JPS61204908A - Magnetic core - Google Patents

Magnetic core

Info

Publication number
JPS61204908A
JPS61204908A JP60045837A JP4583785A JPS61204908A JP S61204908 A JPS61204908 A JP S61204908A JP 60045837 A JP60045837 A JP 60045837A JP 4583785 A JP4583785 A JP 4583785A JP S61204908 A JPS61204908 A JP S61204908A
Authority
JP
Japan
Prior art keywords
magnetic core
gap
magnetic
soft magnetic
magnetic material
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
JP60045837A
Other languages
Japanese (ja)
Inventor
Kiyotaka Yamauchi
山内 清隆
Katsuto Yoshizawa
克仁 吉沢
Osamu Shimoe
治 下江
Susumu Nakajima
晋 中島
Shunsuke Arakawa
俊介 荒川
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.)
Proterial Ltd
Original Assignee
Hitachi Metals Ltd
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 Hitachi Metals Ltd filed Critical Hitachi Metals Ltd
Priority to JP60045837A priority Critical patent/JPS61204908A/en
Publication of JPS61204908A publication Critical patent/JPS61204908A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain a magnetic core for non-linear choke having a simple structure and excellent performance by providing a gap in a portion of an annular magnetic core consisting of a soft magnetic material, and inserting into the whole or a part of the gap a gap spacer made of a soft magnetic material, the resistivity of which has a value sufficiently large as compared with the resistivity of the magnetic core. CONSTITUTION:A gap is provided in a portion of a magnetic core 1, 1' or 2 consisting of a soft magnetic material, and in the whole or a part of the gap, a member made of a soft magnetic material the resistivity of which has a value sufficiently large as compared with the resistivity of the magnetic core 1, 1' or 2 is inserted and arranged as a gap spacers 3, 3'. A thin amorphous alloy band is made by the one-side roll method, the obtained thin band is wound to make a magnetic core 2 having an outer diameter of 35mm, inner diameter of 20mm and thickness of 10mm, and the predetermined heat treatment is performed. After this is impregnated with epoxy resin and is hardened, a part of the magnetic path is cut by means of a grindstone so as to form a 0.8mm gap. A soft magnetic plate 3' made of a pressed powder of ferrite or permalloy having a shape of 15X15X0.8<t>mm is inserted into this gap portion and is fixed by means of an adhesive.

Description

【発明の詳細な説明】 し産業上の利用分野1 本発明は主として直流電流を重畳させて使用するコイル
類の磁心に関するものであり、特にスイッチング電源の
出力平滑回路等のローパスフィルタに用いるチョークコ
イル用磁心として適した磁心に関するものである。すな
わち、本発明は平滑効果が高く、高周波で使用しても発
熱が小さい磁心を提供せんとするものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application 1 The present invention mainly relates to magnetic cores of coils used with superimposed direct current, and particularly to choke coils used in low-pass filters such as output smoothing circuits of switching power supplies. This invention relates to a magnetic core suitable as a commercial magnetic core. That is, the present invention aims to provide a magnetic core that has a high smoothing effect and generates little heat even when used at high frequencies.

し従来の技術1 従来、チョークコイルやスイッチング電源の出力フィル
ターあるいはフライバックコンバータのパワートランス
等の様に、直流電流を重畳させて使用するコイル類にお
いては、直流電流による磁心の磁気飽和を防ぐために、
第5図に例示するように磁心1,1′または2の一部に
ギャップG1またはG2が設けられている。
Conventional technology 1 Conventionally, in coils that are used with superimposed direct current, such as choke coils, output filters of switching power supplies, or power transformers of flyback converters, in order to prevent magnetic saturation of the magnetic core due to direct current, ,
As illustrated in FIG. 5, a gap G1 or G2 is provided in a part of the magnetic core 1, 1' or 2.

この様なギャップを設けることにより、第6図【J例示
する様に、起磁り\11\ −コイルの5数。
By providing such a gap, as shown in FIG.

1“コイルを7Qれる電流)の変(ヒ(こl・1して、
]イルのインダクタシス[−か 、rjどへる様イ【直
流−14畳特性がiffられる。この1楊合、ギ〜・ツ
ブGが人さ゛くなるにつれて直流1畳特性曲線は11−
+ l)→CO)様な形となる。
1" Change in the current flowing through the coil (7Q)
] Ile's inductance [-?, rj. In this case, as Gi~tsubu G becomes less crowded, the DC 1 tatami characteristic curve becomes 11-
+ l)→CO).

