JPH01230721A - Manufacture of grain-oriented silicon steel sheet having high saturation magnetic flux density - Google Patents

Manufacture of grain-oriented silicon steel sheet having high saturation magnetic flux density

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Publication number
JPH01230721A
JPH01230721A JP63109880A JP10988088A JPH01230721A JP H01230721 A JPH01230721 A JP H01230721A JP 63109880 A JP63109880 A JP 63109880A JP 10988088 A JP10988088 A JP 10988088A JP H01230721 A JPH01230721 A JP H01230721A
Authority
JP
Japan
Prior art keywords
annealing
magnetic flux
flux density
silicon steel
grain
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
JP63109880A
Other languages
Japanese (ja)
Other versions
JPH0686630B2 (en
Inventor
Nobuyuki Takahashi
延幸 高橋
Yozo Suga
菅 洋三
Katsuro Kuroki
黒木 克郎
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 Steel Corp
Original Assignee
Nippon Steel 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 Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP63109880A priority Critical patent/JPH0686630B2/en
Priority to DE88118993T priority patent/DE3882502T2/en
Priority to EP88118993A priority patent/EP0321695B1/en
Priority to US07/274,432 priority patent/US4994120A/en
Priority to KR1019880015250A priority patent/KR930001330B1/en
Publication of JPH01230721A publication Critical patent/JPH01230721A/en
Publication of JPH0686630B2 publication Critical patent/JPH0686630B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Manufacturing Of Steel Electrode Plates (AREA)

Abstract

PURPOSE:To manufacture a grain-oriented silicon steel sheet having high magnetic flux density by successively subjecting a hot rolled sheet contg. specified amts. of Si, Al, Ti, N, B and S and/or Se to cold rolling, decarburization annealing in wet hydrogen, coating with a protective coating material for annealing, finish annealing and nitriding. CONSTITUTION:A hot rolled sheet contg., by weight, 1.5-4.8% Si, 0.012-0.05% AC, 0.002-0.012% Ti, 0.001-0.012% N, 0.0005-0.008% B and <=0.012%, in total, of S and/or Se satisfying Mn/(S+Se)>=4 is cold rolled once or more, decarburization-annealed in wet hydrogen, coated with a protective coating material for annealing and finish-annealed. The sheet is further nitrided in a heating stage between the end of the final cold rolling and the beginning of secondary recrystallization during the finish annealing. A grain-oriented silicon steel sheet having high magnetic flux density can be manufactured.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、電機器の鉄心に用いられる一方向性珪素綱板
の製造における基本冶金現象として利用するところの、
二次再結晶の発現に対して有効な析出′+yJ(一般に
インヒビターと呼ばれている)として、新規な成分組合
せを提示し、これにより磁束密度の高い一方向性珪素綱
板の製造を可能にするものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention utilizes basic metallurgical phenomena in the production of unidirectional silicon steel sheets used in iron cores of electrical equipment.
We proposed a new combination of ingredients as a precipitate '+yJ (generally called an inhibitor) that is effective against the development of secondary recrystallization, making it possible to manufacture unidirectional silicon steel plates with high magnetic flux density. It is something to do.

〔従来の技術〕[Conventional technology]

一方向性珪素綱板は綱板面が(110)面で、圧延方向
が< 100>軸を有するいわゆるゴス方位(ミラー指
数で(110)  < 001>方位を表わす)を持つ
結晶粒から構成されており、軟磁性材料として変圧器お
よび発電機用の鉄心に使用される。
The unidirectional silicon steel plate is composed of crystal grains having the so-called Goss orientation (expressed as the (110) <001> orientation in Miller index), with the steel plate plane being the (110) plane and the rolling direction having the <100> axis. It is used as a soft magnetic material in the cores of transformers and generators.

この綱板は磁気特性として磁化特性と鉄損特性が良好で
なければならない。磁化特性の良否はかけられた一定の
磁場中で鉄心内に誘起される磁束密度の高低で決まり、
磁束密度の高い製品では鉄心を小型化出来る。磁束密度
の高さは綱板結晶粒の方位を< 110)  < OO
Hに高度に揃えることによって達成出来る。
This steel plate must have good magnetic properties such as magnetization properties and iron loss properties. The quality of magnetization characteristics is determined by the level of magnetic flux density induced within the iron core in a constant magnetic field.
For products with high magnetic flux density, the iron core can be made smaller. The height of the magnetic flux density is determined by the orientation of the steel plate grains < 110) < OO
This can be achieved by highly aligning with H.

