JPH03219021A - Production of grain-oriented silicon steel sheet minimal in iron loss - Google Patents

Production of grain-oriented silicon steel sheet minimal in iron loss

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Publication number
JPH03219021A
JPH03219021A JP2194496A JP19449690A JPH03219021A JP H03219021 A JPH03219021 A JP H03219021A JP 2194496 A JP2194496 A JP 2194496A JP 19449690 A JP19449690 A JP 19449690A JP H03219021 A JPH03219021 A JP H03219021A
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JP
Japan
Prior art keywords
cold rolling
rolling
hot
annealing
steel sheet
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
Application number
JP2194496A
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Japanese (ja)
Other versions
JPH0781166B2 (en
Inventor
Yasunari Yoshitomi
吉冨 康成
Katsuro Kuroki
黒木 克郎
Kenzo Iwayama
岩山 健三
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Nippon Steel Corp
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Nippon Steel Corp
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Publication date
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Priority to JP2194496A priority Critical patent/JPH0781166B2/en
Publication of JPH03219021A publication Critical patent/JPH03219021A/en
Publication of JPH0781166B2 publication Critical patent/JPH0781166B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Soft Magnetic Materials (AREA)

Abstract

PURPOSE:To stably produce a grain-oriented silicon steel sheet minimal in iron loss by reducing C content to a specific value in the course between the conclusion of hot rolling and the initiation of final cold rolling at the time of producing a grain- oriented silicon steel sheet with a specific composition. CONSTITUTION:A hot rolled plate of a silicon steel having a composition consisting of 2.5-4.0% Si, 0.03-0.10% C, 0.015-0.040% acid-soluble Al, 0.0040-0.0100% N, 0.01-0.04% S, 0.02-0.2% Mn, further <=0.4% Sn and/or Cu, and the balance Fe with inevitable impurities is annealed. Subsequently, this hot rolled plate is successively subjected to two-time or more cold rollings including forced final cold rolling at >80-95% rolling reduction, to process annealing performed between the cold rolling stages, to decarburizing annealing after final cold rolling, and to final finish annealing, by which the thin grain-oriented silicon steel sheet of 0.10-0.23mm sheet thickness having high magnetic flux density is produced. At this time, in the course between the conclusion of hot rolling and the initiation of final cold rolling, decarburizing is carried out so that C content is reduced to 0.0070-0.0300%. By this method, the grain-oriented silicon steel sheet used for iron core for transformer, etc., and excellent in iron loss characteristics can be obtained.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、トランス等の鉄芯に用いられる鉄損特性の優
れた板厚の薄い高磁束密度一方向性電磁鋼板の製造方法
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Application Field) The present invention relates to a method for manufacturing a thin, high magnetic flux density unidirectional electrical steel sheet with excellent iron loss characteristics used for the iron core of transformers and the like. be.

(従来の技術) ・方向性電磁鋼板は軟磁性材料として主にトランスその
他の電気機器の鉄心材料に使用されているもので、磁気
特性として励磁特性と鉄損特性が良好でなくてはならな
い。
(Prior art) - Grain-oriented electrical steel sheets are soft magnetic materials that are mainly used as core materials for transformers and other electrical equipment, and must have good magnetic properties in terms of excitation properties and core loss properties.

この励磁特性を表わす数値として通常B8  (磁場の
強さ800A/mにおける磁束密度)を用い、鉄損特性
を表わす数値としてW + w/so  (50Hzで
1.7Tまで磁化させた時の1kg当りの鉄損)を用い
ている。
B8 (magnetic flux density at a magnetic field strength of 800 A/m) is usually used as a numerical value representing this excitation characteristic, and W + w/so (per 1 kg when magnetized to 1.7 T at 50 Hz) is used as a numerical value representing iron loss characteristics. iron loss) is used.

この一方向性電磁鋼板は通常2次再結晶現象を利用して
鋼板面に(1101面、圧延方向に<001>軸をもっ
たいわゆるゴス組織を発達させることによって得られて
いる。良好な磁気特性を得るためには磁化容易軸である
<001>軸を圧延方向に高度に揃える事が重要である
。又板厚、結晶粒度、固有抵抗、表面被膜、鋼板の純度
等も磁気特性に大きな影響を及ぼす。
This unidirectional electrical steel sheet is usually obtained by developing a so-called Goss structure with a 1101 plane and a <001> axis in the rolling direction on the steel sheet surface using a secondary recrystallization phenomenon. In order to obtain these characteristics, it is important to highly align the <001> axis, which is the axis of easy magnetization, in the rolling direction.Also, sheet thickness, grain size, resistivity, surface coating, purity of the steel sheet, etc. have a large effect on magnetic characteristics. affect.

方向性についてはMnS、AlNをインヒビターとして
利用する最終弾圧下冷間圧延を特徴とする方法によって
大幅に向上し、それに伴って鉄損特性も著しく向上して
きた。
The directionality has been significantly improved by a method characterized by cold rolling under final compression using MnS and AlN as inhibitors, and the iron loss properties have also been improved accordingly.

・方、近年エネルギー価格の高騰を背景として、トラン
スメーカーは低鉄損トランス用素材への指向を一段と強
めている。低鉄損素材としてアモルファス合金や6.5
%Si鋼等の開発も進められてはいるが、トランス用材
料として工業的に使用するには解決すべき問題を残して
いる。そこで低鉄損化の方法として方向性電磁鋼板の板
厚を薄くして、鉄損を減少させるなどの努力も払われて
きた。
・In recent years, against the backdrop of rising energy prices, transformer manufacturers have increasingly focused on materials for low core loss transformers. Amorphous alloys and 6.5 as low iron loss materials
Although progress is being made in the development of steels such as %Si steel, there are still problems that need to be solved before they can be used industrially as materials for transformers. Therefore, efforts have been made to reduce iron loss by reducing the thickness of grain-oriented electrical steel sheets.

鋼板の板厚を薄くすることは鉄損の70%以上を占める
渦流損失を減少する上で有効であることは以前から知ら
れて居ることであるが、従来まではトランスの組立てな
どの作業上の要請から0.301IllI+前後の板厚
が主であった。しかしながら昨今のように省エネルギー
の要請がより強くなると、作業性の要請が上まわって板
厚が0.20mmよりもさらに薄いものまで使用される
ようになって来た。
It has long been known that reducing the thickness of steel plates is effective in reducing eddy current loss, which accounts for over 70% of iron loss, but until now it has been known that reducing the thickness of steel plates is effective in reducing eddy current loss, which accounts for over 70% of iron loss. Due to this request, the main plate thickness was around 0.301IllI+. However, as the demand for energy conservation has become stronger in recent years, the demand for workability has been outweighed, and plates with thicknesses even thinner than 0.20 mm have come to be used.