ところで、従来第5図(a )に示1を様なタイプの磁
心どしては主にフエライ1〜−1−77がl[1いられ
、(b)の様な環状潜心(二はケイ系鋼\511−晶覧
合金が用いられでいる。、(7かし4家がら、これらの
磁心をスイッチング電源の出力ゝ■I謂用f−+−り」
イルとし−C用いた場合には、(1荷電流が小さいとさ
、すなわらチョーク電流が不連続のfl域のどきには出
力電圧が著しく上貸し、出力安定麻が悪くなるという問
題がある。このため、上記問題を解決覆るべく、負荷と
並列にダミーロードを接続し、チョークコイルに流れる
″電流が不連続とならない様に回路設計する方法や、軽
負伺時にはインダクタンスが大きく負荷電流が大きくな
るとインダクタンスが小さくなる様な非線形のヂ」−ク
コイルを用いイ)/J法が促某され(いる1、 しかしながら、部名のh法c(、よダミー冒−・−′4
、[不必要な電流を流ざイー1(〕ればならlJ’、(
七ごi乏少) ::j<ト好ましくない。一方、後前の
Jl−線形1− * −′7こ・〜(ハ、特開昭J 4
−50817 号公報、持回orイ、’)8  !T3
1113号公報、特開昭、58− 9070□1号へ、
907 + 0り:公報。
By the way, conventional magnetic cores of the type 1 shown in FIG. The 511-type steel alloy is used. (7 out of 4 types) These magnetic cores are used for the output of switching power supplies.
When using I-C, there is a problem that (if the current is small, that is, in the fl region where the choke current is discontinuous, the output voltage will increase significantly and the output stability will deteriorate). Therefore, in order to solve the above problem, we need to connect a dummy load in parallel with the load and design the circuit so that the current flowing through the choke coil does not become discontinuous, or when the load is lightly loaded, the inductance is large and the load current is The inductance becomes smaller when the inductance becomes smaller. "Use a quukil) / J law is urged (1, but the H -Law C (, dummy advice, dummy -′ '4 4)
, [If unnecessary current flows 1(], then lJ', (
7go i scarcity) ::j<t unfavorable. On the other hand, the front and rear Jl-linear 1-*-'7ko・~(ha, JP-A-Sho J 4
-50817 Publication, rotation or i, ') 8! T3
No. 1113, JP-A-Sho, No. 58-9070□1,
907+0ri: Publication.

特開昭59.−174109月公報、特開1lii 、
”+ り  17111 Q舅公報吉(ご2軟のものが
知られでいう。しかし、持1111tlG鴇 5081
7昂公報記載の発明cs−1と、1tの’A Y=”f
晶化することにより非線形チョークを作%=Jるしイ;
”) −であるが、ギャップvi度に問題が残るっまた
、特開[lR58−53813号公報記・戒のものi、
1F一部にギャップをイ1する磁心において、そのVV
ツブ付近に磁気特性の異なる2種以北の磁性1本を配置
したちのjであり、この方法によっても確かに非線形チ
ョークを得ることは可能T::あるが、構造が複雑にな
るという新たな問題点がある。
Japanese Patent Publication No. 1983. -17410 September Publication, Unexamined Patent Publication No. 1lii,
"+ ri 17111 Q-in-law Kohokichi (Go2 soft one is known. However, it is 1111tlG 5081
Invention cs-1 described in the 7th Publication and 1t'A Y=”f
Create a nonlinear choke by crystallizing it.
”) - However, there remains a problem with the gap vi degree.
In a magnetic core with a gap in part of 1F, its VV
It is possible to obtain a nonlinear choke with this method by placing one magnetic wire of two or more types with different magnetic properties near the knob, but it is possible to obtain a nonlinear choke, but there is a new problem in that the structure becomes complicated. There are some problems.