鉄損は鉄心に所定の交流磁場を与えた場合に熱エネルギ
ーとして消費される電力[4失であり、その良否に対し
て磁束密度、板厚、不純物量、比抵抗、結晶粒大きさ等
が影響する。
Iron loss is the electric power [4 losses] consumed as thermal energy when a specified alternating magnetic field is applied to the iron core. Affect.

磁束密度の高い綱板は電気機器の鉄心を小さく 。Steel plates with high magnetic flux density make the iron core of electrical equipment smaller.

出来、また鉄(員も少なくなるので望ましく、当該技術
分野では出来る限り磁束密度の高い製品を安いコストで
製造する方法の開発が課題である。
This is desirable because it reduces the amount of magnetic flux that can be produced and requires less iron, and the challenge in this technical field is to develop a method for producing products with as high a magnetic flux density as possible at a low cost.

特に最近は磁区細分化技術が開発され、高い磁束密度を
有する材料はど低い鉄I員値のものが得られるようにな
ってきている。
In particular, recently, magnetic domain refining technology has been developed, and it has become possible to obtain materials with high magnetic flux densities with very low iron I-member values.

ところで、一方向性珪素綱板は、熱延板を適切な冷延と
焼鈍との組合せにより最終板厚になった綱板を仕上焼鈍
することにより (1101< 001>方向を有する
一次再結晶粒を選択成長させる、いわゆる二次再結晶に
よって得られる。二次再結晶は二次再結晶前の綱板中に
微細な析出物、例えばMnS 、  Δj! N  9
MnSe * CuzS+ (八j!、5i)N等が存
在すること、あるいはSn、Sb等の粒界存在型の元素
が存在することによって達成される。これら析出物、粒
界存在型の元素はJ、E、May and D。
By the way, unidirectional silicon steel sheet is produced by finishing annealing the hot-rolled sheet to the final thickness by a combination of appropriate cold rolling and annealing (primary recrystallized grains having the 1101<001> direction). It is obtained by so-called secondary recrystallization, which selectively grows .Secondary recrystallization involves the formation of fine precipitates, such as MnS, Δj!N9, in the steel plate before secondary recrystallization.
This is achieved by the presence of MnSe*CuzS+ (8j!, 5i)N, etc., or by the presence of grain boundary-existing elements such as Sn and Sb. These precipitates and grain boundary-existing elements are described in J, E, May and D.

Turnbull(Trans、tlet、soc、A
IME 212(1958) p769/781)によ
って説明されているように仕上焼鈍工程で(1101<
 001>方位以外の一次再結晶粒の成長を抑え、(1
10)  < 001>方位粒を選択的に成長させる機
能を持つ。このような粒成長の抑制効果は一般にはイン
ヒビター効果と呼ばれている。
Turnbull (Trans, tlet, soc, A
(1101<
The growth of primary recrystallized grains other than the 001> orientation is suppressed, and (1
10) Has the function of selectively growing <001> oriented grains. Such a grain growth suppressing effect is generally called an inhibitor effect.

したがって当該分野の研究開発の重点課題はいかなる種
類の析出物、あるいは粒界存在型の元素を用いて二次再
結晶を安定させるか、そし°ζ正も育な(1101< 
001>方位粒の存在割合を高めるためにそれらの適切
な存在状態をいかに達成するかにある。特に、最近では
一種類の析出物による方法では(110)  < 00
1>方位の高度の制御に限界があるため、各析出物につ
いて短所・長所を深く解明することにより、いくつかの
析出物を有機的に組合せて、より磁束密度の高い製品を
安定に、かつコスト安く製造出来る技術開発が進められ
ている。
Therefore, the key issue for research and development in this field is how to stabilize secondary recrystallization using any kind of precipitates or grain-boundary elements, and how to improve °ζ correction (1101<
The problem lies in how to achieve an appropriate state of existence of grains with a 001> orientation in order to increase their abundance. In particular, recently, in the method using one type of precipitate, (110) < 00
1> Since there is a limit to controlling the height of orientation, by deeply understanding the disadvantages and advantages of each precipitate, it is possible to organically combine several precipitates to produce products with higher magnetic flux density stably and Progress is being made in developing technologies that can be manufactured at low cost.

