JPH01125809A - Magnetic core for variable inductor - Google Patents

Magnetic core for variable inductor

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Publication number
JPH01125809A
JPH01125809A JP28443687A JP28443687A JPH01125809A JP H01125809 A JPH01125809 A JP H01125809A JP 28443687 A JP28443687 A JP 28443687A JP 28443687 A JP28443687 A JP 28443687A JP H01125809 A JPH01125809 A JP H01125809A
Authority
JP
Japan
Prior art keywords
magnetic core
magnetic
core
inductance
gap
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
JP28443687A
Other languages
Japanese (ja)
Inventor
Kenji Sugawara
菅原 賢司
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.)
Tokin Corp
Original Assignee
Tokin 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 Tokin Corp filed Critical Tokin Corp
Priority to JP28443687A priority Critical patent/JPH01125809A/en
Publication of JPH01125809A publication Critical patent/JPH01125809A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain the choke coil having excellent DC superpositional characteristics by a method wherein a small-sized magnetic core, having the magnetic characteristics different from those of the magnetic main body, is inserted into a part of a gap section. CONSTITUTION:An air gap 3 is provided in advance on the whole surface of the butt-together part of a magnetic core, and a small type magnetic core 21 having the magnetic characteristics different from those of the main body magnetic core 1 is separately inserted into said air gap part 3. Accordingly, high inductance L can be obtained in a feeble magnetic field, and on the part having an intensive superposed DC magnetic field, the choke coil having the inductance characteristics equal to the inductance provided with the ordinary air-gap for the product of a superposed DC current and the number of the coil, is constituted. As a result, excellent DC superpositional characteristics can be obtained.

Description

【発明の詳細な説明】 〔分野の概要〕 本発明は、スイッチング電源に使用し二次側回路の直流
重畳電流に対し、非直線インダクタンス特性を持つイン
ダクタとして使用するチョークコイルに用いる磁心に関
するものである。
[Detailed Description of the Invention] [Overview of the Field] The present invention relates to a magnetic core used in a choke coil used in a switching power supply as an inductor having non-linear inductance characteristics against DC superimposed current in a secondary circuit. be.

〔従来技術の内容と間屈点〕[Contents of conventional technology and points of compromise]

従来この種の磁心は、EE型、EI型等の場合は、中脚
接合部の空隙の一部に磁路を階段状に磁心突き合わせ部
を設けることにより、弱磁界では空隙部の磁心突き合わ
せ部は飽和せず実効的な透磁率μeを高くし、強磁界で
は磁心突き合わせ部は飽和し、実効的な磁路全面に空隙
が挿入されたと同じ透磁率μegとなる磁心が用いられ
ている。
Conventionally, in the case of the EE type, EI type, etc., this type of magnetic core has a step-shaped magnetic path in a part of the air gap of the middle leg joint, so that the magnetic core abutment part in the air gap is formed in a weak magnetic field. A magnetic core is used in which the effective magnetic permeability μe is increased without being saturated, and the abutting portion of the magnetic cores is saturated in a strong magnetic field, resulting in the same magnetic permeability μeg as if an air gap was inserted over the entire effective magnetic path.

しかし、特性面では空隙部の磁心突き合わせ部が飽和す
ると、磁心本体の中脚平坦空隙部の一部まで飽和するた
め、直流重畳磁界の値を示すコイルの巻数Nと、コイル
電流工の積NI即ちアンペアターンに対するインダクタ
ンスの値が、磁心中脚全面に空隙を設けた時にインダク
タの値が平坦な特性を示すインダクタと比較し、直流重
畳磁界に対するインダクタンスの値がNIの値に対し高
い方へ伸びないこと、及び研削加工による階段状磁路を
作る磁心突き合わせ部の寸法管理が難しく扱いにくいと
いう欠点があった。
However, in terms of characteristics, when the core abutting part in the air gap is saturated, a part of the middle leg flat gap part of the core body is also saturated, so the product NI of the coil turns N, which indicates the value of the DC superimposed magnetic field, and the coil current In other words, compared to an inductor whose inductance value is flat when an air gap is provided over the entire surface of the center leg of the magnetic core, the inductance value for ampere turns increases to a higher value than the NI value. There were disadvantages in that it was difficult to control the dimensions of the magnetic core abutting portions that created the step-like magnetic path by grinding, and it was difficult to handle.