また、特開昭58−90704号〜90710号公報に
記載の発明においては「一部にギャップを有する磁心に
6いて、前記ギャップの近傍に実質的に非晶質よりなる
磁性簿lIりを添六たことを14徴とづ゛る・・・jも
のである。しかしながら、これらの発明によっても確か
に非線形チョークは(qられるものの非晶質合金薄帯は
比抵抗が小さいために、構造によっては渦電流損失に伴
なうギャップ近傍の発熱が問題となる。
Furthermore, in the inventions described in JP-A-58-90704 to Sho 58-90710, ``a magnetic core having a gap in a part is provided with a substantially amorphous magnetic book lI in the vicinity of the gap. However, even with these inventions, it is true that nonlinear chokes (q) have been developed, but because amorphous alloy ribbons have a small resistivity, their structure In this case, heat generation near the gap due to eddy current loss becomes a problem.

また特開昭59−171409号公報に記載の発明は「
磁心の一部に空隙を設(]、この空隙に磁心を形成する
磁性体よりも透V11!率の大きな磁性材でなる挿入部
材を配置して成る磁心]であり、上記発明においても非
線形チョークは(51られるが、挿入部材が金属の場合
にはやはりギャップ近傍の発熱が問題となる。
In addition, the invention described in JP-A-59-171409 is “
This is a magnetic core in which an air gap is provided in a part of the magnetic core (and an insertion member made of a magnetic material having a higher permeability V11! than the magnetic material forming the magnetic core is placed in this air gap), and the above invention also uses a nonlinear choke. (51) However, when the insertion member is made of metal, heat generation near the gap still becomes a problem.

また、特開昭59−、、、171110号公報に記載の
デそ明は「恒速磁率磁心と高透磁率磁心を磁気的に並列
回路を形成する様に配置し、これらに共通の巻線を施し
てなるもの」であり、この発明によっても非線形チョー
クを1ワることは可能(゛ある。しかし、構造上やや複
雑になるという問題点がある。
In addition, the method described in Japanese Unexamined Patent Publication No. 171110 is that ``a constant-velocity magnetic core and a high-permeability magnetic core are arranged so as to magnetically form a parallel circuit, and a common winding is connected to these cores. It is possible to use a nonlinear choke with this invention.However, there is a problem in that the structure is somewhat complicated.

[光用が解決しようとする問題点1 すなわら、非線形チョークコイルとしては上述した生着
に種々のタイプのものが1定業されているづく、いずれ
し−良一χOがあり、より構造が簡i17zかつ性能的
に優れた非線形チョーク用゛磁心が望まnでいた。
[Problem 1 to be solved by optics] In other words, there are various types of nonlinear choke coils that are used for the above-mentioned engraftment. A magnetic core for nonlinear chokes that is simple and has excellent performance was desired.

本発明の目的は、従来知られている非線形チ・ヨークコ
イルのもつ欠点を解決し、より構造が簡単でかつ性能的
に優れた非線形チョーク用磁心を提(共することにある
An object of the present invention is to solve the drawbacks of conventionally known nonlinear choke coils and to provide a magnetic core for a nonlinear choke that has a simpler structure and superior performance.

[問題点を解決するための手段) 」:足口的を達成するtこめに本発明名ら(3t(Φ’
? j’)非線形チョーク用磁心を設計し、1ift穴
を小わ1−51その結果、軟磁性材料により構成された
1llt 、11VJ) 一部にギャップを設け、前記
ギャップの全部もし・二(J一部に、固有抵抗が前記磁
心の固イj抵抗(こIヒベで光分人さな値をもつ軟磁性
材料から成る部材を−、ギセップスベーザとして挿入し
配置したことを14徴とする磁心が有用であることを見
出し、本5N明を完成したものである。
[Means for solving the problem]: The name of the present invention (3t(Φ'
? j') A magnetic core for a nonlinear choke was designed, and the 1ift hole was made of small 1-51. As a result, 1llt, 11VJ) A gap was provided in a part, and all of the gap was It is useful to use a magnetic core in which a member made of a soft magnetic material whose specific resistance is the same as that of the magnetic core is inserted and arranged as a Gisseps baser. He discovered that this is the case and completed the book 5N Ming.

本発明において、上記ギャップスベーりの固0抵抗は使
用する磁心材料により適宜選択されるが、一般に金属系
軟磁性材料からなる磁心を用いたときは、1Ω・am以
上であれば充分な効果を1qることができる。
In the present invention, the gap-based solid zero resistance is appropriately selected depending on the magnetic core material used, but generally when a magnetic core made of a metal-based soft magnetic material is used, a sufficient effect is obtained if it is 1 Ω・am or more. 1q can be obtained.