析出物の種類として、M、F、Littmannは特公
昭30−3651に、J、E、May and D、T
urnbullはTransMet、Soc、AIME
 212(1958)p769/781にMnSを、田
口、板金は特公昭33−4710にΔINとMnSを、
FiedlerはTrans はTrans 、 Me
t、 Soc AIMB 221(1961) p12
01〜1205にVNを、今中らは特公昭51−134
69にMnSe、Sbを、J、A、Salsgiver
は寸特開昭57−45818号公報にAnと硫化銅を、
小松らは特願昭60−179855に(Al 、5i)
Nを開示しており、その他TiS 、 CrS  、 
CrC、NbC、5iOz等が知られている。又粒界存
在型の元素として「日本金属学会誌J 27(1963
)p186斎藤達雄にAs  。
Regarding the types of precipitates, M, F, Littmann in Japanese Patent Publication No. 30-3651, J, E, May and D, T
urnbull is TransMet, Soc, AIME
212 (1958) p769/781 with MnS, Taguchi, sheet metal with ΔIN and MnS with Special Publication Publication No. 33-4710,
Fiedler is Trans, Me
t, Soc AIMB 221 (1961) p12
VN from 01 to 1205, Imanaka is special public service 1977-134
69 with MnSe, Sb, J, A, Salsgiver
In JP-A No. 57-45818, An and copper sulfide are
Komatsu et al. in patent application No. 179855 (Al, 5i)
N, and other TiS, CrS,
CrC, NbC, 5iOz, etc. are known. In addition, as a grain boundary existing element, “Journal of the Japan Institute of Metals J 27 (1963
) As to p186 Tatsuo Saito.

Sn、Sb等が述べられているが工業生産においてはこ
れら元素単独で使用される例は無く、いずれも析出物と
共存させてその補助的効果を狙って使用されている。さ
らに特徴のあるインヒビターとして、II 、 gre
nob l eによる米国特許第3,905,842号
(1975) 、 tl、Fiedlerによる米国特
許第3,905,843号(1975)がある。すなわ
ち固溶のS、B、Nを適当量だけ存在させることによっ
て、磁束密度の高い一方向性珪素綱板の製造を可能にし
ている。二次再結晶に効果のある析出物の選択基準は必
ずしも明らかにされていないが、その代表的見解が検量
により「鉄と鋼J 53(1967) p1007〜1
023に述べられている。要約すると (1)大きさは0.1p程度 (2)必要容積は0.1 vo1%以上(3)二次再結
晶温度範囲で完全に溶けてしまっても全く溶けなくても
不可であり適当な程度固溶する である。上記各種析出物はこれら条件に当てはまる部分
もあるが、全ての現象がこの条件に当てはまるわけでは
無い。最近の冷間圧延以降において綱板を窒化する方法
においては、上記(1)は重要な意味をもたないことが
分った。この様に現状では析出物の選択をする際の指導
原理は確立しておらず、試行錯誤の操り返しで、新しい
インヒビター制御技術が探索されている。いずれにして
も高い磁束密度(+ 1101  < 001>方位の
高集積度)を得るためには析出物を漱わHで均一かつ多
量に仕上高温焼鈍前の綱板中に存在させる事が必要であ
り、析出物の制御と同時にその析出物の特性に合致すべ
く圧延、熱処理の適切な組合せにより二次再結晶前の性
状を調整する事が重要である。
Although Sn, Sb, etc. have been mentioned, there are no examples of these elements being used alone in industrial production, and all of them are used in coexistence with precipitates to achieve a supplementary effect. As more characteristic inhibitors, II, gre
US Pat. No. 3,905,842 (1975) by Noble, US Pat. That is, the presence of appropriate amounts of solid solution S, B, and N makes it possible to manufacture a unidirectional silicon steel plate with a high magnetic flux density. The selection criteria for precipitates that are effective for secondary recrystallization are not necessarily clear, but a representative opinion is that they are based on the results of calibration, "Tetsu to Hagane J 53 (1967) p. 1007-1.
023. To summarize, (1) the size is about 0.1 p (2) the required volume is 0.1 vol 1% or more (3) it is not possible to completely melt or not melt at all in the secondary recrystallization temperature range, so it is appropriate It is a solid solution to a certain extent. Although some of the above-mentioned various precipitates meet these conditions, not all phenomena meet these conditions. It has been found that (1) above does not have any important meaning in the method of nitriding steel sheets after recent cold rolling. As described above, currently no guiding principles have been established for selecting precipitates, and new inhibitor control techniques are being searched for through trial and error. In any case, in order to obtain a high magnetic flux density (high degree of accumulation in +1101<001> orientation), it is necessary to rinse the precipitates, finish them uniformly and in large quantities with H, and make them exist in the steel sheet before high-temperature annealing. Therefore, it is important to control the precipitates and at the same time adjust the properties before secondary recrystallization by an appropriate combination of rolling and heat treatment to match the characteristics of the precipitates.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

