JPH04192510A - Iron core type reactor with gap - Google Patents
Iron core type reactor with gapInfo
- Publication number
- JPH04192510A JPH04192510A JP32431490A JP32431490A JPH04192510A JP H04192510 A JPH04192510 A JP H04192510A JP 32431490 A JP32431490 A JP 32431490A JP 32431490 A JP32431490 A JP 32431490A JP H04192510 A JPH04192510 A JP H04192510A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- core
- block
- iron core
- magnetic flux
- 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
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 title claims abstract description 23
- 230000005291 magnetic effect Effects 0.000 claims abstract description 72
- 238000004804 winding Methods 0.000 claims abstract description 15
- 239000000696 magnetic material Substances 0.000 claims abstract description 8
- 239000000843 powder Substances 0.000 claims abstract description 8
- 230000004907 flux Effects 0.000 abstract description 27
- 238000005245 sintering Methods 0.000 abstract description 5
- 238000000465 moulding Methods 0.000 abstract description 4
- 229910000976 Electrical steel Inorganic materials 0.000 description 11
- 238000013021 overheating Methods 0.000 description 6
- 238000010030 laminating Methods 0.000 description 4
- 239000012212 insulator Substances 0.000 description 2
- 229910000859 α-Fe Inorganic materials 0.000 description 2
- 230000002159 abnormal effect Effects 0.000 description 1
- 239000000853 adhesive Substances 0.000 description 1
- 230000001070 adhesive effect Effects 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000003302 ferromagnetic material Substances 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 239000011229 interlayer Substances 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 150000003376 silicon Chemical class 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔発明の目的〕
(産業上の利用分野)
本発明はブロック鉄心の上端部および下端部に配置され
、磁束の流れを制御する磁気プロスタを備えたギャップ
付鉄心形リアクトルに関する。[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention provides a gapped core reactor equipped with magnetic prosters arranged at the upper and lower ends of a block core to control the flow of magnetic flux. Regarding.
(従来の技術)
分路リアクトル等に用いられるリアクトルは、従来一般
にギャンプ付鉄心形リアクトルが用いられている。この
ギャップ付鉄心形リアクトルはけい素鋼帯を積層して形
成した複数個の円形ブロック鉄心を複数個の磁気的なギ
ャップを介して積み重ねてギャップ付の鉄心脚を構成し
、その上、下に同じくけい素鋼帯を積層して形成したヨ
ーク鉄心を配置し、前記鉄心脚に巻線を巻装して構成さ
れる。ギャップ部分には一般に絶縁物でできたギャップ
部材が介在される。このようなギャップ付鉄心形リアク
トルでは、ブロック鉄心内およびブロック鉄心と巻線と
の間に流れる磁束の一部が漏れ磁束としてヨーク鉄心の
締付部材に入射し、うず電流の発生により、局部的に過
大な温度上昇をもたらし損失を生じる恐れがある。(Prior Art) As a reactor used for a shunt reactor or the like, an iron core reactor with a gap has been generally used. This gapped core type reactor consists of a plurality of circular block cores formed by laminating silicon steel strips, which are stacked together via multiple magnetic gaps to form gapped core legs. A yoke core also formed by laminating silicon steel strips is disposed, and windings are wound around the core legs. A gap member made of an insulator is generally interposed in the gap portion. In such a gapped core reactor, a part of the magnetic flux flowing within the block core and between the block core and the winding enters the clamping member of the yoke core as leakage flux, causing eddy current to be generated locally. This may cause an excessive temperature rise and result in loss.