しかしながら、一般に板厚が薄くなると2次再結晶が生
じ難くなる傾向がある。その原因のひとつは、同一熱延
板の板厚からより薄い製品を得る場合にはより大きい冷
延圧下を施こすところとなり、集合組織上の不利が生じ
ることである。かかる原因の解決策としては、製品板厚
に応じて熱延板の板厚を減少させる方法が考えられる。
However, in general, as the plate thickness becomes thinner, secondary recrystallization tends to become less likely to occur. One of the reasons for this is that when a thinner product is obtained from the same hot-rolled sheet thickness, a greater cold rolling reduction is required, resulting in disadvantages in terms of texture. A possible solution to this cause is to reduce the thickness of the hot-rolled sheet according to the product thickness.

しかしながら、この方法には限界がある。と云うのは、
熱延板を薄くすることば熱延終了温度が必然的に低くな
り、AI!、N 、 MnSの析出を促進するため過剰
な析出サイズとなって磁性が劣化する欠点が生じるため
である。
However, this method has limitations. That is,
Making the hot-rolled sheet thinner inevitably lowers the hot-rolling finish temperature, which leads to AI! , N, and MnS, resulting in an excessive precipitate size and deterioration of magnetism.

上記の如く、集合組織上の不利を解決する手段としての
熱延板の板厚を薄くすることには限界があるため、工程
が増えるが中間冷間圧延工程を導入しなければならない
。つまり、熱間圧延後、冷間圧延を行ない、さらに中間
焼鈍を行なって、次いで最終板厚まで所定の圧下率で冷
間圧延する方法であり、かかる方法は2次再結晶をかな
り安定化し、高磁束密度も得られ易くはなるが、最終板
厚を0.18mm以下の、しかも鉄損の良い磁性を得る
方法としては未だ不充分である。この不充分な原因のひ
とつは、素地の組織に不均一な領域が残存し、後述の線
状の2次再結晶領域が多発し易いためである。かかる欠
点を排除する方法として、第1回目の冷間圧延に先立っ
て、熱延板の焼鈍を加える方法が提案されている(米国
特許第819426号明細書)。確かに、この方法を付
加した場合の中間冷間圧延にひき続く焼鈍工程により、
組織の再結晶化率が高まり、最終的な脱炭焼鈍後の2次
再結晶発達の素地となる組織は大幅に改善され、0、1
4 mmの板厚までは2次再結晶は安定化するが、磁束
密度が低下するなどの原因で充分満足すべき磁気的性質
は得られ難い。
As mentioned above, there is a limit to reducing the thickness of a hot-rolled sheet as a means of solving disadvantages in texture, so an intermediate cold rolling step must be introduced, although the number of steps increases. In other words, after hot rolling, cold rolling is performed, intermediate annealing is performed, and then cold rolling is performed at a predetermined reduction rate to the final plate thickness.This method considerably stabilizes secondary recrystallization, Although it becomes easier to obtain a high magnetic flux density, it is still insufficient as a method for obtaining magnetism with a final plate thickness of 0.18 mm or less and good iron loss. One of the reasons for this insufficiency is that non-uniform regions remain in the structure of the substrate, and linear secondary recrystallization regions described below are likely to occur frequently. As a method for eliminating such drawbacks, a method has been proposed in which the hot-rolled sheet is annealed prior to the first cold rolling (US Pat. No. 819,426). It is true that when this method is added, the annealing process that follows the intermediate cold rolling
The recrystallization rate of the structure increases, and the structure that forms the basis for the development of secondary recrystallization after the final decarburization annealing is greatly improved.
Although secondary recrystallization is stabilized up to a plate thickness of 4 mm, it is difficult to obtain sufficiently satisfactory magnetic properties due to factors such as a decrease in magnetic flux density.

このように板厚の薄い方向性電磁鋼板の開発にも解決す
べき課題が残っている。またインヒビターとしてINを
用いない成分系で、熱間圧延工程後最終冷間圧延工程終
了前の工程途中で脱炭を行なうことによって磁気特性が
向上するという報告(特開昭58−55530号公報)
があるが、この技術は最終冷延圧下率が40〜80%で
始めて効果が出るとされて居り、80%超の高圧延率を
特徴とする本発明の様な場合とは異った技術と解される
In this way, there are still issues to be solved in the development of thin grain-oriented electrical steel sheets. In addition, it has been reported that magnetic properties are improved by decarburizing a component system that does not use IN as an inhibitor during the process after the hot rolling process but before the end of the final cold rolling process (Japanese Unexamined Patent Publication No. 58-55530).
However, this technology is said to be effective only when the final cold rolling reduction is between 40% and 80%, which is different from the present invention, which is characterized by a high rolling reduction of over 80%. It is understood that

(発明が解決しようとする課題) 本発明はAI!、Nを主インヒビターとする高磁束密度
を有する電磁鋼板を0.10〜0.23 mmの様な薄
板化する場合、2次再結晶安定化を得るためには最終冷
延圧下率を高くすることが出来ず従って高い磁束密度を
得ることが出来ないと云う難点を解決する方法を提供す
るものである。
(Problem to be solved by the invention) The present invention is an AI! When thinning an electromagnetic steel sheet with a high magnetic flux density using N as the main inhibitor to a thickness of 0.10 to 0.23 mm, the final cold rolling reduction ratio must be increased in order to stabilize the secondary recrystallization. The present invention provides a method for solving the problem that it is impossible to obtain a high magnetic flux density.

(課題を解決するための手段) 本発明は熱間圧延後最終冷間圧延前の工程においてCを
0.0070〜0.0300%脱炭させることにより最
終冷延圧下率を80%超にして高磁束密度と共に低鉄損
値をも有する板厚の薄い電磁鋼板の製造方法を提供する
ものである。
(Means for Solving the Problems) The present invention achieves a final cold rolling reduction of over 80% by decarburizing C by 0.0070 to 0.0300% in a step after hot rolling and before final cold rolling. The present invention provides a method for producing a thin electrical steel sheet having a high magnetic flux density and a low iron loss value.