プなわら、第1図に示1ような構成の磁心において、磁
心1,1′およびギャップスペーサ3用軟磁性材わ1に
高透磁率材料を使用すれば軽負荷時には大きなインダク
タンスを示し、負荷電流が大きくなるとギャップスペー
サす3として使用した磁性材料が磁気的に飽和し、実質
的にその部分がエアギャップとなるためにインダクタン
スが急激に小さくなり、その結果第2図に示した様なL
−N1M性が得られる。ここで、インダクタンスの大き
さおよびギャップスペーサ用軟磁性材料が磁気飽和する
起磁力Nloの兼ね合いは、磁心とギャップスペーサ用
軟磁性材料の透磁率の大きさおよび各々の断面積比を適
切に選ぶことにより、種々のタイプの非線形チョークコ
イルが得られる。
However, if a high magnetic permeability material is used for the magnetic cores 1, 1' and the soft magnetic material 1 for the gap spacer 3 in a magnetic core configured as shown in Fig. 1, it will exhibit a large inductance at light loads, and the load will be reduced. As the current increases, the magnetic material used as the gap spacer 3 becomes magnetically saturated, and that part essentially becomes an air gap, resulting in a sudden decrease in inductance, resulting in L as shown in Figure 2.
-N1M property is obtained. Here, the balance between the inductance size and the magnetomotive force Nlo that causes the soft magnetic material for the gap spacer to magnetically saturate is determined by appropriately selecting the magnetic permeability of the magnetic core and the soft magnetic material for the gap spacer, and the cross-sectional area ratio of each. Various types of nonlinear choke coils can be obtained.

かかる構成の本発明による非線形チョークコイルは、従
来のものと比べて次の様な利点がある。
The nonlinear choke coil according to the present invention having such a configuration has the following advantages over conventional ones.

すなわち、第1図(b)の様な環状磁心では、ギャップ
幅を固定するために非磁性のギャップスペーサを挿入し
、接着剤により固定するのが普通であるが、本発明のも
のは非磁性のギャップスペーサのかわりに、固有抵抗の
大きな軟磁性体3′を配置することにより、ギャップを
固定する効果と、8穀な磁気特性を得る効果の双方が得
られ、構造上I2!甲であり、経済的にも好ましい。さ
らにギャップスペーサとして用いる軟磁性材料の固有抵
抗が大きいために、渦電流損失によるギャップ近傍の発
熱の問題が解決できる。
That is, in an annular magnetic core like the one shown in FIG. 1(b), a non-magnetic gap spacer is usually inserted and fixed with an adhesive to fix the gap width, but the one of the present invention uses a non-magnetic gap spacer. By arranging a soft magnetic material 3' with a high specific resistance in place of the gap spacer, it is possible to obtain both the effect of fixing the gap and the effect of obtaining excellent magnetic properties. It is also economically preferable. Furthermore, since the specific resistance of the soft magnetic material used as the gap spacer is high, the problem of heat generation near the gap due to eddy current loss can be solved.

また、これら磁心材料としては、パーマロイ。Permalloy is also used as the magnetic core material.

ケイ素鋼、非晶質合金組成々の磁性材料を用いることが
できるが、飽和磁束密度が大きく、かつ軟磁気特性に優
れ、鉄損の小さな非晶質合金を用いた場合には、さらに
好ましい結果を得る。
Although magnetic materials of various compositions such as silicon steel and amorphous alloy can be used, more favorable results can be obtained when using an amorphous alloy with a large saturation magnetic flux density, excellent soft magnetic properties, and low iron loss. get.

本発明の目的に最もふされしい非晶質合金組成としては
、次の様な組成である。
The most suitable amorphous alloy composition for the purpose of the present invention is as follows.

(Fe、clM 、 )、、、、x、 S iXByM
:Ni、C。
(Fe, clM, ),,,x, SiXByM
: Ni, C.

