JPS6119097B2 - - Google Patents

Info

Publication number
JPS6119097B2
JPS6119097B2 JP56010836A JP1083681A JPS6119097B2 JP S6119097 B2 JPS6119097 B2 JP S6119097B2 JP 56010836 A JP56010836 A JP 56010836A JP 1083681 A JP1083681 A JP 1083681A JP S6119097 B2 JPS6119097 B2 JP S6119097B2
Authority
JP
Japan
Prior art keywords
magnetic
soft magnetic
current
magnetic body
inductance element
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
Application number
JP56010836A
Other languages
Japanese (ja)
Other versions
JPS57126109A (en
Inventor
Akio Nakamura
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.)
TDK Corp
Original Assignee
TDK 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 TDK Corp filed Critical TDK Corp
Priority to JP1083681A priority Critical patent/JPS57126109A/en
Publication of JPS57126109A publication Critical patent/JPS57126109A/en
Publication of JPS6119097B2 publication Critical patent/JPS6119097B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F17/00Fixed inductances of the signal type 
    • H01F17/04Fixed inductances of the signal type  with magnetic core

Description

【発明の詳細な説明】 (技術分野) 本発明は、スイツチングレギユレータ等に使用
するのに適したインダクタンス素子に関する。
DETAILED DESCRIPTION OF THE INVENTION (Technical Field) The present invention relates to an inductance element suitable for use in switching regulators and the like.

(発明の背景) 従来、チヨークコイル等のインダクタンス素子
において脈動電圧を平滑する場合、平滑電流の小
さい値から大きい値まで第1図の如くほぼ一定の
インダクタンスを有することが必要であると考
え、インダクタンスが大きくかつ磁心を軟磁性体
で構成して飽和電流を平滑電流最大値より大きく
なる如く設計したインダクタンス素子を用いてい
た。しかし、これでは、インダクタンス素子の寸
法がLI2(Lはインダクタンス、Iは飽和電流)
にほぼ比例することから大形となつてしまう欠点
がある。
(Background of the Invention) Conventionally, when smoothing a pulsating voltage in an inductance element such as a chiyoke coil, it has been thought that it is necessary to have an almost constant inductance as shown in Figure 1 from a small value to a large value of the smoothed current. An inductance element was used that was large, had a magnetic core made of a soft magnetic material, and was designed so that the saturation current was larger than the maximum value of the smoothed current. However, in this case, the dimensions of the inductance element are LI 2 (L is the inductance, I is the saturation current)
Since it is almost proportional to , it has the disadvantage of becoming large.

(従来技術) そのため、磁気回路をEI磁心で構成し、その
中央磁脚に空隙を設けて、ある程度以上電流が大
きい場合でも磁心が飽和しないようにして小形化
を図ることが提案されている。しかし、それでは
E型磁心として規格品を使用することができず加
工がめんどうであり、かつ所定の特性が得られる
ように調整、設定することが困難である。さら
に、中央磁脚に空隙を設けることは磁気回路の磁
気抵抗が増加し、低電流領域でのインダクタンス
が空隙のない場合よりも低下してしまう欠点が生
じる。
(Prior Art) Therefore, it has been proposed to configure the magnetic circuit with an EI magnetic core and provide an air gap in the central magnetic leg to prevent the magnetic core from being saturated even when the current is large beyond a certain level, thereby reducing the size of the magnetic circuit. However, in this case, it is not possible to use a standard product as the E-type magnetic core, and processing is troublesome, and it is difficult to adjust and set so as to obtain predetermined characteristics. Furthermore, providing an air gap in the central magnetic leg increases the magnetic resistance of the magnetic circuit, resulting in a disadvantage that the inductance in a low current region is lower than when there is no air gap.