即ち、本発明者らは、上記方法、即ちAfNを主なイン
ヒビターとし、最終冷延圧下率を80%超とすることで
高磁束密度材を得る方法において、0.10〜0.23
mmまでの薄い板厚にしてしかも磁束密度、鉄損の良い
材料を安定して得る方法について検討した結果、かかる
板厚の薄い場合には、脱炭焼鈍工程後の2次再結晶発生
位置の素地をより安定な、つまりより整粒化する必要が
あること、さらにはかかる2次再結晶核の数、即ち(1
101<001>方位の1次再結晶粒を増加させること
によって、2次再結晶をより安定化させ、さらにまた2
次再結晶粒の方位がよりシャープな+1101<001
>方位にせしめ得、また(1101 <001>方位2
次再結晶粒のサイズが小さく改善されることを見出した
That is, the present inventors have developed a method for obtaining a high magnetic flux density material by using AfN as the main inhibitor and making the final cold rolling reduction more than 80%.
As a result of examining methods for stably obtaining materials with good magnetic flux density and iron loss while making the plate thickness as thin as 1.0 mm, we found that when the plate thickness is thin, the position of secondary recrystallization after the decarburization annealing process is It is necessary to make the substrate more stable, that is, to make it more grained, and furthermore, the number of secondary recrystallized nuclei, i.e., (1
By increasing the number of primary recrystallized grains with 101<001> orientation, secondary recrystallization is made more stable, and
+1101<001 where the orientation of the next recrystallized grain is sharper
> direction, and (1101 <001> direction 2
It has been found that the size of the recrystallized grains is reduced and improved.

具体的に説明すると、圧下率調整のための中間冷間圧延
の前に熱延板焼鈍工程を行なうことに加えて、熱間圧延
後最終冷間圧延前までの工程において、鋼中のCを0.
0070〜0.0300%脱炭する方法により鉄損、磁
束密度共に優れた0、10〜0.23mmの板厚の方向
性電磁鋼板が得られることを見出したものである。
Specifically, in addition to performing a hot-rolled sheet annealing process before intermediate cold rolling to adjust the rolling reduction ratio, C in the steel is removed during the process after hot rolling and before final cold rolling. 0.
It has been discovered that a grain-oriented electrical steel sheet with a thickness of 0.10 to 0.23 mm, which is excellent in both iron loss and magnetic flux density, can be obtained by decarburizing by 0.070 to 0.0300%.

以下本発明の詳細な説明する。The present invention will be explained in detail below.

本発明の出発素材である熱延板の成分についてはSi:
2.5〜4.0%、C: 0.03〜0.10%、酸可
溶性1/!:0.015〜0.040%、N : 0.
0040〜0.0100%、S : 0.01〜0.0
4%、Mn:0.02〜0.2%、0.4%以下のSn
、  Cuの1種または2種が含有されており、残部F
eおよび不可避的不純物からなることが必要である。
The components of the hot rolled sheet which is the starting material of the present invention are Si:
2.5-4.0%, C: 0.03-0.10%, acid solubility 1/! : 0.015-0.040%, N: 0.
0040-0.0100%, S: 0.01-0.0
4%, Mn: 0.02-0.2%, 0.4% or less Sn
, contains one or two types of Cu, and the remainder is F.
e and unavoidable impurities.

以下、本発明において出発素材である熱延板の成分を規
定した理由について説明する。
The reasons for specifying the components of the hot-rolled sheet as a starting material in the present invention will be explained below.

Siは4%を超すと脆化が激しく冷間圧延が困難となり
好ましくない。−・方2.5%未満では電気抵抗が低く
良好な鉄損特性を得難い。
If Si exceeds 4%, embrittlement becomes severe and cold rolling becomes difficult, which is not preferable. -・If it is less than 2.5%, the electrical resistance is low and it is difficult to obtain good iron loss characteristics.

Cは0.03%未満では脱炭工程以前でのT量が極めて
少なくなってしまい良好な1次再結晶組織を得難い。 
・方0.10%を超えると脱炭不良となり好ましくない
If C is less than 0.03%, the amount of T before the decarburization process becomes extremely small, making it difficult to obtain a good primary recrystallized structure.
- If it exceeds 0.10%, decarburization will be poor, which is not preferable.

酸可溶性へ/2.  Nは本発明において高磁束密度を
得るために必須の主インヒビターiNを得るための基本
成分であり上記範囲を外れると2次再結晶が不安定とな
り好ましくないので酸可溶性へ!は0.015〜0.0
40%、Nは0.0040〜0.0100%とする。
Acid soluble/2. In the present invention, N is a basic component for obtaining the main inhibitor iN, which is essential for obtaining a high magnetic flux density, and if it is out of the above range, secondary recrystallization becomes unstable, which is not preferable, so it should be acid-soluble! is 0.015~0.0
40%, and N is 0.0040 to 0.0100%.

また、MnおよびSはインヒビターMnSを形成するた
めに必要な元素であり、上記範囲を外れると2次再結晶
が不安定となり好ましくないのでMnは0.02〜0.
2%、Sは0.O1〜0.04%と定める。
Further, Mn and S are elements necessary to form the inhibitor MnS, and if outside the above range, secondary recrystallization becomes unstable, which is not preferable, so Mn is 0.02 to 0.0.
2%, S is 0. It is set as O1 to 0.04%.

インヒビター構成元素としては、これらの他に0.4%
以下のSn、 Cuの1種または2種が含有されること
が必要である。上限値は、この値を超えると2次再結晶
の成長が害されるので厳守せねばならない。
In addition to these inhibitor constituent elements, 0.4%
It is necessary that one or two of the following Sn and Cu be contained. The upper limit value must be strictly adhered to since the growth of secondary recrystallization will be impaired if this value is exceeded.

尚、インヒビター構成元素として、それ自体公知である
Sb、 Cr、 Se等を用いることも勿論できる。
Incidentally, it is of course possible to use Sb, Cr, Se, etc., which are known per se, as inhibitor constituent elements.

本発明は前記成分を含有する珪素鋼熱延板を出発素材と
して、これに熱延板焼鈍を行ない、次いで2回以上の冷
間圧延を行って最終板厚を0.10〜0.23 Ilm
となし、その間の中間焼鈍と最終冷間圧延後の脱炭焼鈍
及び仕上焼鈍を施す工程を前提としている。この様な製
造方法により板厚0.14mmまでの2次再結晶は比較
的安定化するが、磁束密度が低下する傾向を示すため、
低鉄損値は得られ難い。
The present invention uses a hot-rolled silicon steel sheet containing the above-mentioned components as a starting material, performs hot-rolled sheet annealing, and then cold-rolls it two or more times to obtain a final sheet thickness of 0.10 to 0.23 Ilm.
It is assumed that the process includes intermediate annealing in between, decarburization annealing after final cold rolling, and final annealing. Although secondary recrystallization up to a plate thickness of 0.14 mm is relatively stable using this manufacturing method, the magnetic flux density tends to decrease.
It is difficult to obtain low iron loss values.