また、ブロック鉄心の断面形状は略々円形をしているこ
とから、ブロック鉄心から積層方向に同一幅のヨーク鉄
心に入射してくる磁束の量はヨーク鉄心の積層方向の中
央部で最大となり、積層方向の外側になるほど入射磁束
量が少なくなってくる。その為、ヨーク鉄心に流れ込ん
だ磁束はヨ−り鉄心と側脚の中を流れる時に磁束密度の
大きな中央部のけい素鋼帯から磁束密度の小さな外側の
けい素鋼帯へと移り流れる。このようにけい素鋼帯間で
調帯厚さ方向に突き抜けるように磁束が流れることによ
り、けい素鋼帯には大きなうず電流が発生して損失が増
加したり、ヨーク鉄心と側脚間の接触部において局部的
に電流が流れ異常過熱を起こす可能性もある。In addition, since the cross-sectional shape of the block core is approximately circular, the amount of magnetic flux that enters the yoke core of the same width from the block core in the stacking direction is maximum at the center of the yoke core in the stacking direction. The amount of incident magnetic flux decreases toward the outside in the stacking direction. Therefore, when the magnetic flux that has flowed into the yoke iron core flows through the yaw iron core and the side legs, it flows from the central silicon steel band where the magnetic flux density is high to the outer silicon steel band where the magnetic flux density is low. As the magnetic flux flows between the silicon steel strips in the direction of the strip thickness, large eddy currents are generated in the silicon steel strips, increasing loss, and causing damage between the yoke core and the side legs. There is also a possibility that current will flow locally at the contact area, causing abnormal overheating.
その為、容量の大きなりアクドルになると、巻線の上、
下端部に空間的絶縁上必要な距離を置いて、鉄心窓内を
貫通する強磁性体の磁気ブロックを設けているものがあ
る。この種の磁気ブロックとしては、米国特許4,25
7,025号公報(第3図参照)や実公昭61−112
625号公報(第4図参照)に公開されているものがあ
る。Therefore, when it comes to large-capacity acdles, the top of the winding,
Some have a magnetic block made of ferromagnetic material that passes through the core window at the lower end at a distance necessary for spatial insulation. As this type of magnetic block, US Pat.
Publication No. 7,025 (see Figure 3) and Utility Model Publication No. 61-112
There is one disclosed in Publication No. 625 (see Figure 4).
(発明が解決しようとする課!III)第3図に示す例
における磁気ブロック10はけい素鋼帯を短冊状に切断
したものを積層し、積層面をヨーク鉄心11の積層面に
対向するように、かつ積層方向が水平になるようにして
ヨーク鉄心11とブロック鉄心I2との間に絶縁物I3
を介してはさみ込まれている。この磁気ブロックにより
、ブロック鉄心12あるいは図示しない巻線からヨーク
鉄心11に向かう磁束は、磁気ブロック10内でヨーク
鉄心11の積層方向に対して均一な磁束分布となるよう
に流れる。しかし、この構造の磁気ブロックIOは、鉄
心窓内側にけい素鋼帯の平面部が位置しているため、巻
線端部のフリンジング磁束により過熱する恐れがある。(Problem to be solved by the invention! III) The magnetic block 10 in the example shown in FIG. An insulator I3 is placed between the yoke core 11 and the block core I2 so that the stacking direction is horizontal.
It is sandwiched through. Due to this magnetic block, the magnetic flux directed from the block core 12 or the winding (not shown) toward the yoke core 11 flows within the magnetic block 10 so as to have a uniform magnetic flux distribution in the stacking direction of the yoke core 11. However, in the magnetic block IO having this structure, since the flat part of the silicon steel strip is located inside the core window, there is a risk of overheating due to fringing magnetic flux at the end of the winding.
第4図は上記欠点を改善することを目的に提案されたも
ので、短冊状に切断されたけい素鋼帯20を放射状に積
層して磁気ブロック21を形成することにより磁気ブロ
ック21に入ってくる磁束による過熱防止を図ったもの
である。しかし、この構造の磁気ブロックにおいては、
ヨーク鉄心の積層方向に磁束が均一になるようにする#
i能が不十分となる欠点を有している。Fig. 4 has been proposed for the purpose of improving the above-mentioned drawbacks, and by forming a magnetic block 21 by laminating silicon steel strips 20 cut into rectangular strips in a radial manner, This is to prevent overheating due to magnetic flux. However, in a magnetic block with this structure,
Make the magnetic flux uniform in the stacking direction of the yoke core#
It has the disadvantage that its performance is insufficient.
本発明は以上の欠点を除去して、磁気ブロック自体の損
失を減らし、もれ磁束によるうず電流損、漂遊損を更に
低減させたギャップ付鉄心形リアクトルを提供すること
を目的とする。SUMMARY OF THE INVENTION An object of the present invention is to provide a gapped iron-core reactor that eliminates the above drawbacks, reduces loss in the magnetic block itself, and further reduces eddy current loss and stray loss due to leakage magnetic flux.
