JPS5934610A - Iron core - Google Patents

Iron core

Info

Publication number
JPS5934610A
JPS5934610A JP14445982A JP14445982A JPS5934610A JP S5934610 A JPS5934610 A JP S5934610A JP 14445982 A JP14445982 A JP 14445982A JP 14445982 A JP14445982 A JP 14445982A JP S5934610 A JPS5934610 A JP S5934610A
Authority
JP
Japan
Prior art keywords
iron core
core
gap material
gap
inductance
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
JP14445982A
Other languages
Japanese (ja)
Inventor
Yoshihiko Sekiguchi
関口 恵彦
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.)
Nippon Kinzoku Co Ltd
Original Assignee
Nippon Kinzoku Co 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 Nippon Kinzoku Co Ltd filed Critical Nippon Kinzoku Co Ltd
Priority to JP14445982A priority Critical patent/JPS5934610A/en
Publication of JPS5934610A publication Critical patent/JPS5934610A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F3/00Cores, Yokes, or armatures
    • H01F3/10Composite arrangements of magnetic circuits

Abstract

PURPOSE:To prevent excessive characteristics as well as to contrive effective utilizatin of an iron core by a method wherein a gap material, consisting of ferrite stainless steel, is inserted in a part of core magnetic path. CONSTITUTION:A gap material 12 consisting of ferrite stainless steel is inserted in a part of the core magnetic path of a thin silicon steel core 11. When the above-mentioned gap material is composed of a non-magnetic gap material, the area of core cross section and the number of winding can be reduced and the cost of the titled core can also be cut down.

Description

【発明の詳細な説明】 本発明は、小型リアクトルに用いられる鉄心に関する。[Detailed description of the invention] The present invention relates to an iron core used in a small reactor.

小型リアクトルは、鉄心に巻線ビしたインダクタンスを
持つ機器で、スイッチング電源、電算機用電源等に使用
される。この小型リアクトルには、チョーク・コイル、
インダクターと呼ばれているものも含まれる。
A small reactor is a device with an inductance wound around an iron core, and is used in switching power supplies, computer power supplies, etc. This small reactor includes a choke coil,
This includes what is called an inductor.

従来この種の鉄心は、第1図に示すように薄けい素鋼鉄
心1の一部に非磁性ギャップ材2を伏み込んでいる。こ
の鉄心は、巻線を施して小型リアクトルとした時の電流
−インダクタンス特性が第2図に示すようになる。この
場合電流に対するインダクタンス値は定格電流(例えば
5A)まで一定であれば十分であるが、従来の小型リア
クトルは1図示の如く定格電流の2倍程度あり、従来の
小型リアクトルは、図示の如く定格電流の2倍程度あり
、過剰特性になるとともに、巻回数も多く鉄心の利用が
十分でない問題があった。
Conventionally, in this type of core, a non-magnetic gap material 2 is sunk into a part of a thin silicon steel core 1, as shown in FIG. This iron core has current-inductance characteristics as shown in FIG. 2 when it is wound to form a small reactor. In this case, it is sufficient that the inductance value for the current is constant up to the rated current (for example, 5A), but in the case of a conventional small reactor, the inductance value is about twice the rated current as shown in Figure 1; The current is about twice that of the current, resulting in excessive characteristics, and the number of turns is large, causing the problem that the iron core is not fully utilized.

従来の構造において過剰特性をなくすためには一非圃性
ギャップ材2のギャップ長を小さくすればよいが、ギヤ
ツブ!形成するための切断用砥石の厚みが0.3 mm
以上であるため、ギャップ長に制限がある。また従来の
ギャップ材であるゾレスポード、力゛ラス積層板などは
、厚みの公差が大きく、選択の幅が狭いなどの問題があ
る。
In order to eliminate excessive characteristics in the conventional structure, it is sufficient to reduce the gap length of the one-dimensional gap material 2, but gears! The thickness of the cutting whetstone for forming is 0.3 mm.
Because of the above, there is a limit to the gap length. In addition, conventional gap materials such as Solespode and force laminated plates have large thickness tolerances and a narrow range of selection.