本発明者らは上記工程を前提として、熱間圧延後最終冷
間圧延前の途中工程において、Cを0.0070〜0.
0300%の量だけ脱炭することにより、板厚0.10
mmまでの2次再結晶を可能にすると共に、磁束密度と
鉄を員を大幅に向上せしめ得たものである。
Based on the above process, the present inventors added C from 0.0070 to 0.000 in an intermediate process after hot rolling and before final cold rolling.
By decarburizing by 0.30%, the plate thickness is reduced to 0.10.
This makes it possible to perform secondary recrystallization up to mm, and also significantly improves magnetic flux density and iron content.

般に熱間圧延時に生ずる鋼中のγ相は、大きく成長した
粗大伸長粒組織を微細に改善するのに有効で、2次再結
晶が成長する素地を良好ならしめるため、線状に発生す
る非2次再結晶域の発生を抑制する作用を持っている。
Generally, the γ phase in steel that is generated during hot rolling is effective in finely improving the coarsely elongated grain structure that has grown significantly, and it is generated in a linear shape to provide a good substrate for secondary recrystallization to grow. It has the effect of suppressing the occurrence of non-secondary recrystallization regions.

それ故通量のγ相を生ゼしめるために、Si量に応じて
製鋼段階で適量のclを加えて居くことが不可欠である
。またCは製品に残留すると磁気時効を生じるために、
途中工程で脱炭する必要がある。また、2次再結晶を起
こさせる仕上焼鈍工程の前に脱炭工程を置くことは2次
再結晶焼鈍中にγ相の発生が生じて目的とする方位粒の
発生・成長を阻害する弊害を無くす上で必要である。以
上の様な理由から方向性電磁鋼板の製造工程において脱
炭工程は必要不可欠の工程である。
Therefore, in order to generate a sufficient amount of γ phase, it is essential to add an appropriate amount of Cl at the steel manufacturing stage depending on the amount of Si. In addition, C causes magnetic aging if it remains in the product, so
It is necessary to decarburize in the middle of the process. In addition, placing the decarburization process before the final annealing process that causes secondary recrystallization can prevent the generation of γ phase during secondary recrystallization annealing, which inhibits the generation and growth of the desired oriented grains. It is necessary to eliminate it. For the above reasons, the decarburization step is an essential step in the manufacturing process of grain-oriented electrical steel sheets.

以下に本発明の特徴である熱間圧延後最終冷間圧延まで
の工程でCを0.0070〜0.0300%の量だけ脱
炭すると、磁性が良くなる理由と、Cの範囲規制の理由
を説明する。
Below are the reasons why magnetism improves when C is decarburized by an amount of 0.0070 to 0.0300% in the process from hot rolling to final cold rolling, which is a feature of the present invention, and the reason for regulating the range of C. Explain.

先ず、第1図に最終冷延前の鋼板の金属組織写真を掲げ
る。
First, Figure 1 shows a photograph of the metallographic structure of a steel sheet before final cold rolling.

出発材としての熱延板の板厚は2.3mmで、(A)は
かかる熱延板を圧下率53%で冷間圧延して1.07m
mとし、引続きN290%、11.10%の乾燥混合ガ
ス中で1130°Cに30秒間保持したのち900°C
に1分間保持し、その後100°Cの湯に入れて冷却し
たもの、(B)は熱延板をN290%、N210%の乾
燥混合ガス中で1100’Cに2分間保持した後、10
0°Cの湯に入れて冷却した後に(A)と同一条件で冷
間圧延、焼鈍を行なったものであり、(C)は熱延板を
N290%、Nz10%の湿潤ガス(露点65°C)中
で1100°Cに2分間保持した後、100°Cの湯に
入れ、次いで(A)と同一条件で冷間圧延、焼鈍を行な
ったものである。
The thickness of the hot-rolled sheet as a starting material is 2.3 mm, and (A) is 1.07 m by cold-rolling the hot-rolled sheet at a reduction rate of 53%.
m, then held at 1130°C for 30 seconds in a dry mixed gas of 90% N2 and 11.10%, and then heated to 900°C.
(B) is a hot-rolled sheet that was held at 1100'C for 2 minutes in a dry mixed gas of 90% N2 and 10% N2, and then cooled in hot water at 100°C.
After cooling in hot water at 0°C, cold rolling and annealing were performed under the same conditions as in (A). In (C), the hot rolled sheet was heated in a wet gas containing 90% N2 and 10% Nz (dew point 65°). After being held at 1100°C for 2 minutes in C), it was placed in hot water at 100°C, and then cold rolled and annealed under the same conditions as in (A).

第1図の(B)、(C)は熱延板焼鈍工程が導入されて
いるため、熱延板焼鈍をしていない(A)に比較してこ
の段階で充分再結晶の発達がなされていることが判り、
後続の最終焼鈍、脱炭焼鈍工程後の組織がより均一にな
ることが理解出来よう。
In (B) and (C) of Figure 1, the hot-rolled sheet annealing process has been introduced, so recrystallization has developed sufficiently at this stage compared to (A) where the hot-rolled sheet is not annealed. I found out that there was
It can be seen that the structure becomes more uniform after the subsequent final annealing and decarburization annealing steps.

また(B)と(C)の銅板表面部を比較すると、脱炭雰
囲気になっている熱延板焼鈍を行なった(C)の方が、
非脱炭雰囲気焼鈍の(B)よりも表面部の結晶粒がより
大きくなっていることが判る。
Also, when comparing the surface parts of the copper sheets in (B) and (C), the surface area of the copper sheets in (C), which was annealed in a decarburized atmosphere, is better.
It can be seen that the crystal grains in the surface area are larger than in (B), which was annealed in a non-decarburizing atmosphere.