〔発明の目的〕[Purpose of the invention]

本発明は、これらの欠点を除去するため、磁心突き合わ
せ部全面に予め空隙を設け、その空隙部に本体磁心の磁
気特性と特性の異なる小型磁心を別途に挿入することに
より、弱磁界ではインダクタンスLを高く得ることが出
来、重畳する直流磁界の強い所では、重畳する直流電流
とコイル巻数との積に対して1通常の空隙を設けたイン
ダクタと同等のインダクタンスの特性を持ったチョーク
コイルを構成するものである。
In order to eliminate these drawbacks, the present invention provides a gap in advance over the entire surface of the magnetic core abutting part, and separately inserts a small magnetic core with different magnetic properties from the main body magnetic core into the gap, thereby reducing the inductance L in a weak magnetic field. In places where the superimposed DC magnetic field is strong, a choke coil is constructed that has the same inductance characteristics as an inductance with a normal air gap of 1 for the product of the superimposed DC current and the number of turns of the coil. It is something to do.

〔発明の構成〕[Structure of the invention]

本発明の磁心は、予め磁心中脚に空隙を設けておき、本
体の磁心と磁気特性の異なる小形磁心を空隙部に接着し
、磁心突き合わせ面を研磨加工し目的とする磁心を構成
するか、最終焼結前の磁心の粉体プレス時に、特性の異
なる材料のチップを予め本体磁心と一体でプレス成型し
、後焼結して一体化し、磁心突き合わせ面を研削し本発
明の磁心とし、磁心の磁路に空隙を設けた可変インダク
タ用磁心に於て、空隙部に磁心本体と異なる磁気特性の
小型磁心を挿入し組立てた構造とした可変インダクタ用
磁心とするものである。
In the magnetic core of the present invention, an air gap is provided in the center leg of the magnetic core in advance, a small magnetic core having different magnetic properties from the magnetic core of the main body is adhered to the air gap, and the abutting surfaces of the magnetic cores are polished to form the intended magnetic core. During the powder pressing of the magnetic core before final sintering, chips of materials with different characteristics are press-molded in advance with the main body magnetic core, and then sintered and integrated, and the abutting surfaces of the magnetic cores are ground to form the magnetic core of the present invention. This magnetic core for a variable inductor has a structure in which a small magnetic core having magnetic characteristics different from that of the core body is inserted into the gap and assembled into the gap.

〔実施例〕 本発明の実施例を図面を用い説明する。〔Example〕 Embodiments of the present invention will be described with reference to the drawings.

第5図は、スイッチング電源の二次側直流平滑回路に使
用されている一般的なチョー・クコイル用磁心の形状で
あり、(a)はEE型磁心1を用いた場合、(b)はE
I型磁心1と2を用いた場合で中脚゛に空隙3を設けて
あり、これら磁心は、中脚部分に入るコイルボビンにコ
イルを巻回してチョークコイルを構成している。従来一
般的に使われているこれら形状の磁心を用いたチョーク
コイルの特性は第4図に示す特性を示し、チョークコイ
ルに重畳する直流電流Iと、コイルの巻数Nとの積NI
に対するインダクタンスLの値は、NIの値が零部分か
ら磁心が飽和する迄はぼ一定のインダクタンスの値を示
す。
Figure 5 shows the shape of a general choke coil magnetic core used in the secondary side DC smoothing circuit of a switching power supply.
When I-type magnetic cores 1 and 2 are used, a gap 3 is provided in the middle leg, and these cores constitute a choke coil by winding a coil around a coil bobbin that enters the middle leg. The characteristics of conventionally commonly used choke coils using magnetic cores of these shapes are shown in Figure 4, where the product NI of the DC current I superimposed on the choke coil and the number of turns N of the coil is
The value of inductance L for NI is approximately constant from the zero value of NI until the magnetic core is saturated.

一方、スイッチング電源の二次側直流平滑回路に使用す
るチョークコイルの特性は、安定な制御特性を得るため
には直流電流の値が小さい時にはチョークコイルとして
高いインダクタンスの値を必要とし、このため最近では
第3図に示す磁心中脚部の空隙3の部分に、中脚の一部
に階段状磁路4の突き合わせ部を設け、その先端は対向
するE型、1型コアの面に接し突き合わせる形状とした
磁心としチョークコイル用の磁心を構成し用いている。
On the other hand, the characteristics of choke coils used in the secondary side DC smoothing circuit of switching power supplies require a high inductance value as a choke coil when the value of DC current is small in order to obtain stable control characteristics. Now, in the part of the air gap 3 of the central leg of the magnetic core shown in Fig. 3, an abutting part of a stepped magnetic path 4 is provided in a part of the middle leg, and its tip touches and butts against the facing surfaces of the E-type and 1-type cores. The magnetic core is shaped like this, and is used to construct a magnetic core for a choke coil.