0≦× ≦15 7≦y ≦15 0くα≦ 0.5 ここでMは、チョークコイル用磁心として最も重要な性
質である飽和磁束密度を大きく損うことがなく、軟磁気
特性および耐蝕性を向上させ得る元素である。
0≦×≦15 7≦y≦15 0α≦0.5 Here, M is a material that does not significantly impair saturation magnetic flux density, which is the most important property for a choke coil magnetic core, and has soft magnetic properties and corrosion resistance. It is an element that can improve

ここでαは好ましくは0.1〜0.4であるが、O〈α
≦ 0.5であっても良い。
Here α is preferably 0.1 to 0.4, but O〈α
It may be ≦0.5.

σが0.5を越えると、飽和磁束密度および軟磁気特性
の両面から好ましくない。またα−〇では耐蝕性の点で
問題がある。
If σ exceeds 0.5, it is unfavorable from both saturation magnetic flux density and soft magnetic properties. Also, α-〇 has a problem in terms of corrosion resistance.

ギャップスペーサ用軟磁性材料としては、金属圧粉磁心
、フェライトなどが考えられるが、軟磁気特性に浸れか
つ加工性にも優れるフェライトを用いることがより好ま
しい。
As the soft magnetic material for the gap spacer, metal dust cores, ferrite, etc. can be considered, but it is more preferable to use ferrite, which has soft magnetic properties and is excellent in workability.

なお本発明において、環状磁心としては必ずしも貞円で
ある必要はなく、楕円あるいは矩形等の形状であっても
、全く同様の効果が1%られる。また、ギャップスペー
サ用磁心材料の厚さ、形状等についても必要な電気仕様
を満足すべく種々の形状が選択できることは言うまでも
ない。
In the present invention, the annular magnetic core does not necessarily have to be a chaste circle, and even if it has an elliptical or rectangular shape, the same effect of 1% can be obtained. Furthermore, it goes without saying that various shapes can be selected for the thickness, shape, etc. of the magnetic core material for the gap spacer in order to satisfy the necessary electrical specifications.

[実711!例〕 以下実施例に基づき本発明を説明する。[Real 711! example〕 The present invention will be explained below based on Examples.

実施例1 μmの非晶質合金薄帯を片ロール法により作製した。)
qられた薄帯ヲ巻回し外径351m、 内径20mm。
Example 1 A micrometer-thick amorphous alloy ribbon was produced by a single roll method. )
The rolled thin strip has an outer diameter of 351 m and an inner diameter of 20 mm.

厚さ10mff1の磁心を作製し、所定の熱処理を行っ
た。
A magnetic core with a thickness of 10 mff1 was prepared and subjected to prescribed heat treatment.

これにエポキシ系の樹脂を含浸し硬化させた後、砥石で
磁路の一部を切断し0.8mmのギャップを形成した。
After this was impregnated with epoxy resin and cured, a part of the magnetic path was cut using a grindstone to form a gap of 0.8 mm.

                 、このギャップ部
に形状が15x15x O,8t ll1mの第1表に
示す各種軟磁性板を挿入し、接着剤で固定した。
Various soft magnetic plates shown in Table 1 having a shape of 15x15x O, 8tll1m were inserted into this gap and fixed with an adhesive.

第1表 この磁心に:1−ディングを施し、イの1−に 1、O
mmφの7オルマール線を35回巻回し、非線彩のf−
ヨークコイルとした。
Table 1: Apply 1-ding to this magnetic core, and add 1, O to 1- of A.
A 7 mmφ Ormar wire is wound 35 times to form a non-linear f-
It was a yoke coil.

これらチョークの直流重畳特性を第3図に示す。Figure 3 shows the DC superimposition characteristics of these chokes.

図において、縦軸は単位巻数当りのインダクタンス値す
なわち1ターン当りのインダクタンス値(Am−VAL
UE)を示す。尚、横軸は磁化力であり、巻数Nおよび
電流■の積で示したものである。
In the figure, the vertical axis is the inductance value per unit number of turns, that is, the inductance value per turn (Am-VAL
UE). The horizontal axis is the magnetizing force, which is expressed as the product of the number of turns N and the current .

また、定格出力12V−5A、スイッチング周波数+0
0kl−1のスイツf−ング電源を使用し、1記y−(
−クニ]イルを・実装しlことさ゛の、磁心のV:ヤツ
!近傍の温度上r7を測定り、た。約20分放置後の値
を第1表に示す。
Also, rated output 12V-5A, switching frequency +0
Using a 0kl-1 SWITCH power supply,
V: That's the guy who implemented the magnetic core! Measure r7 above the nearby temperature. Table 1 shows the values after standing for about 20 minutes.