なお、この場合の出発熱延板のC含有量は0.070%
であるが、(A)、(B)では明確な脱炭が認められな
いのに対し、(C)の場合では鋼板全厚で0.0200
%だけ脱炭していた。第1図に示した組織の相違は成品
の2次再結晶の安定性ならびに磁性に大きく影響する。
In addition, the C content of the starting hot rolled sheet in this case is 0.070%
However, in the case of (A) and (B), clear decarburization is not observed, whereas in the case of (C), the total thickness of the steel plate is 0.0200.
% was decarburized. The difference in structure shown in FIG. 1 greatly affects the stability of secondary recrystallization and magnetism of the product.

(A)、(B)、(C)の履歴を有する各10個の試片
を、そののち86%の圧下率で0.15mmまで冷間圧
延し、さらに公知の方法での脱炭焼鈍、l’1goを主
成分とする焼鈍分離剤の塗布、仕上焼鈍、リン酸、無水
クロム酸を主成分とする張力コーティングの塗布、焼付
けを行ない製品とした。第1表に磁性と2次再結晶率に
ついて一覧する。本発明による(C)が他の場合に比較
し一段と優れていることが判る。
Ten specimens each having histories of (A), (B), and (C) were then cold rolled to 0.15 mm at a reduction rate of 86%, and then decarburized and annealed by a known method. A product was obtained by applying an annealing separator containing l'1go as a main component, finishing annealing, applying a tension coating containing phosphoric acid and chromic anhydride as main components, and baking. Table 1 lists the magnetism and secondary recrystallization rate. It can be seen that (C) according to the present invention is much better than other cases.

第   1   表 (n=10の平均値) 次に、第2図には熱間圧延後最終冷間圧延までの工程で
の脱炭量ΔCと磁気特性との関係を示す。
Table 1 (Average value of n=10) Next, FIG. 2 shows the relationship between the amount of decarburization ΔC and magnetic properties in the process from hot rolling to final cold rolling.

この場合の熱延板の板厚は2.3mmでありSi3.2
5%、C0,078%、酸可溶性へ1.027%、NO
,0083%を含有したもので、1050°Cでの熱延
板焼鈍、第1回目の冷間圧延ののち、1100°Cで中
間焼鈍し、80〜91%の弾圧下最終冷間圧延を行なっ
て最終板厚0.175 mmのサンプルを得、公知の脱
炭焼鈍、MgOa主成分とする焼鈍分離剤塗布、仕上焼
鈍を行ない、最終的にリン酸、無水クロム酸を主成分と
する張力コーティングを施こしたものである。
The thickness of the hot-rolled plate in this case is 2.3 mm, and the Si3.2
5%, CO 0,078%, acid soluble 1.027%, NO
, 0083%, and after hot-rolled plate annealing at 1050°C, first cold rolling, intermediate annealing at 1100°C, and final cold rolling under 80-91% elastic pressure. A sample with a final plate thickness of 0.175 mm was obtained, followed by known decarburization annealing, application of an annealing separator mainly composed of MgOa, and final annealing, and finally a tension coating mainly composed of phosphoric acid and chromic anhydride. It has been subjected to

なお、この工程途上、熱延板焼鈍工程、中間焼鈍工程名
々あるいは単独に雰囲気ガスの露点を変える方法での脱
炭、ならびに熱延板焼鈍工程、中間焼鈍工程の通板の前
に鋼板表面にKzCO:+水溶液を塗布する方法での脱
炭により各種の脱炭量のサンプルを得ることが出来た。
During this process, decarburization is performed by changing the dew point of the atmospheric gas during the hot-rolled plate annealing process, intermediate annealing process, or by changing the dew point of the atmospheric gas, and the steel plate surface is Samples with various amounts of decarburization could be obtained by decarburizing by applying a KzCO:+ aqueous solution to the steel.

第2図より、脱炭量ΔC0,0070〜0.0300%
の範囲で良好な磁性が得られることが判る。第2図に示
した新知見の理由に関しては必ずしも明らかではないが
、本発明者らは以下の如く推察している。
From Figure 2, decarburization amount ΔC0,0070~0.0300%
It can be seen that good magnetism can be obtained within the range of . Although the reason for the new findings shown in FIG. 2 is not necessarily clear, the present inventors speculate as follows.

まず・方向性電磁鋼板用熱延板に(A ) KzCOs
30%水溶液を塗布したもの、(B)塗布しないもの各
々をNz90%、11□10%からなる乾燥の混合ガス
中で1050°Cに2分間保持した後、100°Cの湯
の中に入れて冷却したものの光学顕微鏡写真を第3図に
示す。熱延板でのclは0.072%であり、熱延板焼
鈍での脱炭量は(A)の場合:ΔC−〇、0150%、
(B)の場合:ΔC=0.0030%であった。第3図
より、(A)の場合は(B)の場合よりも表面の再結晶
領域が広いことがわかる。他方、最終圧下率が80%を
超える1回弾圧下冷延法の場合、熱延板焼鈍後の表面再
結晶部分を削ると製品の2次再結晶が不安定となること
が知られている。従って(A)の如く、脱炭によって表
面再結晶部分を増したことが製品の2次再結晶の安定化
並びに磁性向上に結び付いたものと思われる。
First, (A) KzCOs for hot-rolled sheets for grain-oriented electrical steel sheets.
The one coated with the 30% aqueous solution and the one not coated (B) were each kept at 1050°C for 2 minutes in a dry mixed gas consisting of 90% Nz and 10% Nz, and then placed in hot water at 100°C. Fig. 3 shows an optical micrograph of the sample after cooling. Cl in the hot rolled sheet is 0.072%, and the amount of decarburization in hot rolled sheet annealing is (A): ΔC-〇, 0150%,
In the case of (B): ΔC=0.0030%. From FIG. 3, it can be seen that the recrystallized region on the surface is wider in case (A) than in case (B). On the other hand, in the case of the single compression cold rolling method where the final rolling reduction exceeds 80%, it is known that the secondary recrystallization of the product becomes unstable if the surface recrystallized portion after hot-rolled sheet annealing is removed. . Therefore, as shown in (A), it is thought that increasing the surface recrystallized portion by decarburization leads to stabilization of secondary recrystallization and improvement of magnetism of the product.