本発明は、上記事情に鑑みてなされたもので、その目的
とするところは、非磁性ギャッゾ材に代えてフェライト
系ステンIノスtkil Y用いることにより、過剰特
性ビ防ぎ、鉄心の有効利用を図ることができる小型リア
クトル用鉄心乞得んとするものである。
The present invention has been made in view of the above circumstances, and its purpose is to prevent excessive characteristic vibration and to effectively utilize the iron core by using ferritic stainless steel instead of non-magnetic Gyazzo material. An iron core for a small reactor that can be used is highly desirable.

以下本発明を図面を参照して説明する。The present invention will be explained below with reference to the drawings.

第3図は本発明に係る鉄心t′示し、この鉄心は薄けい
素鋼鉄心1ノの鉄心磁路の一部にフェライト系ステンレ
ス鋼からなるギャツゾ材12乞伏み込んでいる。
FIG. 3 shows an iron core t' according to the present invention, in which a gap material 12 made of ferritic stainless steel is embedded in a part of the core magnetic path of a thin silicon steel core 1.

この鉄心によれば、下記の如き特性を有する。This iron core has the following characteristics.

なお符号は第1表による。The codes are according to Table 1.

第1表 まず従来の非母性ギャップの場合、 鉄心上の巻線の回数’4nターンとすると、インダクタ
ンスは− n! L = − 1(ア である。
Table 1 First, in the case of a conventional non-maternal gap, if the number of turns of the winding on the iron core is 4n, then the inductance is -n! L = - 1 (A.

次に本発明に係るラテン1ノスギヤツプの場合、となる
Next, in the case of the Latin 1 nos gap according to the present invention, it becomes as follows.

インダクタンスを非磁性ギャップを用いた時と同じにす
るためには、以上の式から l!日   /!0 μ8   μ0 とすればよい。
In order to make the inductance the same as when using a non-magnetic gap, from the above formula, l! Day /! It may be set to 0 μ8 μ0.

すなわち同じインダクタンスを得るためにステンレスギ
ャップの場合では、非磁性ギャップに比べてμ8/μ0
倍の長さのもの全使用することができる。またギャップ
長を非磁性ギャップと同じとすれば、ステンレスギャッ
プを用いることによりμ0/μa倍の薄い非磁性ギャッ
プを挿入したことと同じになる、 次に本発明の具体的実施例につき説明する。
In other words, in order to obtain the same inductance, in the case of a stainless steel gap, compared to a non-magnetic gap, μ8/μ0
All double length ones can be used. If the gap length is the same as the non-magnetic gap, using a stainless steel gap is equivalent to inserting a non-magnetic gap that is .mu.0/.mu.a times thinner.Next, specific embodiments of the present invention will be described.

鉄心としてo、 05 mm厚の薄けい素鋼を用い、寸
法を幅10mm、内径25mm、外径35mm、ギャッ
プ長’a’ 1 mmとした。またギャップ材としてS
 tJ S 4.3 Q 13 A仕上げ相(フェライ
ト系ステンレス鋼)を用いた。この鉄心に巻線を施して
小型リアクトルを作製し、電流−インダクタンス特性を
調べた。その結果を第4図に曲線Aで示′f。
A thin silicon steel having a thickness of 0.05 mm was used as the iron core, and the dimensions were 10 mm in width, 25 mm in inner diameter, 35 mm in outer diameter, and 1 mm in gap length 'a'. Also, S as a gap material.
tJ S 4.3 Q 13 A finishing phase (ferritic stainless steel) was used. A small reactor was fabricated by winding this iron core, and its current-inductance characteristics were investigated. The results are shown in FIG. 4 by curve A'f.

また比較のために非磁性ギャップ材を用いた同じ寸法の
小型リアクトルを作製し、その電流−インダクタンス特
性を調べた。
For comparison, a small reactor of the same dimensions was fabricated using a non-magnetic gap material, and its current-inductance characteristics were investigated.