第3図に示す形状の磁心を用いたチョークコイルの特性
は、第6図Bの特性曲線を示し、直流重畳電流の小さい
値の部分では従来形状の磁心を用いた場合に比べてイン
ダクタンスの値は高くなったが、従来の同じ空隙長を持
つ磁心の直流重畳特性、第6図Cの特性に比べて直流重
畳電流の大きい部分ではインダクタンスが低くなると言
う問題があった。これは第3図(a)(b)の磁心に於
て、階段状磁路4の突き合わせ部に続く磁心中脚A(ハ
ツチングで示す部分)の部分が直流重畳電流の4αが大
きくなった時、階段状磁路4の磁気飽和領域Aの部分が
等価的に空隙長を長くするためと考えられる。
The characteristics of the choke coil using the magnetic core of the shape shown in Figure 3 show the characteristic curve of Figure 6B, and in the portion where the DC superimposed current is small, the inductance value is higher than when using the magnetic core of the conventional shape. However, there was a problem in that the inductance was lower in the portion where the DC superimposition current was large compared to the DC superimposition characteristics of the conventional magnetic core with the same gap length, the characteristics shown in FIG. 6C. In the magnetic core shown in Fig. 3 (a) and (b), when the DC superimposed current 4α becomes large in the central leg A (the hatched part) following the butt part of the stepped magnetic path 4. This is considered to be because the magnetic saturation region A portion of the stepped magnetic path 4 equivalently increases the air gap length.

叙上の問題点を解消するため本発明では第1図の磁心構
造とするもので、第1図に於て磁心中脚の空隙部3の部
分に、磁心1と異なる特性を持つ磁心21を挿入した構
造とするものである。
In order to solve the above-mentioned problems, the present invention adopts the magnetic core structure shown in FIG. 1. In FIG. This is the inserted structure.

以下余白 実施例−1 スイッチング電源のチョークコイルに使用する磁心材料
の、透磁率μが2500.飽和磁束密度が5000力゛
ウスのMn−Znフェライト(東北金属工業製2500
B材)のEI型コアFEI−28(幅28mm、長さ■
型コアを含め20mm、厚さ11mm)を用い、コイル
ボビンに巻線を100回巻きEIココア中脚に挿入した
Below is a blank Example-1 The magnetic permeability μ of the magnetic core material used for the choke coil of a switching power supply is 2500. Mn-Zn ferrite with a saturation magnetic flux density of 5000 forces (Tohoku Metal Industry Co., Ltd. 2500
B material) EI type core FEI-28 (width 28 mm, length ■
Using a coil bobbin (20 mm including the mold core and 11 mm thick), the wire was wound 100 times around a coil bobbin and inserted into the middle leg of the EI cocoa.

本体磁心は第5図(b)の構造で、空隙長さ1.9mm
とした。
The main body magnetic core has the structure shown in Fig. 5(b), and the air gap length is 1.9 mm.
And so.

此の構造の磁心を用いた時の直流重畳特性は、第2図の
曲1M Kの通りである。横軸NIは、■は直流重畳電
流の値でアンペアを表し、Nはコイル巻数を示す。又、
縦軸ALはコイルボビンたりのインダクタンスの値を示
す。
The DC superposition characteristics when using a magnetic core with this structure are as shown in curve 1MK in Fig. 2. On the horizontal axis NI, ■ represents the DC superimposed current value in ampere, and N represents the number of coil turns. or,
The vertical axis AL indicates the value of inductance per coil bobbin.

実施例−2 実施例−1と同じく、本体磁心材料はフェライトの25
00B材で、第3図(a)の形状に加工したEIココア
寸法は実施例−1と同じ寸法とし、中脚の空隙長は1.
9mm、階段部の幅は1.0mmとした。此のコアは階
段部はコア本体と一体で作られており、従来使われてい
る構造のコアと同じである。
Example-2 Same as Example-1, the main body magnetic core material is ferrite 25
The dimensions of the EI cocoa made of 00B material and processed into the shape shown in FIG. 3(a) are the same as in Example-1, and the gap length of the middle leg is 1.
The width of the step part was 1.0 mm. The staircase part of this core is made integral with the core body, which is the same as the core structure used conventionally.