(A)の如く脱炭によって表面再結晶層を増したものは
、第1図の(C)に示した様に、最終冷延前の表面の深
い領域まで再結晶粒が内部のものよりも大きくなる。板
厚が0.10〜0.23mmと薄くなった場合、2次再
結晶の核がある表面層が幾何学的に薄くなってしまい、
かつ最表面に近くなるため仕上焼鈍の昇温過程で2次再
結晶の核のある表面層が雰囲気の影響をうけやすくなり
、その結果2次再結晶が不安定化し、良好な磁性が得難
くなる。
As shown in (A), the surface recrystallized layer is increased by decarburization, and as shown in (C) of Figure 1, the recrystallized grains are deeper in the surface than the inner part before the final cold rolling. growing. When the plate thickness becomes as thin as 0.10 to 0.23 mm, the surface layer containing the secondary recrystallization nuclei becomes geometrically thinner.
In addition, since it is close to the outermost surface, the surface layer containing the nuclei of secondary recrystallization becomes susceptible to the influence of the atmosphere during the heating process of finish annealing, and as a result, secondary recrystallization becomes unstable and it is difficult to obtain good magnetism. Become.

本発明は、熱延後最終冷延までの工程途中で、脱炭を行
なうことで、表面再結晶部を深くまで作ることによって
2次再結晶の核を深くまで存在させることに成功し、そ
の結果最終冷間圧延を80%超の高圧下率で行なっても
より薄い板厚の場合の2次再結晶の安定化ならびに磁性
向上をなし得たものである。
In the present invention, by performing decarburization during the process from hot rolling to final cold rolling, the surface recrystallization zone is created deep, thereby successfully allowing the secondary recrystallization nuclei to exist deep down. As a result, even if the final cold rolling was carried out at a high reduction rate of over 80%, it was possible to stabilize secondary recrystallization and improve magnetism in the case of a thinner plate.

熱間圧延終了後最終冷間圧延までの脱炭量ΔCが0.0
070%未満の場合には上記の効果が十分でなく 、0
.0300%を超える場合は熱延板焼鈍、中間焼鈍での
γ相の量が少なくなり過ぎてしまうため、脱炭焼鈍工程
後の1次再結晶組織が不適切なものとなるためと、An
Nの析出が粗大なものとなってインヒビターの作用が減
少するために2次再結晶が不安定になるものと推定され
る。本発明は板厚の薄い一方向性電磁鋼板の製造上の問
題を解決したものであり、0.23mmを超える板厚の
場合、必ずしも本発明の様な工程は必要でなく、0.1
0mm未満の板厚では、本発明の効果だけでは不十分で
2次再結晶に不安定性が生しる。最終冷延圧下率は80
%超とすることが高磁束密度を得るために必要であり、
95%を超えると集合組織が不適となるので2次再結晶
に不安定性が生じる。
The amount of decarburization ΔC from the end of hot rolling to the final cold rolling is 0.0
If it is less than 0.070%, the above effect is not sufficient, and 0.
.. If it exceeds 0300%, the amount of γ phase in hot-rolled sheet annealing and intermediate annealing becomes too small, resulting in an inappropriate primary recrystallized structure after the decarburization annealing process.
It is presumed that the secondary recrystallization becomes unstable because the N precipitation becomes coarse and the effect of the inhibitor is reduced. The present invention solves the problem in manufacturing thin unidirectional electrical steel sheets, and when the thickness exceeds 0.23 mm, the process of the present invention is not necessarily necessary.
When the plate thickness is less than 0 mm, the effect of the present invention is insufficient and instability occurs in secondary recrystallization. The final cold rolling reduction is 80
% is necessary to obtain high magnetic flux density,
If it exceeds 95%, the texture becomes inappropriate, resulting in instability in secondary recrystallization.

熱間圧延の後、最終冷間圧延の間での脱炭の方法につい
ては必ずしも限定しないが、熱延巻取後自己の熱で焼鈍
する方法、あるいは700〜1200°Cの温度範囲で
の熱延板焼鈍、中間焼鈍を湿潤ガス中で行なう方法、又
は、それら焼鈍前にに2C03等を塗布する方法などが
考えられる。
The method of decarburization during the final cold rolling after hot rolling is not necessarily limited, but may include a method of annealing with its own heat after hot rolling and winding, or a method of decarburizing in the temperature range of 700 to 1200 ° C. Possible methods include performing rolling annealing and intermediate annealing in a wet gas, or applying 2C03 or the like before these annealing.

以下、実施例について述べる。Examples will be described below.

(実施例) 実施例I C: 0.065%、Si : 3.25%、Mn :
 0.088%、S: 0.026%酸可溶性A f 
: 0.028%、N :0.0075%、Sn : 
0.10%、Cu : 0.10%を含む2.3mmの
熱延板に(A)  :980°Cで2分間、湿潤雰囲気
(n点: 62’C)N2ガス中で焼鈍、(B):98
0°Cで2分間乾燥雰囲気N2ガス中で焼鈍、(C):
焼鈍ナシなる処理をした後、酸洗し、約41%冷間圧延
して1、35 mPAとした。その後乾燥雰囲気N29
0%、■!10%ガス中で1130°Cに30秒保持後
、900°Cに1分間保持後急冷し、しかる後約83%
冷間圧延して0.225 no++とじた。得られた冷
延板を公知の方法で脱炭焼鈍し、焼鈍分離剤を塗布した
後、N2:90%、H210%雰囲気中で15°C/h
rの割合で1200°Cまで昇温し、引続き1200°
Cで20時間の純化焼鈍を行なった後、張力コーティン
グを施して・方向性電磁鋼板を得た。製品の磁気特性、
熱延終了後最終冷間圧延までの脱炭量ΔC(%)を第2
表に示す。
(Example) Example I C: 0.065%, Si: 3.25%, Mn:
0.088%, S: 0.026% acid soluble A f
: 0.028%, N: 0.0075%, Sn:
0.10%, Cu: 0.10% (A): Annealed at 980 °C for 2 minutes in a humid atmosphere (point n: 62'C) in N2 gas, (B ):98
Annealing in a dry atmosphere N2 gas for 2 minutes at 0 °C, (C):
After no annealing, it was pickled and cold rolled by about 41% to 1.35 mPA. After that, drying atmosphere N29
0%, ■! After holding at 1130°C for 30 seconds in 10% gas, holding at 900°C for 1 minute and rapidly cooling, then about 83%
Cold rolled to 0.225 no++ finish. The obtained cold-rolled sheet was decarburized and annealed by a known method, coated with an annealing separator, and heated at 15°C/h in an atmosphere of 90% N2 and 10% H2.
Raise the temperature to 1200°C at a rate of r, then continue to 1200°
After performing purification annealing at C for 20 hours, tension coating was applied to obtain a grain-oriented electrical steel sheet. magnetic properties of the product,
The amount of decarburization ΔC (%) from the end of hot rolling to the final cold rolling is calculated as the second
Shown in the table.