さらに、磁心の空隙に永久磁石を設けて磁気バ
イアスを与えるインダクタンス素子が特公昭54−
5501号、実公昭54−7319号、特公昭54−32696号
において提示されているが、永久磁石を用いるた
めコスト高となり、かつ永久磁石の発熱等の問題
もある。
Furthermore, an inductance element that provided a magnetic bias by installing a permanent magnet in the air gap of the magnetic core was developed in the 1970s.
No. 5501, Japanese Utility Model Publication No. 54-7319, and Japanese Patent Publication No. 54-32696, but since permanent magnets are used, the cost is high and there are problems such as heat generation of the permanent magnets.

(発明の目的) 本発明の目的は、上記従来の欠点をなくし、脈
動電圧の平滑等に適した小形のインダクタンス素
子を提供することにある。
(Objective of the Invention) An object of the present invention is to eliminate the above-mentioned conventional drawbacks and to provide a small inductance element suitable for smoothing pulsating voltage.

(発明の構成の要点) 本発明の特徴は、中央磁脚及び側磁脚を有する
第1の磁心と、それらの磁脚に対接する第2の磁
心とを組合わせた磁心組立体において、第2の磁
心を前記第1の磁心に直接接する第1の磁性体
と、これに非磁性層を介して対向する第2の磁性
体とに分割した点にある。
(Main points of the structure of the invention) A feature of the present invention is that in a magnetic core assembly that combines a first magnetic core having a central magnetic leg and side magnetic legs, and a second magnetic core that is in contact with these magnetic legs, The second magnetic core is divided into a first magnetic body that is in direct contact with the first magnetic core, and a second magnetic body that is opposed to the first magnetic body with a nonmagnetic layer interposed therebetween.

(発明の実施例) 以下、本発明に係るインダクタンス素子の実施
例を図面に従つて説明する。
(Embodiments of the Invention) Hereinafter, embodiments of an inductance element according to the present invention will be described with reference to the drawings.

第2図は本発明の第1実施例を示す。この図に
おいて、インダクタンス素子は、E型軟磁性体1
と2つのI型軟磁性体2,3とでEI磁心を形成
し、I型軟磁性体2,3間に非磁性体、空隙等の
非磁性層4を設け、E型軟磁性体の中央磁脚1a
に巻線5を施したものである。ここで、I型軟磁
性体2はE型軟磁性体1の中央磁脚1a及び側磁
脚1bに直接対接し、好ましくは磁性体1,3よ
り充分大きな透磁率のものであり、I型軟磁性体
3は非磁性層4を介してI型軟磁性体2に構造的
に一体化される。
FIG. 2 shows a first embodiment of the invention. In this figure, the inductance element is an E-type soft magnetic material 1
and the two I-type soft magnetic bodies 2 and 3 form an EI magnetic core, and a non-magnetic layer 4 such as a non-magnetic material or an air gap is provided between the I-type soft magnetic bodies 2 and 3, and the center of the E-type soft magnetic body is Magnetic leg 1a
A winding 5 is applied to the wire. Here, the I-type soft magnetic body 2 is in direct contact with the central magnetic leg 1a and the side magnetic leg 1b of the E-type soft magnetic body 1, and preferably has a sufficiently larger magnetic permeability than the magnetic bodies 1 and 3. The soft magnetic body 3 is structurally integrated with the I-type soft magnetic body 2 via the nonmagnetic layer 4.

次に上記第1実施例の動作を、第3図の動作図
及び第4図の特性図とともに説明する。ただし、
E型及びI型軟磁性体1,2,3を東京電気化学
工業株式会社製EI−30型の同一特性のフエライ
ト磁心とし、E型軟磁性体1は規格品、I型軟磁
性体2は厚さ1mm、I型軟磁性体3は厚さ4mmと
し、非磁性層4は1mmとした。
Next, the operation of the first embodiment will be explained with reference to the operation diagram in FIG. 3 and the characteristic diagram in FIG. 4. however,
The E-type and I-type soft magnetic bodies 1, 2, and 3 are ferrite cores of the same characteristics as EI-30 manufactured by Tokyo Denki Kagaku Kogyo Co., Ltd., and the E-type soft magnetic body 1 is a standard product and the I-type soft magnetic body 2 is a standard product. The thickness was 1 mm, the I-type soft magnetic body 3 was 4 mm thick, and the nonmagnetic layer 4 was 1 mm thick.

