JPS58175807A - Magnetic core for transformer - Google Patents
Magnetic core for transformerInfo
- Publication number
- JPS58175807A JPS58175807A JP57058883A JP5888382A JPS58175807A JP S58175807 A JPS58175807 A JP S58175807A JP 57058883 A JP57058883 A JP 57058883A JP 5888382 A JP5888382 A JP 5888382A JP S58175807 A JPS58175807 A JP S58175807A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic core
- silicon steel
- transformer
- core
- hardener
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/12—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
- H01F1/14—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
- H01F1/147—Alloys characterised by their composition
- H01F1/14766—Fe-Si based alloys
- H01F1/14775—Fe-Si based alloys in the form of sheets
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Chemical & Material Sciences (AREA)
- Dispersion Chemistry (AREA)
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Soft Magnetic Materials (AREA)
Abstract
Description
【発明の詳細な説明】 本発明は、トランス用磁心に関するものである。[Detailed description of the invention] The present invention relates to a magnetic core for a transformer.
従来、トランスをはじめとする磁気回路用の磁心は、3
重量%珪素鋼板が使用されているが、電気抵抗率が低い
ため、電力の損失が大きく、そのためさらに改良の試み
がなされている。その改良材として、一方向珪素鋼板や
二方向性珪素鋼板がある。一方向性珪素鋼板で、第1図
(ム)に示すようなUI型トランス磁心を構成した場合
においては、工型磁心が、圧延方宗に、またU型磁心の
両腕が圧延方向に平行に打抜かれるので、四辺のうち三
辺しか容易磁化方向を利用することができない。Conventionally, magnetic cores for magnetic circuits such as transformers have three
Weight percent silicon steel sheets have been used, but their low electrical resistivity results in large power losses, and further attempts have been made to improve them. As improved materials, there are unidirectional silicon steel plates and bidirectional silicon steel plates. When configuring a UI type transformer core as shown in Figure 1 (m) using a unidirectional silicon steel plate, the working type core is parallel to the rolling direction, and both arms of the U type magnetic core are parallel to the rolling direction. Since it is punched out, the easy magnetization direction can only be used on three of the four sides.
そのため、鉄損が犬きくなる。また、第1図(B)に示
すようなトランス磁心を二方向性珪素鋼板で構成した場
合、四辺で磁化容易方向全利用することができるため、
同図(ム)の磁心に比べて鉄損が小さい。しかし、なお
隅角における磁束の曲がりがあるため、磁路のすべてが
磁化容易方向になっていないため、さらに改良が望まれ
ている。As a result, iron loss increases. In addition, if the transformer core is made of bidirectional silicon steel plates as shown in Figure 1(B), all four sides can be used in all directions of easy magnetization.
Iron loss is smaller than the magnetic core in the same figure (m). However, due to the bending of the magnetic flux at the corners, not all of the magnetic paths are in the direction of easy magnetization, so further improvements are desired.
珪素鋼板においては珪素5〜8重量%を含有させると、
その抵抗率が従来の3%珪素鋼板の電気抵抗率の2倍以
上となり、かつ飽和磁歪定数も小さくなるため、この材
料は電気回路用の磁心用としてきわめて優れたものであ
る。この6〜8重量%の珪素を含む高珪素鋼FjI′i
冷nl圧延がきわめて困鑓であるため、薄板化が難しく
、磁心として実用化されていない。When silicon steel plate contains 5 to 8% by weight of silicon,
Because its resistivity is more than twice the electrical resistivity of conventional 3% silicon steel sheets and its saturation magnetostriction constant is small, this material is extremely suitable for use in magnetic cores for electrical circuits. This high silicon steel FjI′i containing 6 to 8% by weight of silicon
Since cold NL rolling is extremely difficult, it is difficult to reduce the thickness of the sheet, and it has not been put to practical use as a magnetic core.