第   2   表 実施例2 C:  0.081%、Si : 3.35%、Mn 
:  0.077%、S:  0.024%、酸可溶性
へff:0.027%、N : 0.0082%、Sn
:0.15%、Cu : 0.15%を含む板厚2.3
mmの熱延板を、(A)  :1050°Cで3分間、
湿潤雰囲気(露点:55°c)Nz:90%、Hz :
 10%ガス中で焼鈍、(B):1050°Cで3分間
、乾燥雰囲気N2:90%、Hz:10%ガス中で焼鈍
、(C):焼鈍ナシなる処理をした後酸洗し、約49%
の圧下率で冷間圧延して1.2mmとした。その後乾燥
雰囲気N290%、11□10%ガス中で1080°C
に2分間保持後急冷し、しかる後約85%の圧下率で冷
間圧延して0.175mmとした。得られた冷延板を公
知の方法で脱炭焼鈍し、MgOを主成分とする焼鈍分離
剤を塗布した後、仕上焼鈍を行なった。次いでリン酸と
無水クロム酸を主成分とする張力コーティングを施して
一方向性電磁鋼板を得た。製品の磁気特性、熱延終了後
最終冷延までの脱炭量ΔC(%)を第3表に示す。
Table 2 Example 2 C: 0.081%, Si: 3.35%, Mn
: 0.077%, S: 0.024%, acid soluble ff: 0.027%, N: 0.0082%, Sn
: 0.15%, plate thickness 2.3 including Cu: 0.15%
mm hot-rolled plate (A): 3 minutes at 1050°C,
Humid atmosphere (dew point: 55°c) Nz: 90%, Hz:
Annealed in 10% gas, (B): Annealed at 1050°C for 3 minutes, dry atmosphere N2: 90%, Hz: 10% gas, (C): No annealing, then pickled, approx. 49%
It was cold rolled at a reduction rate of 1.2 mm. After that, it was heated to 1080°C in a dry atmosphere of N290%, 11□10% gas.
After being held for 2 minutes, it was rapidly cooled, and then cold-rolled to a thickness of 0.175 mm at a rolling reduction of about 85%. The obtained cold-rolled sheet was decarburized and annealed by a known method, coated with an annealing separator containing MgO as a main component, and then finished annealed. Next, a tension coating containing phosphoric acid and chromic anhydride as main components was applied to obtain a grain-oriented electrical steel sheet. Table 3 shows the magnetic properties of the product and the amount of decarburization ΔC (%) from the end of hot rolling to the final cold rolling.

第   3   表 実施例3 C: 0.072%、Si : 3.25%、Mn :
 0.075%、S:0.028%、酸可溶性7/! 
:  0.025%、N:0.0082%、Sn ; 
0.12%、Cu : 0.19%を含む厚さ2.3m
mの熱延板に(A) K、CO330%水溶液を塗布、
(B)塗布ナシなる処理をした後、1100°Cで3分
間、乾燥雰囲気Nz : 90%、Hz:10%ガス中
で焼鈍後急冷し、その後酸洗し、約53%の圧下率で冷
間圧延して1.07mmとした。しかる後乾燥雰囲気N
2ガス中で1000°Cで2分間焼鈍し、約86%の圧
下率で冷間圧延して0.150 mmとした。得られた
冷延板を公知の方法で脱炭焼鈍し、焼鈍分離剤を塗布し
、仕上焼鈍を行なった。次いでリン酸、無水クロム酸を
主成分とする張力コーティングを施して、一方向性電磁
鋼板を得た。製品の磁気特性、熱延後最終冷延までの脱
炭量ΔC(%)を第4裏に示す。
Table 3 Example 3 C: 0.072%, Si: 3.25%, Mn:
0.075%, S: 0.028%, acid soluble 7/!
: 0.025%, N: 0.0082%, Sn;
0.12%, Cu: 2.3m thick including 0.19%
(A) Apply a 30% K, CO3 aqueous solution to a hot-rolled sheet of m.
(B) After treatment without coating, annealing at 1100°C for 3 minutes in a dry atmosphere Nz: 90%, Hz: 10% gas, followed by rapid cooling, followed by pickling and cooling at a reduction rate of approximately 53%. It was rolled to a thickness of 1.07 mm. Afterwards drying atmosphere N
It was annealed at 1000°C for 2 minutes in 2 gases and cold rolled to a thickness of 0.150 mm at a reduction of about 86%. The obtained cold-rolled sheet was decarburized and annealed by a known method, coated with an annealing separator, and finished annealed. Next, a tension coating containing phosphoric acid and chromic anhydride as main components was applied to obtain a grain-oriented electrical steel sheet. The magnetic properties of the product and the amount of decarburization ΔC (%) from hot rolling to final cold rolling are shown on the fourth back.

第   4   表 実施例4 C: 0.072%、Si : 3.40%、Mn :
 0.078%、S二0.026%、酸可溶性^f :
  0.029%、N:0.0080%、Sn : 0
.09%、Cu : 0.06%、Sb : 0.02
8%を含む厚さ2.3mmの熱圧延に1000’Cに5
分間、乾燥雰囲気J:90%、N2:10%ガス中で焼
鈍した後、酸洗し、約22%の圧下率で冷間圧延して1
.8 m+nとした。その後(A) 1120°Cで4
分間、乾燥雰囲気Ng;90%、11□:10%ガス中
で焼鈍後、象、冷、(B)1120°Cで4分間、湿潤
雰囲気(露点:60”C)Nz:90%、lh:10%
ガス中で焼鈍した後、急冷、なる処理をした後、酸洗し
、約89%の圧下率で冷間圧延して0.20抛鍋とした
。その後冷延板を公知の方法で脱炭焼鈍し、焼鈍分離剤
を塗布し仕上焼鈍した後張力コーティングを施して一方
向性電磁鋼板を得た。製品の磁気特性、熱間圧延終了後
、最終冷間圧延までの脱炭量ΔC(%)を第5表に示す
Table 4 Example 4 C: 0.072%, Si: 3.40%, Mn:
0.078%, S2 0.026%, acid soluble^f:
0.029%, N: 0.0080%, Sn: 0
.. 09%, Cu: 0.06%, Sb: 0.02
5% hot rolled at 1000'C to a thickness of 2.3mm containing 8%
After annealing in a dry atmosphere J: 90%, N2: 10% gas for 1 minute, pickling and cold rolling at a reduction rate of about 22%.
.. 8 m+n. Then (A) 4 at 1120°C
minutes, dry atmosphere Ng: 90%, 11□: After annealing in 10% gas, elephant, cold, (B) 4 minutes at 1120°C, humid atmosphere (dew point: 60”C) Nz: 90%, lh: 10%
After annealing in a gas, the material was rapidly cooled, then pickled, and cold-rolled at a rolling reduction of about 89% to form a 0.20 mm ladle. Thereafter, the cold rolled sheet was decarburized and annealed by a known method, coated with an annealing separator, final annealed, and then tension coated to obtain a unidirectional electrical steel sheet. Table 5 shows the magnetic properties of the product and the amount of decarburization ΔC (%) from the end of hot rolling to the final cold rolling.

