JPS6025208A - electromagnetic core - Google Patents
electromagnetic coreInfo
- Publication number
- JPS6025208A JPS6025208A JP58133832A JP13383283A JPS6025208A JP S6025208 A JPS6025208 A JP S6025208A JP 58133832 A JP58133832 A JP 58133832A JP 13383283 A JP13383283 A JP 13383283A JP S6025208 A JPS6025208 A JP S6025208A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- core
- ribbon
- thermal expansion
- electromagnetic core
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/24—Magnetic cores
- H01F27/25—Magnetic cores made from strips or ribbons
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Manufacturing Cores, Coils, And Magnets (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、磁性薄帯により電磁鉄心全製造する場合、磁
気時性の劣化を極力小さくし、製造 作業の艮好なif
f、(蔽鉄心に関するものである。[Detailed Description of the Invention] Industrial Field of Application The present invention is aimed at minimizing the deterioration of magnetic properties when manufacturing an electromagnetic core entirely using magnetic ribbons, and making the manufacturing process more convenient.
f, (relating to the shielding core.
従来例のIM成とその問題点
従来の屯(蔽鉄心は磁性薄帯として、非晶質合金全巻心
に巻付けた後、アニールを行い巻心を取外した後、磁心
の形が変形しないように金具で支持していfc。その電
磁鉄心の斜視図および半裁断面図1を第1図(A) 、
(B)に示す。1は磁性薄帯で、Fes+ B15,
5 Sis、s 02 、Feya B+5 5i9F
e79 1316 Sis 等の鉄系のものが広く使用
されている。ところが、前記の磁性薄帯1は鈑厚か約2
o〜30μで、磁歪定数が27〜30X10のきわめて
大きい値である。したがって作業中の徽少な応力により
著しい特性劣化が発生していた。Conventional IM configurations and their problems Conventional IM configurations (The shielding core is a magnetic ribbon, which is wound around an amorphous alloy core, then annealed and removed, so that the shape of the magnetic core does not deform. The electromagnetic core is supported by metal fittings on the fc.A perspective view and a half-cut sectional view 1 of the electromagnetic core are shown in Fig. 1(A).
Shown in (B). 1 is a magnetic ribbon, Fes+ B15,
5 Sis, s 02, Feya B+5 5i9F
Iron-based materials such as e79 1316 Sis are widely used. However, the magnetic ribbon 1 has a sheet thickness of about 2
o~30μ, and the magnetostriction constant is an extremely large value of 27~30×10. Therefore, significant property deterioration occurred due to the small stress during work.
%に板厚が薄くなると一定応力に対する歪量が増大する
ために作粟時の特性劣化に深刻な問題点を有していた。%, the amount of strain for a given stress increases, causing a serious problem in deterioration of properties during millet production.
発明の目的
本発明に、前記従来の電磁鉄心の欠点を除去するもので
、磁性薄帯の巻付、樹脂含侵、切断等の加工による磁気
特性劣化全極力小さくし、さらに磁心の製造作業性の良
好な電磁鉄心を提供すること全目的とするもので8る。Purpose of the Invention The present invention eliminates the drawbacks of the conventional electromagnetic core, minimizes deterioration of magnetic properties due to processing such as winding of magnetic ribbon, resin impregnation, and cutting, and further improves the workability of manufacturing the magnetic core. The overall purpose is to provide a good electromagnetic core.
発明の(l′6成
そのための構成として、本発明*、g!を性薄帯により
形成された磁心の積層端面f:磁性薄帯の磁歪が正のも
のについては磁性薄帯の熱膨張係数より小さい熱膨張係
数の磁性薄帯の磁歪が負のものについてに磁性薄帯の熱
膨張係数より大きい熱膨張係数の絶縁性の無機質層で被
覆したものである。As a configuration for achieving the invention (l'6), the present invention*, g! A magnetic ribbon having a smaller coefficient of thermal expansion and negative magnetostriction is coated with an insulating inorganic layer having a coefficient of thermal expansion larger than that of the magnetic ribbon.
実施例の説明
以下本発明の実施例につき図面の第2図u) 、 (B
)および第3図に沿って詳細に説明する。DESCRIPTION OF THE EMBODIMENTS The following is a description of the embodiments of the present invention as shown in Figures 2(u) and (B) of the drawings.
) and FIG. 3.
1は磁性薄帯で、超急冷法等で作製される優位的に非晶
質の合金薄帯または同様に超急冷法等で作製される珪素
鉄合金薄帯またに機械的な方法等で作製され、板厚が比
較的薄いものである。この板厚に薄い程、磁心端面に形
成する絶縁性の無機質層2の厚さを薄くして効果を得る
ことができる。1 is a magnetic ribbon, which is a predominantly amorphous alloy ribbon produced by an ultra-quenching method, a silicon-iron alloy ribbon similarly produced by an ultra-quenching method, or a mechanical method, etc. The plate thickness is relatively thin. The thinner the plate thickness is, the thinner the insulating inorganic layer 2 formed on the end face of the magnetic core can be.
また前記磁性薄帯1として、F、・B・s1糸の非晶質
合金、例えばFe79B+6 8is の組成のもの音
用いると、この利料の磁歪に27X10 で、か)膨張
係数が約100X 1o ”Cでらり、磁心端面に形成
する無機質層2として熱膨張係数90X10−7仝のア
ロンセラミックD(アルミナ系)を用い、その後必要に
応じて樹脂含浸を行う。Furthermore, if the magnetic ribbon 1 is an amorphous alloy of F, B, s1 threads, such as Fe79B+68is, the magnetostriction of this material is 27X10, and the expansion coefficient is approximately 100X10. Aron ceramic D (alumina type) having a coefficient of thermal expansion of 90.times.10@-7 is used as the inorganic layer 2 formed on the end face of the magnetic core, and then impregnated with resin as necessary.