現在、工業生産されている代表的な一方向性珪素綱板製
造方法として3種類あるが、各々については長所・短所
がある。第一の技術はM、F Littmannによる
特公昭30−3651号公報に示されたMnSを用いた
二回冷延工程であり、得られる二次再結晶粒は安定して
発達するが、高い磁束密度が得られない。第二の技術は
川口等による特公昭40−15644号公報に示された
AAN +MnSを用いた最終冷延を80%以上の強圧
下率とするプロセスであり、高い磁束密度は得られるが
、工業生産に際してその製造条件の適切範囲が狭く最高
磁性の製品の安定生産に欠ける。第三の技術は今生等に
よる特公昭51−13469号公?[こ示されたMnS
 (および/またはMnSe> +Sbを含有する珪素
鋼を二回冷延工程によって製造するプロセスであり、比
較的に高い磁束密度は得られるが、Sb、Seのような
有害でかつ高価な元素を使用し、しかも二回冷延法であ
ることから製造コストが高(なる。上記3種類の技術に
おいては共通して次のような問題がある。
Currently, there are three typical methods for manufacturing unidirectional silicon steel sheets that are industrially produced, and each method has its advantages and disadvantages. The first technique is a two-time cold rolling process using MnS, which was disclosed in Japanese Patent Publication No. 30-3651 by M.F. Littmann, and the resulting secondary recrystallized grains develop stably, but the magnetic flux is high. Density cannot be obtained. The second technology is a process in which the final cold rolling using AAN + MnS has a strong reduction rate of 80% or more, which was disclosed in Japanese Patent Publication No. 40-15644 by Kawaguchi et al. During production, the appropriate range of manufacturing conditions is narrow and stable production of products with the highest magnetic properties is lacking. Is the third technique published by Imao et al. in Special Publication No. 13469/1983? [The MnS shown here
(and/or MnSe> This is a process of manufacturing silicon steel containing Sb through a double cold rolling process, and although a relatively high magnetic flux density can be obtained, harmful and expensive elements such as Sb and Se are used. However, since it is a double cold rolling method, the manufacturing cost is high.The above three types of techniques have the following problems in common.

すなわち、上記技術はいずれもが析出物を微細、均一に
制御する技術として熱延に先立つスラブ加熱温度を第一
の技術では1260℃以上、第二の技術では特開昭48
−51852号公報に示すように素材Si量によるが3
%Siの場合で1350℃、第三の技術では特開昭51
−20716号公報に示されるように1230℃以上、
高い磁束密度の得られた実施例では1320°Cといっ
た極めて高い温度にすることによって粗大に存在する析
出物を一旦固溶させ、その後の熱延中、あるいは熱処理
中に析出させている。スラブ加熱温度を上げることはス
ラブ加熱時の使用エネルギーの増大、ノロの発生による
歩留り低下および加熱炉補修費の増大ならびに加熱炉補
修頻度の増大に起因する設備稼!’t)+率の低下、さ
らには特公昭57−41526号公報に示されるように
線状二次再結晶不良が発生ずるために連続鋳造スラブが
使用出来ないという問題がある。しかしこのようなコス
ト上の問題以上に重要なことは、鉄損向上のためにSi
を多く、成品板厚を薄く、といった手段を採るとこの線
状二次再結晶不良の発生が増大し、高温スラブ加熱法を
前提にした技術では将来の鉄(4向上に希望を持てない
。これ番こ対し特公昭61−60896号公報に開示さ
れている技術では鋼中のSを少なくすることによって二
次再結晶が極めて安定し、高Si薄手成品を可能にした
。しかしこの技術は量産規模で工場生産する上で磁束密
度の安定性に問題があり、例えば特開昭62−4031
5号公報に開示されているような改良技術が提案されて
いるが今まで完全に解決するに至っていない。
That is, all of the above-mentioned technologies are technologies for controlling precipitates finely and uniformly, with the first technology increasing the heating temperature of the slab prior to hot rolling to 1260°C or higher, and the second technology increasing the heating temperature of the slab to 1260°C or higher, while the second technology
As shown in Publication No. 51852, it depends on the amount of Si in the material.
1350°C in the case of %Si, and 1350°C in the case of the third technology
-1230℃ or higher as shown in Publication No. 20716,
In the examples in which a high magnetic flux density was obtained, the temperature was raised to an extremely high temperature of 1320° C., so that the coarsely existing precipitates were once solid-dissolved, and then precipitated during the subsequent hot rolling or heat treatment. Increasing the slab heating temperature increases the energy used when heating the slab, reduces yield due to the generation of slag, increases heating furnace repair costs, and increases the frequency of heating furnace repairs. 't) There is a problem that continuous casting slabs cannot be used because of a decrease in the + ratio and, as shown in Japanese Patent Publication No. 57-41526, linear secondary recrystallization defects occur. However, more important than these cost issues is the use of Si to improve iron loss.
If measures are taken to increase the thickness of the finished product and reduce the thickness of the finished product, the occurrence of linear secondary recrystallization defects will increase, and with technology based on high-temperature slab heating, there is no hope for future improvements in steel (4). On the other hand, the technology disclosed in Japanese Patent Publication No. 61-60896 made secondary recrystallization extremely stable by reducing the amount of S in the steel, making it possible to produce thin, high-Si products.However, this technology was not suitable for mass production. There is a problem with the stability of magnetic flux density when manufacturing on a large scale, for example, in JP-A-62-4031.
Although improved techniques as disclosed in Japanese Patent No. 5 have been proposed, the problem has not been completely solved until now.