第   5   表 (発明の効果) 以上のとおり、本発明によれば最終冷間圧延前の含有炭
素量を制御するだけで鉄損特性の良好な高磁束密度薄手
−・方向性電磁鋼板を安定して得ることができるので、
その工業的効果は大きい。
Table 5 (Effects of the Invention) As described above, according to the present invention, a thin, high magnetic flux density, grain-oriented electrical steel sheet with good iron loss characteristics can be stabilized simply by controlling the carbon content before final cold rolling. Since you can get
Its industrial effects are significant.

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

第1図は最終冷間圧延前の金属組織の比較顕微鏡写真、
第2図は熱間圧延後最終冷間圧延までの脱炭量ΔCと磁
気特性との関係図、第3図は熱延板焼鈍後の金属組繊の
比較顕微鏡写真である。 第1s (A) 第3 f B : 0.2  mm 第2図
Figure 1 is a comparative micrograph of the metal structure before final cold rolling.
FIG. 2 is a diagram showing the relationship between the amount of decarburization ΔC after hot rolling and the final cold rolling and magnetic properties, and FIG. 3 is a comparative microscopic photograph of the metal composite fibers after annealing the hot rolled sheet. 1st s (A) 3rd f B: 0.2 mm Fig. 2

Claims (1)

【特許請求の範囲】[Claims] Si:2.5〜4.0%、C:0.03〜0.10%、
酸可溶性Al:0.015〜0.040%、N:0.0
040〜0.0100%、S:0.01〜0.04%、
Mn:0.02〜0.2%を含有し、さらに0.4%以
下のSn、Cuの1種または2種を含有し、残部Feお
よび不可避的不純物からなる珪素鋼熱延板を焼鈍し、圧
下率80%超〜95%の弾圧下最終冷間圧延を含む2回
以上の冷間圧延とその間に行う中間焼純と、最終冷間圧
延後の脱炭焼鈍、最終仕上焼鈍によって板厚が0.10
〜0.23mmの高磁束密度の薄手一方向性電磁鋼板を
製造する方法において、熱間圧延終了後最終冷間圧延前
の工程途中に、Cを0.0070〜0.0300%脱炭
させる工程を有することを特徴とする鉄損の少ない一方
向性電磁鋼板の製造方法。
Si: 2.5-4.0%, C: 0.03-0.10%,
Acid-soluble Al: 0.015-0.040%, N: 0.0
040-0.0100%, S: 0.01-0.04%,
A silicon steel hot-rolled sheet containing Mn: 0.02 to 0.2%, further containing 0.4% or less of one or both of Sn and Cu, and the balance consisting of Fe and inevitable impurities is annealed. The plate thickness is improved by two or more cold rollings including final cold rolling under compression at a rolling reduction of more than 80% to 95%, intermediate annealing performed in between, decarburization annealing after the final cold rolling, and final finish annealing. is 0.10
In a method for manufacturing a thin unidirectional electrical steel sheet with a high magnetic flux density of ~0.23 mm, a step of decarburizing C by 0.0070 to 0.0300% during the process after hot rolling and before final cold rolling. A method for producing a unidirectional electrical steel sheet with low iron loss, characterized by having the following.
JP2194496A 1990-07-23 1990-07-23 Manufacturing method of grain-oriented electrical steel sheet with low iron loss Expired - Lifetime JPH0781166B2 (en)

Priority Applications (1)

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Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2194496A JPH0781166B2 (en) 1990-07-23 1990-07-23 Manufacturing method of grain-oriented electrical steel sheet with low iron loss

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP59228014A Division JPS61117215A (en) 1984-10-31 1984-10-31 Manufacture of grain oriented magnetic steel sheet of low iron loss

Publications (2)

Publication Number Publication Date
JPH03219021A true JPH03219021A (en) 1991-09-26
JPH0781166B2 JPH0781166B2 (en) 1995-08-30

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Country Link
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH10259424A (en) * 1997-02-28 1998-09-29 Armco Inc Production of silicon-chromium grain-oriented silicon steel
KR100501005B1 (en) * 2000-12-08 2005-07-18 주식회사 포스코 A method for manufacturing grain oriented electrical steel sheet

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5239520A (en) * 1975-09-08 1977-03-26 Allegheny Ludlum Ind Inc Making process of anisotropic silicon steel saved the growth of nitride alluminium
JPS55154526A (en) * 1979-05-21 1980-12-02 Allegheny Ludlum Ind Inc Treating method of cubic oriented silicon steel
JPS5932528A (en) * 1982-08-18 1984-02-22 Nissan Motor Co Ltd Vehicle light control device
JPS61117215A (en) * 1984-10-31 1986-06-04 Nippon Steel Corp Manufacture of grain oriented magnetic steel sheet of low iron loss

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5239520A (en) * 1975-09-08 1977-03-26 Allegheny Ludlum Ind Inc Making process of anisotropic silicon steel saved the growth of nitride alluminium
JPS55154526A (en) * 1979-05-21 1980-12-02 Allegheny Ludlum Ind Inc Treating method of cubic oriented silicon steel
JPS5932528A (en) * 1982-08-18 1984-02-22 Nissan Motor Co Ltd Vehicle light control device
JPS61117215A (en) * 1984-10-31 1986-06-04 Nippon Steel Corp Manufacture of grain oriented magnetic steel sheet of low iron loss

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH10259424A (en) * 1997-02-28 1998-09-29 Armco Inc Production of silicon-chromium grain-oriented silicon steel
KR100501005B1 (en) * 2000-12-08 2005-07-18 주식회사 포스코 A method for manufacturing grain oriented electrical steel sheet

Also Published As

Publication number Publication date
JPH0781166B2 (en) 1995-08-30

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