さて、動作は大別して電流の小さい1A未満の
領域と、電流がそれより大きい領域とに分離され
る。まず、電流が小さい領域では、巻線5による
磁束φiは2つのI型軟磁性体2,3のうち、磁
性体2の方を通ることになり、インダクタンスは
大きな値(約500μH)となる。
Now, the operation can be roughly divided into a region where the current is small, less than 1A, and a region where the current is larger. First, in a region where the current is small, the magnetic flux φi due to the winding 5 passes through the magnetic body 2 of the two I-type soft magnetic bodies 2 and 3, and the inductance becomes a large value (approximately 500 μH).

次に巻線5に流れる電流が大きく(1A以上)
になつた場合は、磁束φiが多くなり、I型軟磁
性体2を通る磁束も多くなる。この結果、I型軟
磁性体2は薄い板状であるため、その飽和磁束密
度を超えることになり、I型軟磁性体2の部分の
磁気抵抗は磁性体が存在しない状態と等価とな
る。これにより、実質的にはE型軟磁性体1とI
型軟磁性体3とから成る大きな等価的空隙Gを有
するEI磁心となり、インダクタンス素子は小さ
な値(約150μH)となる。この状態は、巻線5
による磁束φlがI型軟磁性体3を通るようにな
つてから、20Aを超える電流による磁束でI型軟
磁性体3の飽和磁束密度を超えるまで続くことに
なる。
Next, the current flowing through winding 5 is large (1A or more)
When it becomes , the magnetic flux φi increases, and the magnetic flux passing through the I-type soft magnetic body 2 also increases. As a result, since the I-type soft magnetic body 2 has a thin plate shape, its saturation magnetic flux density will be exceeded, and the magnetic resistance of the I-type soft magnetic body 2 will be equivalent to the state where no magnetic body exists. As a result, the E-type soft magnetic body 1 and I
The EI magnetic core has a large equivalent air gap G formed by the soft magnetic material 3, and the inductance element has a small value (approximately 150 μH). In this state, winding 5
After the magnetic flux φl starts to pass through the I-type soft magnetic body 3, it continues until the magnetic flux due to the current exceeding 20 A exceeds the saturation magnetic flux density of the I-type soft magnetic body 3.

以上説明したように、上記第1実施例によれ
ば、平滑電流の小さい領域では大きなインダクタ
ンス値を、平滑電流の大きな領域では小さなイン
ダクタンス値を得ることができ、小形でスイツチ
ングレギユレータ等に適したインダクタンス素子
を実現できる。また、I型軟磁性体2,3の厚み
を変えることにより任意の特性を得ることができ
る。さらに、スイツチングレギユレータに用いれ
ば、負荷が軽負荷の場合チヨークコイルに流れる
電流が不連続となり、フイルタ効果を失う事にな
るが、その電流を臨界電流IULとして、 IUL≧Ein−Eout/2L・tON (ただし、Ein:入力直流電圧、Eout:出力直
流電圧、tON:トランジスタのオン時間、L:チ
ヨークコイルのインダクタンス) であることが必要である。従つて、スイツチング
レギユレータでは臨界電流IULを超えさせるた
め、通常ダミー抵抗を出力端に接続し、ダミー電
流を流している。しかし、本発明のインダクタン
ス素子は軽負荷でのインダクタンスが大きいので
臨界電流IULは少なくて良いこととなる。この結
果、ダミーロードを減らして効率の改善を図るこ
とが可能である。
As explained above, according to the first embodiment, a large inductance value can be obtained in a region where the smoothed current is small, and a small inductance value can be obtained in a region where the smoothed current is large. A suitable inductance element can be realized. Moreover, by changing the thickness of the I-type soft magnetic bodies 2 and 3, arbitrary characteristics can be obtained. Furthermore, if used in a switching regulator, when the load is light, the current flowing through the choke coil will be discontinuous and the filter effect will be lost, but if this current is defined as the critical current IUL , then IUL ≧Ein-Eout /2L·t ON (where, Ein: input DC voltage, Eout: output DC voltage, t ON : transistor on time, L: inductance of the choke coil). Therefore, in a switching regulator, in order to exceed the critical current IUL , a dummy resistor is usually connected to the output terminal to flow a dummy current. However, since the inductance element of the present invention has a large inductance under light loads, the critical current I UL may be small. As a result, it is possible to reduce the dummy load and improve efficiency.