その結果を第4図に曲線Bで示す。The results are shown by curve B in FIG.

比較用の従来の小型リアクトルは、定格5A、100μ
Hのものであるが、曲線Bに示すように12Aまで10
0μI」’11保っており、過剰品質である。
A conventional small reactor for comparison has a rating of 5A and 100μ.
10 to 12A as shown in curve B.
It maintains 0 μI"'11, which is excessive quality.

これに対し本発明に係る小型リアクトルは、電流1−5
AでインダクタンスL=400μIIとなっている。こ
こで μ二透磁率(I4/m) S;鉄心断面積(Jr?) 1m;鉄心m路長(m) N;巻回数 である。従って本発明により定格5 A 、 100μ
Hの小型リアクトルを得るには、鉄心断■l積乞%、又
は巻回数をHに減らすことができ、コストを下げること
ができる。
On the other hand, the small reactor according to the present invention has a current of 1-5
At A, the inductance L is 400 μII. Here, μ2 magnetic permeability (I4/m) S: Core cross-sectional area (Jr?) 1 m; Iron core m path length (m) N: Number of turns. Therefore, according to the present invention, the rating is 5 A, 100μ
In order to obtain a small reactor of H, the iron core breakage rate or the number of windings can be reduced to H, and the cost can be reduced.

なお参考例として、ギヤラフ月に圧粉鉄心を用いた鉄心
からなる小型リアクトルの特性を示す。この鉄心は、0
.05 mm厚の薄けい素鋼を用いて、高さ10mm、
外径35+nmの寸法とし、ギャップ長を4mmとして
ここに圧粉鉄心を挾み込んだものである。この鉄心に巻
線全施した小型リアクトルの電流−インダクタンス特性
ン第5図に曲線Cで示す。また曲線Bは圧粉鉄心のかわ
りに同じ長さの非磁性ギヤツブ材乞はさみこんだもので
ある。
As a reference example, the characteristics of a small reactor consisting of an iron core using a powdered iron core in the gear rough month are shown. This iron core is 0
.. Using thin silicon steel with a thickness of 0.05 mm, the height is 10 mm,
It has an outer diameter of 35+nm, a gap length of 4 mm, and a dust core is inserted therein. The current-inductance characteristic of a small reactor in which all wires are wound around this iron core is shown by curve C in FIG. In addition, curve B is obtained by inserting a non-magnetic gear tooth material of the same length instead of a dust core.

この小型リアクトルは、小電流時に大きなインダクタン
ス2持ち、大電流時に小さなインダクタンス2持つ、こ
のためアノード、リアクトル、過飽和リアクトル等に好
適である。
This small reactor has a large inductance 2 when the current is small and a small inductance 2 when the current is large, so it is suitable for an anode, a reactor, a supersaturated reactor, etc.

以上の如く本発明によれば、ギャップ長さを減さなくと
も薄手の非磁性ギャップ材を用いたのと同じ効果欠得る
ことができる。このためこの鉄心Z小fr9アクドルに
用いると、鉄心材料費もしくは脇線工数の削減が可能で
ある。またフェライトステンレスfli(d ’l使用
するので、選択の幅が広く、厚みの公差が少さいので、
小型リアクトルの品質を安定とすることができるなど顕
著な効果馨4’ijる。
As described above, according to the present invention, the same effect as using a thin non-magnetic gap material can be obtained without reducing the gap length. Therefore, when this iron core Z small fr9 axle is used, it is possible to reduce the iron core material cost or side line man-hours. In addition, since ferrite stainless steel is used, there is a wide range of selection and small tolerances in thickness, so
There are significant effects such as the ability to stabilize the quality of small reactors.