(課題を解決するための手段)
以上の目的を達成するために本発明においては磁気ブロ
ックを、粉体磁性体を焼結、成形したフェライトで形成
するようにしたものである。(Means for Solving the Problems) In order to achieve the above object, in the present invention, the magnetic block is formed of ferrite obtained by sintering and molding powder magnetic material.
(作 用)
このように磁気ブロックとして、粉体磁性体を焼結、成
形したフェライトで形成するようにしたので、磁気ブロ
ックの体積抵抗率が金属の106以上と極めて大きく、
商用周波数領域の磁束に対してはうず電流損を無視する
ことができる。従って磁気ブロックの過熱は全く問題に
ならず、ブロック鉄心および巻線からの不均一な分布の
磁束をヨーク鉄心へ均一に入射させる機能を十分果たす
ことができる。(Function) Since the magnetic block is made of ferrite formed by sintering and molding powder magnetic material, the volume resistivity of the magnetic block is extremely high, exceeding 106 of that of metal.
Eddy current losses can be ignored for magnetic flux in the commercial frequency range. Therefore, overheating of the magnetic block is not a problem at all, and the function of uniformly injecting the non-uniformly distributed magnetic flux from the block core and the windings into the yoke core can be fully achieved.
(実施例) 以下本発明の一実施例を図面を参照して説明する。(Example) An embodiment of the present invention will be described below with reference to the drawings.
第1図および第2図において、複数のブロック鉄心1を
磁気的なギャップ2を介して積み重ねてギャップ付の鉄
心脚3を構成し、この鉄心脚3の上、下端に粉体磁性体
を焼結、成形した板状の磁気ブロック9a、9bを左、
右の側脚4と共に少くとも巻線6を覆うように上、下か
らヨーク鉄心5a、5bにより挾み込む。In FIGS. 1 and 2, a plurality of block cores 1 are stacked with magnetic gaps 2 in between to form gapped core legs 3, and powder magnetic material is sintered at the upper and lower ends of the core legs 3. Finally, place the molded plate-shaped magnetic blocks 9a and 9b on the left.
It is inserted between the yoke cores 5a and 5b from above and below so as to cover at least the winding 6 together with the right side leg 4.
ブロック鉄心lと磁気ブロック9aとの間および磁気ブ
ロック9aと上部のヨーク鉄心5aとの間には、磁気ブ
ロック9aの体積抵抗率がきわめて大きいことから、ヨ
ーク鉄心5aやブロック鉄心1の層間短絡防止用の絶縁
板は不要であるが、けい素鋼体の積層面の工作上の不揃
いによる局所的な応力集中をさける為の薄い緩衝板を挿
入してもよい。また下部のヨーク鉄心5bと磁気ブロッ
ク9bとの間も同様である。Between the block iron core 1 and the magnetic block 9a and between the magnetic block 9a and the upper yoke iron core 5a, since the volume resistivity of the magnetic block 9a is extremely large, interlayer short circuits of the yoke iron core 5a and the block iron core 1 are prevented. Although an insulating plate is not necessary, a thin buffer plate may be inserted to avoid local stress concentration due to irregularities in the laminated surfaces of the silicon steel body. The same applies to the space between the lower yoke core 5b and the magnetic block 9b.
このような構成にすることにより、ブロック鉄心lから
ヨーク鉄心5a、5bに流れる磁束が外側にフリンジン
グして磁気ブロック9a、9bにどの方向から入射して
も、磁気ブロック9a、9b自身の体積抵抗率が極めて
大きいため、発熱して過熱する心配は全くない。また磁
気ブロンク9a。With this configuration, the magnetic flux flowing from the block iron core l to the yoke iron cores 5a, 5b fringes outward and enters the magnetic blocks 9a, 9b from any direction, reducing the volume of the magnetic blocks 9a, 9b themselves. Since the resistivity is extremely high, there is no need to worry about overheating. Also magnetic bronc 9a.
9bは無方向性であることから、磁気ブロック9a。Since 9b is non-directional, it is a magnetic block 9a.