第5図は本発明の第2実施例を示す。この図に
おいて、インダクタンス素子は、軟磁性体のポツ
ト型磁心10と円板状磁心を2分割した2つの円
板状軟磁性体11,12とで磁気回路を構成し、
円板状軟磁性体11,12間に非磁性体、空隙等
の非磁性層13を設け、ポツト型磁心10の中央
磁脚10aに巻線14を施したものである。ここ
で、円板状軟磁性体11はポツト型磁心10の中
央磁脚10a及び円筒状側磁脚10bに直接対接
し、円板状軟磁性体12は非磁性層13を介して
円板状軟磁性体11に構造的に一体化される。
FIG. 5 shows a second embodiment of the invention. In this figure, the inductance element constitutes a magnetic circuit with a pot-shaped magnetic core 10 made of soft magnetic material and two disc-shaped soft magnetic materials 11 and 12 that are divided into two disc-shaped magnetic cores.
A non-magnetic layer 13 such as a non-magnetic material or an air gap is provided between the disc-shaped soft magnetic bodies 11 and 12, and a winding 14 is provided on the central magnetic leg 10a of the pot-shaped magnetic core 10. Here, the disc-shaped soft magnetic body 11 is in direct contact with the central magnetic leg 10a and the cylindrical side magnetic leg 10b of the pot-shaped magnetic core 10, and the disc-shaped soft magnetic body 12 is connected to the disc-shaped soft magnetic body 12 through the nonmagnetic layer 13. It is structurally integrated with the soft magnetic body 11.

上記の第2実施例においても、円板状軟磁性体
11が飽和するまでは高インダクタンス値を、そ
れ以上の電流では小さなインダクタンス値を示
し、前述の第1実施例と同様の効果を上げること
ができる。
The second embodiment described above also exhibits a high inductance value until the disc-shaped soft magnetic body 11 is saturated, and exhibits a small inductance value when the current exceeds that value, thereby achieving the same effect as the first embodiment described above. I can do it.

(発明の効果) 叙上のように、本発明によれば、電流の小さい
領域では大きなインダクタンス値を、電流の大き
な領域では小さなインダクタンス値を得ることが
でき、小形でスイツチングレギユレータ等に適し
たインダクタンス素子を実現できる。
(Effects of the Invention) As described above, according to the present invention, it is possible to obtain a large inductance value in a small current region and a small inductance value in a large current region, making it possible to obtain a small inductance value for a switching regulator, etc. A suitable inductance element can be realized.

