JP2736134B2 - DC reactor iron core - Google Patents
DC reactor iron coreInfo
- Publication number
- JP2736134B2 JP2736134B2 JP27171889A JP27171889A JP2736134B2 JP 2736134 B2 JP2736134 B2 JP 2736134B2 JP 27171889 A JP27171889 A JP 27171889A JP 27171889 A JP27171889 A JP 27171889A JP 2736134 B2 JP2736134 B2 JP 2736134B2
- Authority
- JP
- Japan
- Prior art keywords
- iron core
- leg
- core
- silicon steel
- reactor
- 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
Links
Landscapes
- Regulation Of General Use Transformers (AREA)
- Dc-Dc Converters (AREA)
Description
【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明は整流装置の直流回路の高調波成分を低くする
ために使われる直流リアクトルの鉄心に関する。DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial application field) The present invention relates to an iron core of a DC reactor used for reducing a harmonic component of a DC circuit of a rectifier.
(従来の技術) コンピュータの無停電電源装置としては、定電圧,定
周波数出力を得るCVCF電源装置が広く用いられている。(Conventional technology) As an uninterruptible power supply for a computer, a CVCF power supply for obtaining a constant voltage and a constant frequency output is widely used.
このCVCF電源装置には、その中に整流装置があり、そ
こでの直流回路の高調波成分を低くする目的から直流リ
アクトルが入っている。In this CVCF power supply, there is a rectifier in which a DC reactor is inserted for the purpose of reducing harmonic components of the DC circuit.
一般に直流リアクトルの磁気回路では、直流分の磁束
密度BDCは次式で表わされる。Generally, in a magnetic circuit of a DC reactor, the magnetic flux density B DC of the DC component is expressed by the following equation.
BDC=0.4πNIDC/Lg ここで、NIDCは直流のアンペアターン,Lgは全空隙長
であり、空隙部断面積と鉄心見掛け断面積が等しい場合
である。上式からわかるように大電流が流れても磁気回
路を飽和させないように空隙長Lgを設けている。B DC = 0.4πNI DC / Lg Here, NI DC is a DC ampere-turn, Lg is the total gap length, and the case where the sectional area of the gap is equal to the apparent sectional area of the iron core. As can be seen from the above equation, the gap length Lg is provided so as not to saturate the magnetic circuit even when a large current flows.
この磁気回路上の空隙は一ケ所で集中的に大きくとる
と、漏洩磁束や巻線との結合係数が悪くなる。そのため
直流リアクトルでは、レグ鉄心磁路の上下端に、あるい
はレグ鉄心磁路を複数個に分割してそれぞれの分割部分
に空隙を設けた構成をとっている。この場合空隙には絶
縁物製の間隔板を介在させている。If the air gap on the magnetic circuit is intensively increased in one place, the leakage magnetic flux and the coupling coefficient with the windings are deteriorated. For this reason, the DC reactor has a configuration in which a gap is provided at the upper and lower ends of the leg iron core magnetic path or the leg iron core magnetic path is divided into a plurality of parts and each divided part is provided with a gap. In this case, a spacing plate made of an insulating material is interposed in the gap.
第2図はこうした鉄心構成を有する乾式直流リアクト
ルを示し、第3図は鉄心を示している。FIG. 2 shows a dry DC reactor having such an iron core configuration, and FIG. 3 shows an iron core.
ここで、1はレジンモールドされたコイル、2はその
コイルを貫通して磁気回路を構成する鉄心である。この
鉄心2は上部当板3と下部の脚板4を介して複数本の鉄
心締付ボルト5で固定されている。また鉄心2は第3図
に示すようにけい素鋼板を積層してなるブロック状のレ
グ鉄心を絶縁物製の間隔板203を介して交互に積み重ね
てなるレグ鉄心磁路202a,202bと、このレグ鉄心磁路202
a,202bの両端を閉じるように上,下に配置されたヨーク
鉄心磁路201a,201bとで構成されて磁気回路を成してい
る。Here, 1 is a resin-molded coil, and 2 is an iron core penetrating the coil and constituting a magnetic circuit. The iron core 2 is fixed with a plurality of iron core tightening bolts 5 via an upper contact plate 3 and a lower leg plate 4. Also, as shown in FIG. 3, the iron core 2 has leg iron magnetic paths 202a and 202b formed by alternately stacking block-shaped leg irons made of laminated silicon steel plates via insulating spacers 203. Leg core magnetic path 202
The magnetic circuit is composed of yoke iron core magnetic paths 201a and 201b arranged above and below so as to close both ends of the a and 202b.