第3図かられかるように、これら(31いずれも井線形
ヂョーク特性を示すが、第1表かられかるように、本発
明の磁心は特にギt?ツブ近傍における温度上昇が小さ
く、電源効渠および信頼性の面−C極めて聞杓Cいるこ
とがわかる。
As can be seen from Fig. 3, all of these (31) exhibit straight-line jog characteristics, but as can be seen from Table 1, the magnetic core of the present invention has a particularly small temperature rise near the girt, and has a low power supply efficiency. It can be seen that the drain and reliability aspects are extremely difficult.

実施例2 次に磁心材料どし−(非晶質合金を使用しIに場合と、
比較材としてパーマロイ、ケイ素鋼1ノジよびノエライ
1−を使用した場合とで特性比較を行った。
Example 2 Next, the case where magnetic core materials (amorphous alloy is used for I),
Characteristics were compared with cases where permalloy, silicon steel 1-noji, and noelai 1- were used as comparative materials.

磁心形状および測定条件は、実施例1と同様である。(
ギャップスペーサには実施例1ど同じ]Jライトを用い
でいる) 第2表J3よび第4図にその結果を示す。
The magnetic core shape and measurement conditions are the same as in Example 1. (
The results are shown in Table 2 J3 and FIG. 4. The gap spacer is the same as in Example 1.

第2表 図および表から明らかなように、磁心材料がパーマロイ
およびケイ素鋼の場合には、直流重畳特性は比較釣車t
Jfであるが、ギャップ部の温度1臀が本発明の磁心と
比較して大きい。またフ丁ライ[・を用いた場合には、
温度上r?は良好イrるも、直流重畳特性が他の磁心と
比べて劣るため、磁心材料どしでは7tルフアスを用い
たものが府もQくバランスがとねCいる。。
As is clear from the figures and tables in Table 2, when the magnetic core material is permalloy or silicon steel, the DC superposition characteristic is
Jf, the temperature at the gap part is larger than that of the magnetic core of the present invention. In addition, when using Fuchorai [・,
Above temperature? Although the performance is good, the direct current superimposition characteristics are inferior compared to other magnetic cores, so when it comes to magnetic core materials, those using 7t Rufus have a poor balance. .

実施例3 次に磁心材料として用いる′)7tルーツノ・スの組成
ど飽和磁束密度Bs、fヤツ1部温度[−胃と耐蝕性の
評価を1°iっだ。
Example 3 Next, the composition of 7t roots used as the magnetic core material, the saturation magnetic flux density Bs, f, the temperature [-- and the corrosion resistance were evaluated by 1°i.

ヂj−り用材料としでは3sが1n<、耐蝕ゼlに優れ
るものほど使用し易い、、耐蝕”↑4の評価【、1、高
温高湿試験(60”C,80%Rl−、−4、4B+−
1>を()い、全くさびないものを5、全面さび/jも
のを1と()、5段階評価により行った。その結果を第
3表にシアくず。
As a material for dipping, 3s is less than 1n, the better the corrosion resistance, the easier it is to use, the evaluation of corrosion resistance ↑ 4 [, 1, high temperature and high humidity test (60"C, 80% Rl-, - 4, 4B+-
Evaluation was made on a five-point scale, with 1> being rated as (), 5 being no rust at all, and 1 being being completely rusted/j (). The results are shown in Table 3.

第3表 表から明らかなように、本発明合金は、飽和磁束密度が
高く、非線形チョークとしたときのギャップ部の温度上
昇が低く、耐蝕性にも優れ、チョーク用磁心材料として
好ましいことがわかる。
As is clear from Table 3, the alloy of the present invention has a high saturation magnetic flux density, a low temperature rise in the gap when used as a nonlinear choke, and excellent corrosion resistance, making it preferable as a magnetic core material for chokes. .