以上の技術とは別にIl、grenobleによる米国
特許第3.905.842号、H,Fiedlerによ
る米国特許第3.905.843号があるが、この技術
は本質的に矛盾があり工業生産されていない。すなわち
、この技術ではインヒビターとして固溶Sが中心である
ため、固溶S確保のためにMnを下げて、MnSを形成
させない事が必須である。具体的にはMn/Sり2.1
が必要である。ところで固溶SおよびSeは材料の靭性
に極めて悪影響を持つことは広く知られている。したが
ってSi量が多く割れ易い一方向性珪素綱板ではこのよ
うな固溶S或いはSeのある状態で冷間圧延することは
、工業生産では極めて困難である。以上に詳述したよう
に、コストを低く、特性的には高い磁束密度でしかも将
来の低鉄損の可能性の大きい高31%薄手成品も満足さ
せるためにはインヒビター設計を再構築する必要がある
Apart from the above-mentioned technology, there are U.S. Patent No. 3.905.842 by Il. Grenoble and U.S. Patent No. 3.905.843 by H. Fiedler, but these technologies are inherently contradictory and have not been industrially produced. do not have. That is, since this technology mainly uses solid solution S as an inhibitor, it is essential to lower Mn and prevent the formation of MnS in order to ensure solid solution S. Specifically, Mn/S ratio 2.1
is necessary. By the way, it is widely known that solid solution S and Se have an extremely adverse effect on the toughness of materials. Therefore, in industrial production, it is extremely difficult to cold-roll a unidirectional silicon steel sheet that has a large amount of Si and is easily cracked in the presence of solid solution S or Se. As detailed above, it is necessary to rebuild the inhibitor design in order to satisfy the needs of 31% thin products that have low costs, high magnetic flux density characteristics, and a high possibility of low iron loss in the future. be.

〔課題を解決するための手段〕[Means to solve the problem]

本発明者等は溶鋼中のS又はSe又はその複合量を一定
量以下に少なくし、しかも固溶S又はS’eを少なくす
る条件下で適当量のA1とN、及びBとTiを複合して
含有させた素材を通常の1回又は2回の冷延工程で最終
板厚とし、脱炭焼鈍、焼鈍分離剤塗布、仕上焼鈍を行な
うプロセスを採るとともに最終冷延から仕上焼鈍での二
次再結晶開始までの昇温段階の間に窒化処理を行うこと
により、極めて磁束密度の高い一方向性珪素綱板を製造
することに成功した。
The present inventors combined appropriate amounts of A1 and N, and B and Ti under the conditions of reducing the amount of S or Se or their combination in molten steel below a certain amount and also reducing the amount of solid solution S or S'e. The final plate thickness is obtained by one or two normal cold rolling processes, and the process includes decarburization annealing, application of an annealing separator, and final annealing. By performing nitriding during the temperature rising stage before the start of the next recrystallization, we succeeded in manufacturing a unidirectional silicon steel plate with extremely high magnetic flux density.

この結果、磁区制御技術との組合せにより、従来にもま
して鉄損値の低い材料を得ることが可能となった。
As a result, in combination with magnetic domain control technology, it has become possible to obtain a material with a lower iron loss value than ever before.

本発明を特徴づける構成条件について説明する。The structural conditions that characterize the present invention will be explained.