直流重畳値NIに対するAL値は第2図Mの通りである
The AL value for the DC superimposition value NI is as shown in FIG. 2M.

5アンペアターン以下でインダクタンスの値は急激に大
きくなっているが、NIの大きい部分ではNIの値に対
しALの値は急激に小さくなる。
The value of inductance increases rapidly below 5 ampere turns, but in the portion where NI is large, the value of AL decreases rapidly with respect to the value of NI.

実施例−3 実施例−1のコアに初透磁率12000のMn−Znフ
ェライトコアを中脚の幅(中脚の幅は7.5mm)に対
し3mm幅でコア厚さはE1コアと同じ厚さとし、空隙
部3には■コア2に達する長さに小形磁心21を加工し
て樹脂により接着挿入し、磁心突き合わせ面は研削加工
し仕上げた。挿入した磁心材質の特性は初透磁率120
00、磁化力10エルステツドの時の飽和磁束密度は3
400力゛ウスである。此の時の直流重畳NIに対する
インダクタンスの値は第2図曲線Oの通りである。
Example-3 A Mn-Zn ferrite core with an initial permeability of 12,000 is used as the core of Example-1, and the width of the middle leg is 3 mm (the width of the middle leg is 7.5 mm), and the core thickness is the same as the E1 core. Then, a small magnetic core 21 was machined to a length that reached the core 2 and inserted into the gap 3 by adhesive bonding with resin, and the abutting surfaces of the magnetic cores were finished by grinding. The inserted magnetic core material has an initial permeability of 120.
00, the saturation magnetic flux density when the magnetizing force is 10 oersted is 3
It has 400 power. The value of inductance for DC superposition NI at this time is as shown by curve O in Figure 2.

実施例−4 実施例−1のコアに、初透磁率600のNi−Znフェ
ライトコアを中脚の幅に対し実施例−3と同じ犬きさに
小形磁心に加工し、(コア大きさは3mm幅でコア厚さ
はEIココア同じ厚さとし、空隙部の長さは■コアに達
する長さとした)空隙部に接着し、突き合わせ部は研削
加工した。磁心材質の特性は初透磁率600.磁化力1
0繕ステツドの時の磁束密度は2700力゛ウスである
Example-4 In the core of Example-1, a Ni-Zn ferrite core with an initial magnetic permeability of 600 was processed into a small magnetic core with the same size as in Example-3 for the width of the middle leg (the core size was It was 3 mm wide, the core thickness was the same as EI cocoa, and the length of the gap was set to reach the core.) It was glued to the gap, and the abutting part was ground. The characteristics of the magnetic core material are an initial magnetic permeability of 600. Magnetizing force 1
The magnetic flux density at zero maintenance mode is 2700 forces.

これらの実施例に於けるコアの直流重畳NIとインダク
タンスの特性は、第2図Pの通りである。
The characteristics of DC superposition NI and inductance of the core in these embodiments are as shown in FIG. 2P.

実施例−1ないし実施例−4の結果より、第3図(b)
の形状のコアを用い作ったインダクタの直流重畳特性は
第2図Mの曲線で示されるが、直流重畳NIが小さい時
はインダクタンスの値が大きいのに対し、200アンペ
アタ一ン以上の直流重畳NIに対しては、に、O,Pの
特性曲線に比べて直流重畳NIの低い値で飽和に達して
いるのに対し、空隙部に、磁心材料特性の異なる小形磁
心を挿入し構成した時はインダクタンスの値に対する直
流重畳NIは従来構造の磁心を使用したインダクタンス
に比べてNIの値は高く、はぼ20%高い方へ伸びてい
る。此の値は、磁心断面寸法で約10%小さく出来るこ
とを示し、第1図の構造の磁心とすることにより磁心寸
法を小さく出来ること、又同一寸法の時は直流重畳電流
に対する冗長度を持たせ得ることを示し、本発明の工業
的な効果は大きい。
From the results of Example-1 to Example-4, Fig. 3(b)
The DC superimposition characteristics of an inductor made using a core with the shape of are shown by the curve M in Figure 2. When the DC superposition NI is small, the inductance value is large, but when the DC superposition NI is 200 amperes or more, the inductance value is large. In contrast, saturation is reached at a lower value of DC superposition NI compared to the O and P characteristic curves, whereas when a small magnetic core with different core material properties is inserted in the air gap, The DC superposition NI with respect to the inductance value is higher than that of the inductance using a magnetic core of the conventional structure, and increases by about 20%. This value indicates that the cross-sectional dimension of the magnetic core can be reduced by approximately 10%, and that the core size can be reduced by using the magnetic core with the structure shown in Figure 1, and that when the dimensions are the same, it has redundancy against DC superimposed current. The present invention has a great industrial effect.