最近、液体超急冷技術を用い、高珪素鋼薄帯を作製する
ことが研究されている。その結果によれば、珪素含有量
の多い珪素鉄合金においても超急冷法を用いるときわめ
て靭性に富む薄帯が容易に得られることがわかった。こ
の薄帯では、その凝固過程で薄帯の厚さ方向に主として
熱流が発生するので、結晶の優先成長が厚さ方向におこ
る。つまりその優先方位は<100>であり、かつ、薄
帯の面内で無配向になっていることが、X線回折により
明らかとなったニ したがって、この薄帯をトロイダル
巻きか、打抜きにより積層にしてトランス用磁心に用い
ると、磁束の流れ方向は磁化容易方向ではなく、従来の
配向性珪素鋼板と比べて鉄損の点で特徴がでない。発明
者らは、かかる超急冷高珪素鋼帯について種々研究した
結果、8×10 ’torrのより低い真空中か、不活
性ガス雰囲気中において、900〜1200℃で熱処理
をすることにより、薄帯面内で薄帯の長手方向にLとし
て<O’11 >方位が配向することを見出した。Recently, research has been conducted on producing high-silicon steel ribbons using liquid ultra-quenching technology. According to the results, it was found that even in silicon-iron alloys with a high silicon content, thin ribbons with extremely high toughness can be easily obtained by using the ultra-quenching method. In this ribbon, heat flow is mainly generated in the thickness direction of the ribbon during the solidification process, so preferential growth of crystals occurs in the thickness direction. In other words, X-ray diffraction revealed that the preferred orientation is <100> and that there is no orientation within the plane of the ribbon. Therefore, this ribbon can be laminated by toroidal winding or punching. When used in a magnetic core for a transformer, the flow direction of magnetic flux is not the direction of easy magnetization, and there is no characteristic in terms of iron loss compared to conventional oriented silicon steel sheets. As a result of various studies on such ultra-quenched high-silicon steel strips, the inventors found that they can be made into thin strips by heat treatment at 900 to 1200°C in a lower vacuum of 8 x 10' torr or in an inert gas atmosphere. It has been found that <O'11> orientation is oriented as L in the longitudinal direction of the ribbon within the plane.
集合組織としては、(10o)〔011〕であった。こ
のような薄帯ヲ、]第第2図に示すように、薄帯9の長
手方向に対して、磁心薄片10’i45度傾けて打ち抜
き、得られた磁心薄片を積層すると磁束の流れ方向が全
て磁化容易軸方向となる。そして、この磁心は珪素を大
量に含有しているため、抵抗率が高くなり、従来にない
、低鉄損のトランス用磁心が得ちれた。また本発明によ
る磁心を用いてトランス全構成し、騒音特性を測定する
ときわめて低いことがわかった。これは配向性が高いこ
とによるもので、低騒音、低損失のトランス用磁心を実
現するものである。The texture was (10o)[011]. As shown in FIG. 2, such a thin strip is punched out at an angle of 45 degrees with respect to the longitudinal direction of the thin strip 9. When the obtained thin magnetic core pieces are stacked, the flow direction of the magnetic flux is changed. All are in the easy axis direction of magnetization. Since this magnetic core contains a large amount of silicon, it has a high resistivity, making it possible to obtain a transformer core with unprecedentedly low iron loss. Furthermore, when the entire transformer was constructed using the magnetic core according to the present invention and the noise characteristics were measured, it was found that the noise characteristics were extremely low. This is due to its high orientation, and enables the realization of a magnetic core for transformers with low noise and low loss.
次に、本発明の実施例について説明する。Next, examples of the present invention will be described.
実施例1
F2O3,4Si6.6 (組成比率は重量百分率)の
母合金を作製し、第3図に示すように、この母合金をノ
ズル2に入れ、コイル1に高周波電流を流し、1606
℃に誘導加熱して、溶湯eとした。この溶湯6にアルゴ
ンガスにより0.3〜O、’ K// cAOif力を
加えて、周速22m/秒で回転する円柱状の鉄製回転体
3の回転面上にノズル2から噴出させ、急冷、凝固させ
ることにより高珪素鋼帯6’i得た。このようにして得
られた薄帯は、中16傷厚さ60μmのものであった。Example 1 A mother alloy of F2O3,4Si6.6 (composition ratio is weight percentage) was prepared, and as shown in FIG.
It was induction heated to ℃ to obtain molten metal e. A force of 0.3~0,'K//cAOif is applied to the molten metal 6 using argon gas, and the molten metal is jetted from the nozzle 2 onto the rotating surface of the cylindrical iron rotating body 3 rotating at a circumferential speed of 22 m/sec to rapidly cool it. , a high-silicon steel strip 6'i was obtained by solidification. The ribbon thus obtained had a thickness of 60 μm with 16 scratches.
この薄帯を第2図に示すように長手方向に46゜傾けて
打ち抜き、得られた磁心薄片7を第4図に示すように絶
縁膜8と全交互に積層して、トランス用磁心を形成した
。This thin strip is punched out at an angle of 46° in the longitudinal direction as shown in FIG. 2, and the obtained magnetic core thin pieces 7 are laminated alternately with insulating films 8 as shown in FIG. 4 to form a magnetic core for a transformer. did.
比較のために従来の高配向性珪素鋼板で巻鉄心トランス
を作製した。For comparison, a wound core transformer was fabricated using a conventional highly oriented silicon steel plate.
このようにして得られた磁心の5oHzでの鉄損を第5
図に示す。これから明らかなように、本発明の方法によ
れば鉄損が大巾に減少している。The core loss at 5oHz of the magnetic core obtained in this way is calculated as
As shown in the figure. As is clear from this, according to the method of the present invention, iron loss is significantly reduced.
そして、騒音も、上記従来の巻鉄心トランスのノベル’
1iodBとしたとき、本発明のトランスは一41iB
であった。And the noise is also reduced by the novelty of the conventional wound core transformer mentioned above.