9bに入射した磁束は、磁気ブロック9a、9b内のど
の方向にも自由に流れることができ、ヨーク鉄心5a、
5bに流れ込む磁束分布が積層方向において均一になる
ように磁気ブロック9a、9b内を流れる。従って、ヨ
ーク鉄心5a、5b内の積層けい素抗鋼帯間の磁束の移
り流れによる損失の発生や、ヨーク鉄心5a、5bと側
脚4接合部におけるうず電流の局部通電による過熱の発
生も抑制できる。The magnetic flux incident on the magnetic blocks 9b can freely flow in any direction within the magnetic blocks 9a, 9b, and the yoke cores 5a,
The magnetic flux flowing into the magnetic blocks 9a and 9b flows in such a manner that the magnetic flux distribution flowing into the magnetic blocks 5b becomes uniform in the stacking direction. Therefore, the occurrence of loss due to the flow of magnetic flux between the laminated silicon steel bands in the yoke cores 5a, 5b, and the occurrence of overheating due to local eddy current flow at the joints between the yoke cores 5a, 5b and the side legs 4 are also suppressed. can.
また、従来の磁気ブロックは厚さ0.3曽−程度の薄い
短冊状のけい素鋼帯を数1000枚も積層し、接着剤で
固着して形成していたため、磁性ブロックを製作するの
に多大な時間を要していたが、本発明による磁性ブロッ
クは粉体磁性体を焼結して一体成形することにより容易
に製作することができる。In addition, conventional magnetic blocks were formed by laminating several thousand thin rectangular silicon steel strips with a thickness of about 0.3 mm and fixing them with adhesive. Although it took a lot of time, the magnetic block according to the present invention can be easily manufactured by sintering powder magnetic material and integrally molding it.
以上のように複数のブロック鉄心を磁気的なギャップ部
材を介して積み重ねて鉄心脚を形成し、この鉄心脚に巻
線を巻装し、この鉄心脚を側脚と共に上、下からヨーク
鉄心により挾み込んだギャップ付鉄心形リアクトルにお
いて、鉄心脚の端部とヨーク鉄心との間に少くとも巻線
を覆うように粉体磁性体を焼結して成形した磁気ブロッ
クを挿入するようにしたので、磁気ブロック自体の損失
を減らし、もれ磁束によるうず電流積、漂遊損を更に低
減させたギャップ付鉄心形リアクトルを得ることができ
る。As described above, a plurality of block cores are stacked together via a magnetic gap member to form a core leg, a winding is wound around this core leg, and this core leg is connected to a yoke core from above and below along with side legs. In a sandwiched gap iron core type reactor, a magnetic block formed by sintering powder magnetic material is inserted between the end of the iron core leg and the yoke iron core so as to cover at least the winding wire. Therefore, it is possible to obtain a gapped iron-core reactor in which the loss of the magnetic block itself is reduced, and the eddy current product and stray loss due to leakage magnetic flux are further reduced.
第1図は本発明の一実施例を示す正面図、第2図は同側
面図、第3図は従来の磁気ブロンクを使用したりアクド
ルの斜視図、第4図は従来の他の磁気ブロックの平面図
である。
1・・・ブロック鉄心、2・・・ギャップ、3・・・鉄
心脚、5a、5b・・・ヨーク鉄心、6・・・巻線、9
a、9b・・・磁気ブロック。
出願人代理人 弁理士 鈴 江 武 彦3
5b
第1図
第2図
第3図
第4図Fig. 1 is a front view showing an embodiment of the present invention, Fig. 2 is a side view of the same, Fig. 3 is a perspective view of an axle using a conventional magnetic bronch, and Fig. 4 is a perspective view of another conventional magnetic block. FIG. DESCRIPTION OF SYMBOLS 1...Block core, 2...Gap, 3...Core legs, 5a, 5b...Yoke core, 6...Winding, 9
a, 9b...magnetic block. Applicant's agent Patent attorney Takehiko Suzue 3
5b Figure 1 Figure 2 Figure 3 Figure 4
Claims (1)
み重ねて鉄心脚を形成し、この鉄心脚に巻線を巻装し、
この鉄心脚を側脚と共に上、下からヨーク鉄心により挾
み込んだギャップ付鉄心形リアクトルにおいて、鉄心脚
の端部とヨーク鉄心との間に少くとも巻線を覆うように
粉体磁性体を焼結して成形した磁気ブロックを挿入して
なるギャップ付鉄心形リアクトル。A plurality of block iron cores are stacked together via a magnetic gap member to form a core leg, and a winding wire is wound around this core leg,