又、本発明は空隙部へ取り付ける磁気特性の異なる材料
を取り付ける方法として、予め加工したブロックを樹脂
接着により取り付けたが、磁心の焼結前に予め空隙に挿
入する磁気特性の異なる材料を作っておき、磁心の粉末
プレス成形時に一体プレス成形し、焼結、加工して所望
の磁心を作ってもよい。又実施例−1ないし実施例−4
はEI型磁心を用い実施した例により説明したものであ
るが、他の形状の磁心であるEE型、UU型。
Further, in the present invention, as a method for attaching materials with different magnetic properties to be inserted into the gap, pre-processed blocks are attached by resin bonding, but it is also possible to make materials with different magnetic properties to be inserted into the gap in advance before sintering the magnetic core. Then, the desired magnetic core may be produced by integral press molding during powder press molding of the magnetic core, sintering, and processing. Also, Example-1 to Example-4
Although the above was explained using an example using an EI type magnetic core, magnetic cores of other shapes such as EE type and UU type can also be used.

UI型の磁心を用い本発明を実施した時も本発明による
効果が得られることは当然である。
It goes without saying that the effects of the present invention can also be obtained when the present invention is implemented using a UI type magnetic core.

〔発明の効果〕〔Effect of the invention〕

本発明は、スイッチング電源の二次側整流回路に使用す
るチョークコイルの磁心として従来一体で成形して作っ
ていた階段磁路を持つ空隙成形法に対し、予め磁心の磁
路に空隙を形成して空隙に空隙部の体積より小さい磁気
特性の異なる小形磁心を樹脂接着、或いは一体プレス成
形磁心とすることにより、直流重畳特性に優れたチョー
クコイルとすることが出来る。
In contrast to the air-gap molding method that has a stepped magnetic path, which was conventionally made by integrally molding the magnetic core of a choke coil used in the secondary side rectifier circuit of a switching power supply, the present invention creates an air gap in the magnetic path of the magnetic core in advance. By attaching a small magnetic core with different magnetic properties smaller than the volume of the gap to the air gap with resin or forming an integrally press-molded magnetic core, a choke coil with excellent DC superimposition characteristics can be obtained.

又、階段磁路を持つ空隙は、加工が難しいのに対し、本
発明の方法は、予め空隙部は磁心の磁路を全面にわたり
所定の空隙長さに研削し、後小形磁心を取り付け、後突
き合わせ面を研削して作るもので、加工は容易である。
Furthermore, while it is difficult to process a gap with a stepped magnetic path, in the method of the present invention, the gap part is ground in advance to a predetermined gap length over the entire magnetic path of the magnetic core, and then a small magnetic core is attached. It is made by grinding the mating surfaces and is easy to process.