S又はSe量が多(なると成品長手方向に線状二次再結
晶不良が増加し安定生産が出来ない。この傾向は特にS
tが3.2%(以下%は全で重量%である)を超えた高
Si範囲で、又0.23mm (9mil成品)以下の
薄手成品で顕著になる。この様な線状二次再結晶不良が
全く発生しないS十Seの含有量の上限値として0.0
12%を限定した。この限定範囲の中でも本発明では従
来有効であるとされていたS又はSe量が多くなるとむ
しろ磁束密度は劣化し、少ないもの程良好な磁束密度と
なるが、現状の溶製技術ではコストを高くせずに下げ得
る範囲として0.0005%以上が一般的である。次に
本発明ではコストを下げるため熱延および冷延時の圧延
割れを皆無にすることを狙っており、固溶S又はSeに
よる割れを防ぐためMn /S+Se≧4とすることに
より鋼中に存在する微ff1s、seを出来るだけMn
S 、 MnSeとして固着することにしである。
If the amount of S or Se is large, linear secondary recrystallization defects will increase in the longitudinal direction of the product, making stable production impossible.
It becomes noticeable in a high Si range where t exceeds 3.2% (hereinafter, all percentages are by weight), and in thin products of 0.23 mm (9 mil products) or less. The upper limit of the S+Se content at which such linear secondary recrystallization defects do not occur is 0.0.
Limited to 12%. Even within this limited range, in the present invention, if the amount of S or Se, which was conventionally considered to be effective, increases, the magnetic flux density actually deteriorates, and the smaller the amount, the better the magnetic flux density becomes.However, with the current melting technology, the cost increases. The range that can be lowered without causing damage is generally 0.0005% or more. Next, in order to reduce costs, the present invention aims to completely eliminate rolling cracks during hot rolling and cold rolling, and in order to prevent cracking due to solid solution S or Se, Mn /S + Se ≧ 4 is set so that Mn/S+Se≧4 exists in the steel. Fine ff1s, se as much as possible
It was decided to fix it as S, MnSe.

第1図はC: 0.053%、Si:3.35%、P:
0.030%、Ae : 0.030%、N : 0.
0075%、B:0.0039%、Ti  : 0.0
038%を含有し、更にMn0.04%と0.12%を
含んだ溶鋼にs3Bを変えた50kgインゴットを13
60°Cと1150℃に加熱した後、熱間圧延した後の
熱延板端部の割れを示したものである。Mn/S≧4で
急激に割れが減少し、特にMnSを固溶させない115
0°Cの低温スラブ加熱材ではほとんど割れは発生しな
い。
Figure 1 shows C: 0.053%, Si: 3.35%, P:
0.030%, Ae: 0.030%, N: 0.
0075%, B: 0.0039%, Ti: 0.0
13. A 50 kg ingot containing Mn 0.038% and s3B changed to molten steel containing Mn 0.04% and 0.12%.
This figure shows cracks at the end of a hot rolled sheet after hot rolling after heating to 60°C and 1150°C. Cracking decreases rapidly when Mn/S≧4, especially when MnS is not dissolved as a solid solution 115
Cracks hardly occur when heating slabs at a low temperature of 0°C.

なお、第2図(aHb)は第1図の端部における金属組
織を表わす写真であり、同図(a)は第1図において、
Mn/S=2におけるスラブ加熱温度1350℃の場合
の状態を示し、同図(b)はMn/5=14の場合の状
態(スラブ加熱温度1350℃の場合(1150°Cの
場合も殆んど同様))を示す。
In addition, FIG. 2 (aHb) is a photograph showing the metal structure at the edge of FIG. 1, and FIG.
The figure shows the state when the slab heating temperature is 1350°C at Mn/S=2, and (b) shows the state when the slab heating temperature is 1350°C (1150°C as well). (similar to)).

次にBの効果について説明する。Next, the effect of B will be explained.

C: 0.053%、Si:3.25%、Mn:0.1
4%、S : 0.007%、Ti  : 0.003
0%、P : 0.023%、Al : 0.028%
、N : 0.0085%にBを0.0002〜0.0
095%を含有する50kgインゴットを1150°C
に加熱後2.0鰭の熱延板とした。1120°(Hx3
minの熱延板焼鈍後0.20龍に冷延し、810℃、
830℃。
C: 0.053%, Si: 3.25%, Mn: 0.1
4%, S: 0.007%, Ti: 0.003
0%, P: 0.023%, Al: 0.028%
, N: 0.0085% and B 0.0002 to 0.0
50kg ingot containing 095% was heated to 1150°C.
After heating, it was made into a 2.0 fin hot-rolled plate. 1120° (Hx3
After hot-rolled plate annealing for 0.20 min, cold-rolled to 810°C,
830℃.

850℃、870℃1890℃、  910’cで脱炭
焼鈍し、窒化フェロマンガンを含有するMgOを塗布後
に1200℃の二次再結晶焼鈍を行なった。この結果を
第3図に示す。図から脱炭焼鈍温度を上げると磁束密度
B8は上るが、Bの少ないものは細粒が発生し易く、か
つBaの最高値が小さいことが分る。
Decarburization annealing was performed at 850°C, 870°C, 1890°C, and 910'c, and after coating MgO containing ferromanganese nitride, secondary recrystallization annealing was performed at 1200°C. The results are shown in FIG. It can be seen from the figure that when the decarburization annealing temperature is increased, the magnetic flux density B8 increases, but when the B content is low, fine grains are likely to be generated and the maximum value of Ba is small.