このようにして得られた磁心に13+oの特性が1゜K
G以上で、20 K l(zにおける鉄損値は従来のも
のに比し約1710になった。なお、前記磁性薄帯1の
端面に熱膨張係数が磁性薄帯1のそれより大きい11Q
×10−7′℃ の低融点ガラスを用いた場合、B+o
がほとんど零になり、磁心として実用に供することが不
可能となることがらも本実施例の効果が著しいことが実
証される。The magnetic core obtained in this way has a characteristic of 13+o of 1°K.
G or more, the iron loss value at 20 K l (z is about 1710 compared to the conventional one.In addition, the end face of the magnetic ribbon 1 has a 11Q material whose coefficient of thermal expansion is larger than that of the magnetic ribbon 1.
× When using low melting point glass of 10-7′℃, B+o
is almost zero, making it impossible to put it to practical use as a magnetic core, which proves that the effect of this example is remarkable.
寸た磁性薄帯1として6.5〜6.7%珪素鉄合金薄帯
を用いる場合、この相別は磁歪が負であるために無膨張
係数が磁性薄帯1のそれより大きい低融点ガラスを用い
ることにより磁気特性を向上させることができた。When using a 6.5 to 6.7% silicon-iron alloy ribbon as the thin magnetic ribbon 1, this phase is a low-melting glass whose non-expansion coefficient is larger than that of the magnetic ribbon 1 because the magnetostriction is negative. By using , we were able to improve the magnetic properties.
また第2図(A) 、 CB)は巻鉄心であるが、第3
図に示すような打抜型の積層鉄心にも同様に前記の原理
は適用される。ただしこの場合他の磁心との突合せ部分
Vr−げ無機質15ηを形成しない。なお1r」層D:
:、’i面に形成する無機質層2の厚さに磁性薄帯1の
板厚より厚くすることにより、優れた特性を得ることが
できる。また無機質層2に磁界による短絡回路を構成し
ないように電気絶縁相であることが婦女である。Also, Fig. 2 (A), CB) shows the wound core, but the third
The above principle is similarly applied to a punched laminated core as shown in the figure. However, in this case, the inorganic material 15η is not formed in the abutting portion with the other magnetic core. Note that 1r” layer D:
:, By making the thickness of the inorganic layer 2 formed on the i-plane thicker than the thickness of the magnetic ribbon 1, excellent characteristics can be obtained. Further, the inorganic layer 2 should be an electrically insulating phase so as not to form a short circuit due to a magnetic field.
−1:た無(幾質層2會磁心の端面に形成することにつ
いて記載したが、磁心の全面に)1多成しても本実施例
の効果は失なわれない。-1: None (although it has been described that two geometric layers are formed on the end face of the magnetic core, the effect of this embodiment is not lost even if one or more geometric layers are formed on the entire surface of the magnetic core).
発明の効果
本発明によれば、?at生薄帯による磁心製造時の磁気
特性の低下全防止し、かつ磁性1.9帯相互間の固着全
充分に行うので、磁心の固定が不をとなり、製作のため
の作業14(二が向」二する優れた効果を奏するもので
ある。Effects of the Invention According to the present invention? Since the magnetic properties are completely prevented from deteriorating during the manufacture of the magnetic core using the AT raw thin ribbon, and the magnetic 1.9 bands are firmly fixed to each other, the fixing of the magnetic core becomes difficult and the manufacturing process 14 (second It has excellent effects on both sides.
4、図面の1バ1単な説り」
第1図(A) 、 (B)に従来の巻鉄心の概略斜視図
および半裁断面図、第2図(A) 、 (B)は本発明
の実施例による電磁鉄心の概略斜視図および半裁断「1
1図、第3図に他の実施例を示す積層磁心の概1略斜視
図である。4. Simple Explanation of Drawings" Figures 1 (A) and (B) are schematic perspective views and half-cut sectional views of the conventional wound core, and Figures 2 (A) and (B) are of the present invention. Schematic perspective view and half-cut “1” of an electromagnetic core according to an embodiment
1 and 3 are schematic perspective views of laminated magnetic cores showing other embodiments. FIG.
1・・・・・・(磁性薄帯、2・・・・・・無機質層。1... (Magnetic ribbon, 2... Inorganic layer.
Claims (1)
性薄帯の磁歪が正のものについては磁性薄帯の熱膨張係
数より小さい熱膨張係数の磁性薄帯の磁歪が負のものに
ついてに磁性薄帯の熱膨張係数より大きい熱膨張係数の
絶縁性の無機質層で被覆した電磁鉄心。Value 1! :The laminated end face of the magnetic core formed by lE ribbons is a magnetic thin strip with a thermal expansion coefficient smaller than the thermal expansion coefficient of the magnetic ribbon with a positive magnetostriction. An electromagnetic core coated with an insulating inorganic layer with a coefficient of thermal expansion greater than that of the band.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58133832A JPS6025208A (en) | 1983-07-21 | 1983-07-21 | electromagnetic core |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58133832A JPS6025208A (en) | 1983-07-21 | 1983-07-21 | electromagnetic core |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6025208A true JPS6025208A (en) | 1985-02-08 |
| JPH0376571B2 JPH0376571B2 (en) | 1991-12-05 |
Family
ID=15114079
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58133832A Granted JPS6025208A (en) | 1983-07-21 | 1983-07-21 | electromagnetic core |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6025208A (en) |
-
1983
- 1983-07-21 JP JP58133832A patent/JPS6025208A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0376571B2 (en) | 1991-12-05 |
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