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

第1図は、本発明の可変インダクタ用磁心の構造を示す
図。 第2図は、第1図の磁心形状の磁心を用いて作ったチョ
ークコイルのインダクタンスと直流重畳NIとの特性曲
線、及び第3図(b)、第5図(b)に示す従来の形状
の磁心を用いた場合のチョークコイルのインダクタンス
と直流重畳NIとの特性曲線を示す。 K:第5図(b)の形状の磁心の直流重畳アンペアター
ン(AT)とコイル1回巻当たりのインダクタンス(A
LμH)との関係を示す図。 M:第3図(b)の形状の磁心の直流重畳アンペアター
ンとコイル1回巻当たりのインダクタンスを示す図。 ○:第1図の形状の磁心で、21の小形磁心に透磁率μ
m2000のMn−Znフェライトコアの小形磁心を用
いた時の直流重畳特性。 P:第1図の形状の磁心で、21の小形磁心に透磁率μ
600のNi−Znフェライトコアの小形磁心を用いた
時の直流重畳特性。 第3図は、スイッチング電源二次側チョークコイルに使
用されている磁心形状を示す図。 (a)はEE型の磁心。(b)はEI型磁心。 Aは磁気飽和領域を示す。 第4図は、第3図の磁心を用いチョークコイルとした時
の直流重畳Nlとインダクタンスとの値。 第5図は、従来一般的にチョークコイルに使われている
磁心形状。 (a)はEE型磁心。 (b)はE1型磁心。 第6図は、第3図の磁心をチョークコイルにした時の直
流重畳特性を示す曲線Bと、第5図に示す従来一般的に
使われている磁心を用いたチョークコイルの特性を示す
曲線Cを示す図。 1・・・E型磁心(磁心本体)。 2・・・■型磁心。 3・・・空隙。 4・・・階段状磁路。 5・・・中脚。 21・・・小形磁心。 特許出願人 東北金属工業株式会社 第1図 第312 第5図 I N/
FIG. 1 is a diagram showing the structure of a magnetic core for a variable inductor according to the present invention. Figure 2 shows the characteristic curves of the inductance and DC superposition NI of a choke coil made using the magnetic core with the magnetic core shape shown in Figure 1, and the characteristic curve of the choke coil with the conventional shape shown in Figures 3(b) and 5(b). The characteristic curve of the inductance of the choke coil and the DC superposition NI when using the magnetic core of FIG. K: DC superimposed ampere turns (AT) of the magnetic core with the shape shown in Figure 5(b) and inductance per coil turn (A
FIG. M: A diagram showing the DC superimposed ampere turns of the magnetic core having the shape of FIG. 3(b) and the inductance per coil turn. ○: The magnetic core has the shape shown in Figure 1, and the magnetic permeability μ is 21 small magnetic cores.
DC superposition characteristics when using a small Mn-Zn ferrite core of m2000. P: The magnetic core has the shape shown in Figure 1, and the magnetic permeability μ is 21 small magnetic cores.
DC superposition characteristics when using a small magnetic core of 600 Ni-Zn ferrite core. FIG. 3 is a diagram showing the shape of the magnetic core used in the secondary choke coil of the switching power supply. (a) is an EE type magnetic core. (b) is an EI type magnetic core. A indicates the magnetic saturation region. FIG. 4 shows the values of DC superposition Nl and inductance when the magnetic core of FIG. 3 is used as a choke coil. Figure 5 shows the shape of the magnetic core commonly used in choke coils. (a) is an EE type magnetic core. (b) is an E1 type magnetic core. Figure 6 shows a curve B showing the DC superposition characteristics when the magnetic core in Figure 3 is used as a choke coil, and a curve B showing the characteristics of a choke coil using a conventionally commonly used magnetic core as shown in Figure 5. A diagram showing C. 1...E-type magnetic core (magnetic core body). 2... ■ type magnetic core. 3...Void. 4...Stepped magnetic path. 5... Middle leg. 21...Small magnetic core. Patent applicant Tohoku Metal Industry Co., Ltd. Figure 1 Figure 312 Figure 5 I N/

Claims (1)

【特許請求の範囲】[Claims]  磁心の磁路に空隙を設けた可変インダクタ用磁心に於
て、空隙部の一部に磁心本体と異なる磁気特性の小型磁
心を挿入し、組立てた構造としたことを特徴とする可変
インダクタ用磁心。
A magnetic core for a variable inductor, characterized in that a magnetic core for a variable inductor has an air gap provided in the magnetic path of the magnetic core, and has an assembled structure in which a small magnetic core with magnetic characteristics different from that of the magnetic core body is inserted into a part of the air gap. .
JP28443687A 1987-11-10 1987-11-10 Magnetic core for variable inductor Pending JPH01125809A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28443687A JPH01125809A (en) 1987-11-10 1987-11-10 Magnetic core for variable inductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28443687A JPH01125809A (en) 1987-11-10 1987-11-10 Magnetic core for variable inductor

Publications (1)

Publication Number Publication Date
JPH01125809A true JPH01125809A (en) 1989-05-18

Family

ID=17678525

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28443687A Pending JPH01125809A (en) 1987-11-10 1987-11-10 Magnetic core for variable inductor

Country Status (1)

Country Link
JP (1) JPH01125809A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105990013A (en) * 2015-02-28 2016-10-05 怀化亚信电子有限公司 Large-current high-saturation-resistance inductor
JP2017525147A (en) * 2014-07-01 2017-08-31 キム, ドン‐フンKim, Dong‐Hun Variable inductor and inductor manufacturing method

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2017525147A (en) * 2014-07-01 2017-08-31 キム, ドン‐フンKim, Dong‐Hun Variable inductor and inductor manufacturing method
US10037845B2 (en) 2014-07-01 2018-07-31 Dong-hun Kim Variable inductor and method for manufacturing the same
CN105990013A (en) * 2015-02-28 2016-10-05 怀化亚信电子有限公司 Large-current high-saturation-resistance inductor

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