一方多すぎても高B8が得られず、適性範囲は0.00
05〜0.0080%である。
On the other hand, if there is too much, high B8 cannot be obtained, and the appropriate range is 0.00.
05 to 0.0080%.

第4図はBとTiを複合添加した場合の結果を示したも
のである。
FIG. 4 shows the results when B and Ti were added in combination.

C: 0.048%、Si:3.30%、Mn  : 
0.100%、S : 0.008%、P : 0.0
25%、Aβ: 0.032%、N : 0.0075
〜0.0092%を基本成分としこれにTiを0.00
10〜0.0180%、Bを0.0002〜0.009
0%の範囲で複合添加した50kgインゴットを115
0°Cに加熱後2.0龍の熱延板を遣った。これを11
20°c×3m1nの熱延板焼鈍をした後0.20mm
に冷延し、850°Cで脱炭焼鈍をし、窒化フェロマン
ガンを含有するMgOを塗布後に1200℃の二次再結
晶焼鈍を行なった。
C: 0.048%, Si: 3.30%, Mn:
0.100%, S: 0.008%, P: 0.0
25%, Aβ: 0.032%, N: 0.0075
The basic component is ~0.0092%, and 0.00% Ti is added to this as a basic component.
10-0.0180%, B 0.0002-0.009
115 50 kg ingot with compound addition in the range of 0%
After heating to 0°C, a hot-rolled plate of 2.0 mm was used. This is 11
0.20mm after annealing a hot rolled plate of 20°c x 3m1n
The material was cold-rolled, decarburized annealed at 850°C, coated with MgO containing ferromanganese nitride, and then subjected to secondary recrystallization annealing at 1200°C.

第4図によれば、B (II) :  1.93T以上
の高磁束密度のものがTi O,0020〜0.012
0%、B O,0011)5〜0.0080%の範囲で
複合添加した場合に得られることが明らかになった。
According to FIG. 4, B (II): those with a high magnetic flux density of 1.93T or more are TiO,0020~0.012
It has become clear that this can be obtained when the compound is added in a range of 5% to 0.0080% (BO,0011).

このBとTiの効果は冷間圧延以降に綱板が窒化される
場合に意味があり恐らく微細なりN或はTiNが効果を
持つと考えられる。N : 0.0010%未満では二
次再結晶粒の発達が悪くなる。0.0120%を超える
とブリスターと呼ばれる綱板のふくれが発生する。
This effect of B and Ti is significant when the steel plate is nitrided after cold rolling, and it is thought that fine N or TiN probably has an effect. N: If it is less than 0.0010%, secondary recrystallized grains will not develop well. If it exceeds 0.0120%, swelling of the rope plate called blister will occur.

次にA1はNと結合してAINとなるが、本発明では後
工程で窒化によりAlを含む化合物を形成させることを
必須としているためそのフリーの/lが一定量以上必要
である。そのためには、Alの適正範囲は0.012〜
0.050%必要である。
Next, A1 combines with N to form AIN, but in the present invention, it is essential to form a compound containing Al by nitriding in a subsequent step, so a certain amount or more of free /l is required. For this purpose, the appropriate range of Al is 0.012~
0.050% is required.

なお、以上の成分の他に、Cは0.025〜0.075
%の範囲が好ましい。
In addition to the above components, C is 0.025 to 0.075
A range of % is preferred.

C含有量が0.025%未満では、二次再結晶が不安定
になりかつ、二次再結晶した場合でも製品の磁束密度が
低い。一方、C含有量が0.075%を超えると、脱炭
焼鈍時間が長くなり、生産性を阻害する。
If the C content is less than 0.025%, secondary recrystallization becomes unstable, and even when secondary recrystallization occurs, the magnetic flux density of the product is low. On the other hand, if the C content exceeds 0.075%, the decarburization annealing time becomes longer, which inhibits productivity.

また、Mnの含有量は、Sの含有量との関係において、
上述した如く、Mn/S≧4.0で熱延板の耳割れを防
止するという観点からは十分であるが、Mn含有量の上
限は0.45%が好ましい。0.45%を超えると、皮
膜欠陥が出る。
In addition, the Mn content has the following relationship with the S content:
As mentioned above, Mn/S≧4.0 is sufficient from the viewpoint of preventing edge cracking of the hot rolled sheet, but the upper limit of the Mn content is preferably 0.45%. If it exceeds 0.45%, film defects will occur.