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

第1図は従来のインダクタンス素子の電流とイ
ンダクタンスとの関係を示す特性図、第2図は本
発明に係るインダクタンス素子の第1実施例を示
す斜視図、第3図は同動作図、第4図は第1実施
例の場合の電流とインダクタンスとの関係を示す
特性図、第5図は本発明の第2実施例を示す分解
斜視図である。 1……E型軟磁性体、2,3……I型軟磁性
体、4,13……非磁性層、5,14……巻線、
10……ポツト型磁心、11,12……円板状軟
磁性体。
FIG. 1 is a characteristic diagram showing the relationship between current and inductance of a conventional inductance element, FIG. 2 is a perspective view showing a first embodiment of the inductance element according to the present invention, FIG. 3 is a diagram of the same operation, and FIG. The figure is a characteristic diagram showing the relationship between current and inductance in the case of the first embodiment, and FIG. 5 is an exploded perspective view showing the second embodiment of the present invention. 1... E type soft magnetic material, 2, 3... I type soft magnetic material, 4, 13... Nonmagnetic layer, 5, 14... Winding wire,
10... Pot-shaped magnetic core, 11, 12... Disc-shaped soft magnetic material.

Claims (1)

【特許請求の範囲】 1 中央磁脚及び側磁脚を有する第1の磁心と、
それらの磁脚に対接する第2の磁心とを組合わせ
て磁気回路を構成し、前記中央磁脚に巻線を施し
たインダクタンス素子において、前記第2の磁心
を前記第1の磁心の中央磁脚及び側磁脚に直接接
する第1の磁性体と、これに非磁性層を介して対
向する第2の磁性体とで構成したことを特徴とす
るインダクタンス素子。 2 前記第1の磁性体が、前記第1の磁心及び第
2の磁性体よりも透磁率の高い軟磁性体である特
許請求の範囲第1項記載のインダクタンス素子。
[Claims] 1. A first magnetic core having a central magnetic leg and side magnetic legs;
In an inductance element in which a magnetic circuit is configured by combining these magnetic legs with a second magnetic core that is in contact with the magnetic legs, and a wire is wound around the central magnetic leg, the second magnetic core is connected to the central magnetic core of the first magnetic core. An inductance element comprising a first magnetic body in direct contact with a leg and a side magnetic leg, and a second magnetic body facing the first magnetic body with a nonmagnetic layer interposed therebetween. 2. The inductance element according to claim 1, wherein the first magnetic body is a soft magnetic body having higher magnetic permeability than the first magnetic core and the second magnetic body.
JP1083681A 1981-01-29 1981-01-29 Inductance element Granted JPS57126109A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1083681A JPS57126109A (en) 1981-01-29 1981-01-29 Inductance element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1083681A JPS57126109A (en) 1981-01-29 1981-01-29 Inductance element

Publications (2)

Publication Number Publication Date
JPS57126109A JPS57126109A (en) 1982-08-05
JPS6119097B2 true JPS6119097B2 (en) 1986-05-15

Family

ID=11761431

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1083681A Granted JPS57126109A (en) 1981-01-29 1981-01-29 Inductance element

Country Status (1)

Country Link
JP (1) JPS57126109A (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60141111U (en) * 1983-04-21 1985-09-18 株式会社トーキン nonlinear inductance element
JPS63162517U (en) * 1987-04-10 1988-10-24
US5815062A (en) * 1995-06-30 1998-09-29 Hitachi Metal, Ltd. Magnetic core
DE60137058D1 (en) * 2000-09-20 2009-01-29 Det Int Holding Ltd PLANAR INDUCTIVE ELEMENT
JP2002134328A (en) * 2000-10-20 2002-05-10 Nippon Koden Corp Coil
JP5474893B2 (en) * 2010-08-31 2014-04-16 サムソン エレクトロ−メカニックス カンパニーリミテッド. Inductor integrated transformer

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5136564A (en) * 1974-09-24 1976-03-27 Hitachi Metals Ltd INDAKUTAA
JPS5254938A (en) * 1975-10-31 1977-05-04 Sony Corp Switching regulator

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5136564A (en) * 1974-09-24 1976-03-27 Hitachi Metals Ltd INDAKUTAA
JPS5254938A (en) * 1975-10-31 1977-05-04 Sony Corp Switching regulator

Also Published As

Publication number Publication date
JPS57126109A (en) 1982-08-05

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