(発明が解決しようとする課題) 前記磁気回路には、本来の直流リアクトルの役目であ
る高周波成分を低くする狙いのために高周波成分が入り
込み、直流分にのった高周波リップルが鉄心を励磁して
磁歪振動を引き起こす。磁歪振動はレグ鉄心と間隔板20
3との間で相対振動を起すか、ヨーク鉄心に上下振動を
伝え、更に直流リアクトルの取付床面に伝わるかする。
いずれの場合も高周波成分だけに耳障りな振動音を発生
することになり問題点をもっていた。(Problems to be Solved by the Invention) In the magnetic circuit, a high-frequency component enters for the purpose of lowering a high-frequency component, which is a function of an original DC reactor, and a high-frequency ripple on a DC component excites an iron core. Causes magnetostrictive vibration. Magnetostrictive vibration is leg iron core and spacing plate 20
Either a relative vibration is generated between them, or a vertical vibration is transmitted to the yoke iron core, and further transmitted to the mounting floor of the DC reactor.
In any case, an unpleasant vibration sound is generated only by the high frequency component, which has a problem.
従って本発明は鉄心の磁歪による振動および振動音を
極めて小さくする直流リアクトルの鉄心を提供すること
を目的としている。Accordingly, it is an object of the present invention to provide a DC reactor iron core in which vibration and vibration noise due to magnetostriction of the iron core are extremely reduced.
[発明の構成] (課題を解決するための手段) 上記目的を達成するために本発明はけい素鋼板を積層
してなるレグ鉄心を有するレグ鉄心磁路と、けい素鋼板
を積層してなり前記レグ鉄心を閉じるヨーク鉄心磁路と
で構成される直流リアクトルの鉄心において、前記レグ
鉄心のみ少なくとも一部に6.5%けい素鋼板を用いたこ
とを特徴とする。[Constitution of the Invention] (Means for Solving the Problems) In order to achieve the above object, the present invention provides a leg core magnetic path having a leg core formed by laminating silicon steel plates, and a silicon steel plate laminated. In the iron core of a DC reactor comprising a yoke iron core magnetic path closing the leg iron core, a 6.5% silicon steel plate is used at least partially for the leg iron core.
(作用) 振動音の直接的な発生源はレグ鉄心磁路であり、この
レグ鉄心磁路を構成するレグ鉄心の少なくとも一部に磁
歪がほとんどない鉄心材料を用いることで、振動の発生
が極めて抑制され、その結果直流リアクトルの課題とさ
れた振動音の激減されることになる。(Operation) The direct generation source of the vibration sound is the leg iron core magnetic path. At least a part of the leg iron core constituting the leg iron core magnetic path is made of an iron core material having almost no magnetostriction. As a result, the vibration noise, which is a problem of the DC reactor, is drastically reduced.
(実施例) 以下本発明の一実施例を説明する。Example An example of the present invention will be described below.
第1図はレグ鉄心磁路を構成するレグ鉄心202の図で
ある。このレグ鉄心202の構成はけい素鋼板202−1を積
層し、その両側に端板当板202−2を配置し、締付ボル
ト202−3でもって一体化している。このレグ鉄心202は
そのほとんどを方向性けい素鋼板を積層して構成されて
いるが、積層方向両側部分に6.5%けい素鋼板を用いて
所定の積層厚さlとしている。この6.5%けい素鋼板は
下表に示すように一般の方向性けい素鋼板よりも磁歪と
鉄損(1kHz)が低い。FIG. 1 is a view of a leg core 202 constituting a leg core magnetic path. The configuration of the leg iron core 202 is such that silicon steel plates 202-1 are laminated, end plate contact plates 202-2 are arranged on both sides thereof, and integrated with fastening bolts 202-3. Most of the leg core 202 is formed by laminating directional silicon steel sheets, and a predetermined lamination thickness 1 is formed by using 6.5% silicon steel sheets on both sides in the laminating direction. As shown in the table below, this 6.5% silicon steel sheet has lower magnetostriction and iron loss (1 kHz) than ordinary oriented silicon steel sheet.
第1図に示すレグ鉄心202において、磁束はそのレグ
鉄心202の上面と直角方向のA方向に流れる。従って通
常磁歪は上下方向に大きく発生するが、この鉄心材料が
6.5%けい素鋼板となっているため磁歪は極めて小さい
ものとなる。この場合、一部だけでなくレグ鉄心の全て
に6.5%けい素鋼板を用いても同様である。レグ鉄心202
の磁歪が大幅に減少すれば、間隔板との間で相対振動を
起こさず振動音の発生がなくなる。従ってレグ鉄心磁路
からヨーク鉄心磁路へ、あるいはレグ鉄心磁路の外側へ
振動伝幅させることもなくなる。 In the leg core 202 shown in FIG. 1, the magnetic flux flows in the direction A perpendicular to the upper surface of the leg core 202. Therefore, magnetostriction is usually large in the vertical direction.
Since it is a 6.5% silicon steel sheet, the magnetostriction is extremely small. In this case, the same applies to the case where 6.5% silicon steel sheet is used for not only a part but also all of the leg cores. Leg iron core 202
If the magnetostriction is greatly reduced, no relative vibration occurs between the spacer and the spacing plate, and no vibration noise is generated. Therefore, the vibration does not propagate from the leg core magnetic path to the yoke core magnetic path or outside the leg core magnetic path.