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

第1図は従来の小型リアクトル用鉄心の斜視図、第2図
は同鉄心を用いた小型リアクトルの電流−インダクタン
ス特性を示す図、第3図は本発明の一実施例7示す小型
リアクトル用妖心の斜視図、第4図は同鉄心を用いた小
型リアクトルの電流−インダクタンス特性乞従来のもの
と比較して示す図、第5図は参考の小型リアクトルの電
流−インダクタンス特性を示す図である、 11・・・薄けい素鋼鉄心、12・・・フェライト系ス
テンレス鋼からなるギャップ材 出願人代理人  弁理士 鈴性成彦 矛星図     矛2図 覧几(A) 矛3図 矛4図 q耗1(A) 3IP5図
Fig. 1 is a perspective view of a conventional iron core for a small reactor, Fig. 2 is a diagram showing the current-inductance characteristics of a small reactor using the same iron core, and Fig. 3 is a perspective view of a conventional iron core for a small reactor. Figure 4 is a diagram showing the current-inductance characteristics of a small reactor using the same iron core in comparison with a conventional one, and Figure 5 is a diagram showing the current-inductance characteristics of a small reactor for reference. , 11...Gap material made of thin silicon steel core, 12...Gap material made of ferritic stainless steel Applicant's representative Patent attorney Narihiko Suzuki Star map of spear 2 Illustration guide (A) Illustration of spear 3 Illustration of spear 4 q Worn 1(A) 3IP5 diagram

Claims (1)

【特許請求の範囲】[Claims] 鉄心磁路の一部にフェライト系ステンレス鋼からなるギ
ャップ材を挾み込んでなる鉄心。
An iron core made by sandwiching a gap material made of ferritic stainless steel into a part of the iron core magnetic path.
JP14445982A 1982-08-20 1982-08-20 Iron core Pending JPS5934610A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14445982A JPS5934610A (en) 1982-08-20 1982-08-20 Iron core

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14445982A JPS5934610A (en) 1982-08-20 1982-08-20 Iron core

Publications (1)

Publication Number Publication Date
JPS5934610A true JPS5934610A (en) 1984-02-25

Family

ID=15362744

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14445982A Pending JPS5934610A (en) 1982-08-20 1982-08-20 Iron core

Country Status (1)

Country Link
JP (1) JPS5934610A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02251107A (en) * 1989-03-24 1990-10-08 Murata Mfg Co Ltd Choke coil
JPH0489721A (en) * 1990-07-30 1992-03-23 Nisshin Plant Eng Kk Dropping device for powder and granular material
US5615051A (en) * 1993-10-08 1997-03-25 Olympus Optical Co., Ltd. Bright triplet

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02251107A (en) * 1989-03-24 1990-10-08 Murata Mfg Co Ltd Choke coil
JPH0489721A (en) * 1990-07-30 1992-03-23 Nisshin Plant Eng Kk Dropping device for powder and granular material
US5615051A (en) * 1993-10-08 1997-03-25 Olympus Optical Co., Ltd. Bright triplet

Similar Documents

Publication Publication Date Title
EP0042525B1 (en) Amorphous magnetic alloy
CA1122289A (en) Flux control in tape windings
JP3009686B2 (en) Inductor
US6144279A (en) Electrical choke for power factor correction
JPS60716A (en) Amorphous cut core
JPS5934610A (en) Iron core
JP2754641B2 (en) Converter transformer
JPS639918A (en) Reactor for blocking radio interference
JPS5934608A (en) Core for small sized reactor
JPH07153613A (en) Core for choke coil and nonlinear choke coil
JPH02165610A (en) Transformer
JP2804029B2 (en) Noise reduction element
JP2005072160A (en) Amorphous iron-core transformer and three-phase five-leg wound iron-core transformer
JPH0834160B2 (en) Swing choke coil
JP2602843B2 (en) Noise reduction element
JPS63228605A (en) Inductance element
JPS59182514A (en) Magnetic core for choke coil
JPH0366801B2 (en)
JPS6032313A (en) Magnetic core
JPH0745440A (en) Pulse transformer
JPS5844704A (en) Inductor for power supply line filter
JPS5910147A (en) Stator for rotary electric machine
SU758270A1 (en) Inductance coil
JPS5593524A (en) Multi-channel magnetic head
JPH05291020A (en) Composite toroidal core for noise filter