPS607115A (en) 3-phase inner core type transformer
JP3566481B2 (en) Eddy current shield device and three-phase transformer
JP3533252B2 (en) Transformer
JP3646595B2 (en) Static induction machine
US4663700A (en) Way of placing chokes with air core
JPH01283911A (en) Power transformer
JPS59119810A (en) Interphase reactor device
JPH0722996Y2 (en) Noise prevention device
KR100428459B1 (en) An apparatus for reducing harmonics
JPS61161942A (en) Voltage compensating circuit of synchronous generator
KR100790523B1 (en) Harmonics removal equipment that possess electric power curtailment function
JPH0613250A (en) Motor-transformer
JPS59229809A (en) Triangular three-leg type three-phase reactor
JPH0741144Y2 (en) Current transformer
JPS61170010A (en) Transformer iron core
JP3327460B2 (en) Current transformer
JPH0419992Y2 (en)
JP2656057B2 (en) Transformers for vehicles
JPS61166015A (en) High tension transformer
JPH01108714A (en) Current transformer
JP3226051B2 (en) DC power supply
JPH02220419A (en) Split type stationary electric apparatus