ここで、ヨーク鉄心磁路に6.5%けい素鋼板を用いな
いのは、ヨーク鉄心磁路も磁歪を生じるが、その磁歪の
方向は長手方向であり、他に影響を及ぼして振動音を発
生させたり振動を大きく伝幅させるようには作用しない
ためである。Here, the reason for not using a 6.5% silicon steel plate for the yoke core magnetic path is that the yoke core magnetic path also generates magnetostriction, but the direction of the magnetostriction is the longitudinal direction, which affects other parts and generates vibration noise. This is because it does not act to greatly propagate the vibration.
また、高価で加工性が難しい6.5%けい素鋼板を効果
の少ないヨーク鉄心磁路にまで用いる必要はないためで
もある。Another reason is that it is not necessary to use an expensive and difficult-to-work 6.5% silicon steel sheet even for a yoke core magnetic path with little effect.
[発明の効果] 以上のように、けい素鋼板を積層してなるレグ鉄心の
み少なくともその一部に6.5%けい素鋼板を用いること
により、従来の直流リアクトルに特有な耳障りな振動音
の発生や外部への振動伝幅を極めて小さくすることが出
来る。[Effects of the Invention] As described above, by using 6.5% silicon steel sheet for at least a part of only the leg iron core formed by stacking silicon steel sheets, generation of annoying vibration sound peculiar to the conventional DC reactor can be achieved. The width of vibration transmission to the outside can be made extremely small.
第1図は本発明の一実施例による直流リアクトルのレグ
鉄心の斜視図,第2図は一般的な乾式直流リアクトルの
構造を示す正面図,第3図は直流リアクトルの鉄心を示
す正面図である。 1……レジンモールドコイル,2……鉄心, 3……上部当板,4……脚板,5……締付ボルト, A……磁束の方向,l……レグ鉄心幅, 201……ヨーク鉄心, 201a,201b……上下部ヨーク鉄心, 202……レグ鉄心,202a,202b……右側レグ鉄心, 202−1……方向性けい素鋼板,202−2……端当板, 202−3……締付ボルト,203……間隔板。FIG. 1 is a perspective view of a leg core of a DC reactor according to one embodiment of the present invention, FIG. 2 is a front view showing a structure of a general dry DC reactor, and FIG. 3 is a front view showing an iron core of the DC reactor. is there. 1 ... resin molded coil, 2 ... iron core, 3 ... upper plate, 4 ... leg plate, 5 ... tightening bolt, A ... direction of magnetic flux, l ... leg core width, 201 ... yoke core , 201a, 201b ... Upper and lower yoke cores, 202 ... Leg cores, 202a, 202b ... Right leg cores, 202-1 ... Oriented silicon steel plate, 202-2 ... End plate, 202-3 ... … Tightening bolt, 203 …… Space plate.
Claims (1)
るレグ鉄心磁路と、けい素鋼板を積層してなり前記レグ
鉄心を閉じるヨーク鉄心磁路とで構成される直流リアク
トルの鉄心において、前記レグ鉄心のみ少なくとも一部
に6.5%けい素鋼板を用いたことを特徴とする直流リア
クトルの鉄心。1. A DC reactor core comprising: a leg core magnetic path having a leg core formed by laminating silicon steel sheets; and a yoke core magnetic path formed by laminating silicon steel sheets and closing the leg core. An iron core of a DC reactor, wherein at least a part of the leg iron core is made of a 6.5% silicon steel sheet.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP27171889A JP2736134B2 (en) | 1989-10-20 | 1989-10-20 | DC reactor iron core |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP27171889A JP2736134B2 (en) | 1989-10-20 | 1989-10-20 | DC reactor iron core |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH03135007A JPH03135007A (en) | 1991-06-10 |
| JP2736134B2 true JP2736134B2 (en) | 1998-04-02 |
Family
ID=17503873
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP27171889A Expired - Lifetime JP2736134B2 (en) | 1989-10-20 | 1989-10-20 | DC reactor iron core |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2736134B2 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7965163B2 (en) * | 2007-01-15 | 2011-06-21 | Hitachi Metals, Ltd. | Reactor core and reactor |
| JP2009141117A (en) * | 2007-12-06 | 2009-06-25 | Daikin Ind Ltd | Reactor |
| JP2009259971A (en) * | 2008-04-15 | 2009-11-05 | Tdk Corp | Coil product and reactor |
| CN109461564A (en) * | 2018-12-27 | 2019-03-12 | 日新电机(无锡)有限公司 | A kind of iron core package assembly and reactor based on radial iron core cake |
-
1989
- 1989-10-20 JP JP27171889A patent/JP2736134B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH03135007A (en) | 1991-06-10 |
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