1 iodB, the transformer of the present invention has a power of -41 iB.
Met.
実施例2
Q1QIEI厚の高珪素鋼帯Fe、。。−xSix(x
二4.6 、5.3 、 e、s )と絶縁膜とを実施
例1のように交互に積層した。Example 2 High silicon steel strip Fe with Q1QIEI thickness. . −xSix(x
24.6, 5.3, e, s) and an insulating film were alternately laminated as in Example 1.
第6図にその鉄損(1,sT 、 5OHz )k示す
。Figure 6 shows the iron loss (1,sT, 5OHz)k.
図において、点ムはo、3ysJの高配向性珪素鋼板の
磁心、曲線BはFe、oo、Si !(100)無配向
高珪素鋼帯による磁心、曲線Cは、本発明の磁心の鉄損
特性をそれぞれ示す。これから本発明の磁心の鉄損の少
ないことがわかる。In the figure, point M is o, 3ysJ highly oriented silicon steel plate magnetic core, curve B is Fe, oo, Si! A magnetic core made of a (100) non-oriented high-silicon steel strip and a curve C each represent the iron loss characteristics of the magnetic core of the present invention. It can be seen from this that the core loss of the magnetic core of the present invention is small.
以上のように、本発明によれば、鉄損が低く、かつ騒音
の小さい磁気特性の優れたトランス用磁心を提供するこ
とができる。As described above, according to the present invention, it is possible to provide a transformer core with low iron loss, low noise, and excellent magnetic properties.
第1図(A) 、 (B)はそれぞれ方向性珪素鋼板の
打抜四角閉磁路積層磁心を示す図、第2図は本発明の磁
心の形成方法を示す図、第3図は液体超急冷方法を示す
図、第4図は本発明の一実施例である。磁心の斜視図、
第6図は本発明の磁心と方向性珪素鋼板の鉄損を比較し
て示す図、第6図は本発明の池の実施例である磁心と比
較例の鉄損を対比させて示す図である。
7・・・磁心薄片、8・・・・・・絶縁膜、9・・・・
・・(1oO)〔o11〕組織をもつ高珪素鋼帯、1o
・・・・・・打抜きコア。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第3
図
第4図
第5図
石並永尿洩(J)
富6図
Fe tca−y 3bXFigures 1 (A) and (B) are diagrams showing the square closed magnetic circuit laminated magnetic core punched from grain-oriented silicon steel sheets, Figure 2 is a diagram showing the method for forming the magnetic core of the present invention, and Figure 3 is a diagram showing the method of forming the magnetic core of the present invention. A diagram illustrating the method, FIG. 4, is an embodiment of the present invention. Perspective view of the magnetic core,
Figure 6 is a diagram comparing the iron loss of the magnetic core of the present invention and a grain-oriented silicon steel plate. Figure 6 is a diagram comparing the iron loss of the magnetic core of the present invention and a comparative example. be. 7...Magnetic core thin piece, 8...Insulating film, 9...
...(1oO) [o11] High silicon steel strip with structure, 1o
...Punching core. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 3
Fig. 4 Fig. 5 Ishinami Eigaureki (J) Tomi 6 Fig. Fe tca-y 3bX
Claims (1)
100)方位が実質的に配向するとともに、長手方向に
くoll〉方位が実質的に配向している高珪素鋼帯から
なり、磁束の流れる方向が磁化容易方向であることを特
徴とするトランス用磁心。Contains 5.0 to 8.0% by weight of silicon, and in the thickness direction (
100) A transformer comprising a high-silicon steel strip whose orientation is substantially oriented and whose orientation is substantially oriented in the longitudinal direction, and characterized in that the direction in which magnetic flux flows is the direction of easy magnetization. core.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57058883A JPS58175807A (en) | 1982-04-07 | 1982-04-07 | Magnetic core for transformer |
US06/390,132 US4427462A (en) | 1981-06-18 | 1982-06-18 | Electric apparatus and its magnetic core of (100)[011] silicon-iron sheet made by rapid quenching method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57058883A JPS58175807A (en) | 1982-04-07 | 1982-04-07 | Magnetic core for transformer |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS58175807A true JPS58175807A (en) | 1983-10-15 |
Family
ID=13097163
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57058883A Pending JPS58175807A (en) | 1981-06-18 | 1982-04-07 | Magnetic core for transformer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58175807A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4990197A (en) * | 1986-08-01 | 1991-02-05 | Allied-Signal, Inc. | Heat treatment of rapidly quenched Fe-6.5 wt % Si ribbon |
-
1982
- 1982-04-07 JP JP57058883A patent/JPS58175807A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4990197A (en) * | 1986-08-01 | 1991-02-05 | Allied-Signal, Inc. | Heat treatment of rapidly quenched Fe-6.5 wt % Si ribbon |
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