In a gap core type reactor in which this core leg is sandwiched between the yoke core from above and below along with the side legs, powder magnetic material is placed between the end of the core leg and the yoke core so as to cover at least the winding. An iron core reactor with a gap made by inserting a sintered and formed magnetic block.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP32431490A JPH04192510A (en) | 1990-11-27 | 1990-11-27 | Iron core type reactor with gap |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP32431490A JPH04192510A (en) | 1990-11-27 | 1990-11-27 | Iron core type reactor with gap |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04192510A true JPH04192510A (en) | 1992-07-10 |
Family
ID=18164415
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP32431490A Pending JPH04192510A (en) | 1990-11-27 | 1990-11-27 | Iron core type reactor with gap |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04192510A (en) |
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2000025327A1 (en) * | 1998-10-26 | 2000-05-04 | A.T.T. Advanced Transformer Technologies (1998) Ltd. | A three-phase transformer |
JP2008041880A (en) * | 2006-08-04 | 2008-02-21 | Sumitomo Electric Ind Ltd | Spacer for reactor and reactor |
JP2013069826A (en) * | 2011-09-22 | 2013-04-18 | Fuji Electric Co Ltd | Reactor |
CN103578692A (en) * | 2012-08-08 | 2014-02-12 | 成都达瑞斯科技有限公司 | Active-field all-magnetic shielding mouse cage-shaped iron yoke-free dry-type iron core reactor |
CN103632809A (en) * | 2012-08-28 | 2014-03-12 | 成都昊地科技有限责任公司 | Active field fully-magnetic shielding mouse-cage-shaped compensation reactor |
CN103632807A (en) * | 2012-08-28 | 2014-03-12 | 成都昊地科技有限责任公司 | Active field fully-magnetic shielding mouse-cage-shaped iron core filter reactor |
US20140292455A1 (en) * | 2011-10-31 | 2014-10-02 | Hitachi, Ltd. | Reactor, Transformer, and Power Conversion Apparatus Using Same |
JP2015053464A (en) * | 2013-09-09 | 2015-03-19 | 台達電子企業管理(上海)有限公司 | Inductor, and switching circuit including the same |
-
1990
- 1990-11-27 JP JP32431490A patent/JPH04192510A/en active Pending
Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2000025327A1 (en) * | 1998-10-26 | 2000-05-04 | A.T.T. Advanced Transformer Technologies (1998) Ltd. | A three-phase transformer |
US6792666B1 (en) | 1998-10-26 | 2004-09-21 | A.T.T Advanced Transformer Technologies (1998) Ltd. | Three-phase transformer |
US6880228B2 (en) | 1998-10-26 | 2005-04-19 | A.T.T. Advanced Transformer Technologies, Ltd. | Method for manufacturing a three-phase transformer |
JP2008041880A (en) * | 2006-08-04 | 2008-02-21 | Sumitomo Electric Ind Ltd | Spacer for reactor and reactor |
JP2013069826A (en) * | 2011-09-22 | 2013-04-18 | Fuji Electric Co Ltd | Reactor |
US20140292455A1 (en) * | 2011-10-31 | 2014-10-02 | Hitachi, Ltd. | Reactor, Transformer, and Power Conversion Apparatus Using Same |
CN103578692A (en) * | 2012-08-08 | 2014-02-12 | 成都达瑞斯科技有限公司 | Active-field all-magnetic shielding mouse cage-shaped iron yoke-free dry-type iron core reactor |
CN103632809A (en) * | 2012-08-28 | 2014-03-12 | 成都昊地科技有限责任公司 | Active field fully-magnetic shielding mouse-cage-shaped compensation reactor |
CN103632807A (en) * | 2012-08-28 | 2014-03-12 | 成都昊地科技有限责任公司 | Active field fully-magnetic shielding mouse-cage-shaped iron core filter reactor |
JP2015053464A (en) * | 2013-09-09 | 2015-03-19 | 台達電子企業管理(上海)有限公司 | Inductor, and switching circuit including the same |
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