[発明の効果] 以上詳細に説明したように、本発明による磁心を用いた
非線形チョークコイルは、優れた非線形の直流重畳特性
をもち、特に高周波駆動のスイッチング電源の出力平滑
チョーク用として温度上背が小さく実用的価値は高い。
[Effects of the Invention] As explained in detail above, the nonlinear choke coil using the magnetic core according to the present invention has excellent nonlinear DC superposition characteristics, and is particularly suitable for use in output smoothing chokes of high-frequency driven switching power supplies. is small and has high practical value.

また本発明は、同様の設計によりフライバックコンバー
タのパワートランス等への応用も可能である。
Further, the present invention can also be applied to a power transformer of a flyback converter, etc. with a similar design.

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

第1図は本発明に係るチョークコイル用磁心の形状を示
す図、第2図は本発明による非線形チョークコイルの直
流重畳特性の例を示す図、第3図および第4図は本発明
の実施例における△L−VALUEの直流重畳特性を示
す図、第5図は従来のチョークコイル用磁心の形状を示
す図、第6図は従来のチョークコイルの直流重畳特性を
示す第7図 算2″回 パノI NI(791ツ メ/1(メ9γ〕
FIG. 1 is a diagram showing the shape of a magnetic core for a choke coil according to the present invention, FIG. 2 is a diagram showing an example of DC superposition characteristics of a nonlinear choke coil according to the present invention, and FIGS. 3 and 4 are diagrams showing an embodiment of the present invention. Figure 5 shows the shape of the conventional choke coil magnetic core. Figure 6 shows the DC bias characteristic of the conventional choke coil. Pano I NI (791 nails/1 (Me9γ)

Claims (1)

【特許請求の範囲】 1、軟磁性材料により構成された環状磁心の一部にギャ
ップを設け、前記ギャップの全部もしくは一部に固有抵
抗が前記磁心の固有抵抗に比べて充分大きい値をもつ軟
磁性材料から成るギャップスペーサを挿入したことを特
徴とする磁心。 2、上記磁心を構成する磁性材料が非晶質合金から成る
ことを特徴とする特許請求の範囲第1項記載の磁心。 3、上記非晶質合金の組成が、 (Fe_1_−_αM_α)_1_0_0_−_x_−
_ySi_xB_yただし、M=Ni、Coのうちの1
種または2種0≦x≦15 7≦y≦15 0≦α≦0.5 であることを特徴とする特許請求の範囲第2項記載の磁
心。 4、上記ギャップスペーサとして軟磁性フェライト材料
を用いことを特徴とする特許請求の範囲第1項乃至第3
項のいずれかに記載の磁心。
[Scope of Claims] 1. A gap is provided in a part of the annular magnetic core made of a soft magnetic material, and all or part of the gap is made of a soft magnetic material whose specific resistance is sufficiently larger than that of the magnetic core. A magnetic core characterized in that a gap spacer made of a magnetic material is inserted. 2. The magnetic core according to claim 1, wherein the magnetic material constituting the magnetic core is made of an amorphous alloy. 3. The composition of the amorphous alloy is (Fe_1_−_αM_α)_1_0_0_−_x_−
_ySi_xB_y However, M = 1 of Ni, Co
3. The magnetic core according to claim 2, characterized in that species or two species 0≦x≦15 7≦y≦15 0≦α≦0.5. 4. Claims 1 to 3, characterized in that a soft magnetic ferrite material is used as the gap spacer.
The magnetic core described in any of paragraphs.
JP60045837A 1985-03-08 1985-03-08 Magnetic core Pending JPS61204908A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60045837A JPS61204908A (en) 1985-03-08 1985-03-08 Magnetic core

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60045837A JPS61204908A (en) 1985-03-08 1985-03-08 Magnetic core

Publications (1)

Publication Number Publication Date
JPS61204908A true JPS61204908A (en) 1986-09-11

Family

ID=12730332

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60045837A Pending JPS61204908A (en) 1985-03-08 1985-03-08 Magnetic core

Country Status (1)

Country Link
JP (1) JPS61204908A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62211910A (en) * 1986-03-13 1987-09-17 Toshiba Corp Manufacture of magnetic core
KR100518677B1 (en) * 1997-03-18 2005-10-05 메트글라스, 인코포레이티드 Electrical choke

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62211910A (en) * 1986-03-13 1987-09-17 Toshiba Corp Manufacture of magnetic core
KR100518677B1 (en) * 1997-03-18 2005-10-05 메트글라스, 인코포레이티드 Electrical choke

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