スラブ加熱温度については、従来のようにインヒビター
を固溶する高温スラブ加熱でも、また殆んど従来では無
理と考えられていた普通銅皿の低温スラブ加熱でも二次
再結晶は行なわれる。しかし第1図に示した様に熱延の
割れが少なく出来る事、又当然の事として熱エネルギー
が少ない低温スラブ加熱が有利である事からノロの発生
しない1200°C以下が望ましい。
Regarding the slab heating temperature, secondary recrystallization can be carried out either by high-temperature slab heating to dissolve the inhibitor as in the past, or by low-temperature slab heating using an ordinary copper plate, which was considered almost impossible in the past. However, as shown in FIG. 1, the temperature is preferably 1200° C. or lower, where no slag occurs, because cracks in the hot rolling can be reduced, and low-temperature slab heating, which requires less thermal energy, is advantageous.

熱延以降の工程においては、最も高いB8を得るために
短時間の焼鈍後80%以上の高圧延率の冷延によって最
終板厚にする方法が望ましい。しかし特性はやや劣るが
低コストとするために熱延板焼鈍を省略してもよい。又
最終成品の結晶粒を小さくするため中間焼鈍を含む工程
でも可能である。
In the steps after hot rolling, in order to obtain the highest B8, it is desirable to perform short-time annealing and then cold rolling at a high rolling reduction of 80% or more to achieve the final thickness. However, the hot-rolled sheet annealing may be omitted in order to reduce the cost, although the properties are slightly inferior. It is also possible to use a process that includes intermediate annealing to reduce the grain size of the final product.

次に湿水素或いは湿水素、窒素混合雰囲気ガス中で脱炭
焼鈍をする。このときの温度は特にこだわらないが80
0℃〜900°Cが好ましい範囲である。
Next, decarburization annealing is performed in wet hydrogen or a mixed atmosphere of wet hydrogen and nitrogen. The temperature at this time is not particularly important, but it is 80
The preferred range is 0°C to 900°C.

なお、このときの雰囲気の露点は+30°C以上が好ま
しい。
Note that the dew point of the atmosphere at this time is preferably +30°C or higher.

次いで焼鈍分離剤を塗布し高IA(通常1100℃〜1
200°C)長時間の仕上げ焼鈍を行なう。本願の窒化
における最も好ましい実施態様は、上記仕上げ焼鈍の昇
温過程において窒化する事であり、これにより二次再結
晶に必要なインヒビターを作り込む事ができる。これを
達成するために焼鈍分離剤中に窒化能のある化合物、例
えばMnN 、 CrN等を適当量添加するか或いはN
H3等の窒化能のある気体を雰囲気ガス中に添加する。
Next, an annealing separator is applied and a high IA (usually 1100℃~1
200°C) long-term final annealing. The most preferred embodiment of nitriding in the present application is to perform nitriding during the temperature raising process of the final annealing, thereby making it possible to create an inhibitor necessary for secondary recrystallization. To achieve this, an appropriate amount of a compound with nitriding ability, such as MnN, CrN, etc., is added to the annealing separator, or N
A gas capable of nitriding, such as H3, is added to the atmospheric gas.

なお、本発明における窒化の他の実施態様として、脱炭
焼鈍時均熱以降で窒化能のある気体の雰囲気で窒化する
か、又は、脱炭焼鈍後別途設けたNH,等の雰囲気を有
する熱処理炉に通過せしめて窒化してもよく、以上の手
段の組合せでもよい。
In addition, as other embodiments of nitriding in the present invention, nitriding is performed in an atmosphere of a gas capable of nitriding after soaking during decarburization annealing, or heat treatment with an atmosphere of NH, etc. separately provided after decarburization annealing. It may be passed through a furnace for nitriding, or a combination of the above methods may be used.

二次再結晶完了後は水素雰囲気中において純化焼鈍を行
なう。
After completion of secondary recrystallization, purification annealing is performed in a hydrogen atmosphere.

〔実施例〕〔Example〕

(1)  C: 0.055%、Si:3.3%、Mn
  : 0.14%、P : 0.030%、S : 
0.007%、Ti  : 0.0040%、Cr:0
.12%、/l : 0.030%、N : 0.00
80%、残部Fe及び不可避的不純物からなる珪素鋼に
Bを下表に記した添加量のスラブを1150°Cで加熱
し2. Oamの熱延板を造った。これを1100”C
x 2分の焼鈍をし、1回の冷延で0.20uとし85
0℃×90秒の脱炭焼鈍を60℃の湿水素窒素混合ガス
中で行なった。次にMgO中にTiO□3%とフェロ窒
化マンガン5重量%を添加した焼鈍分離剤(a)とMg
OとTi0□3%のみの焼鈍分離剤(b)の二種類に塗
り分け、10℃/hrの昇温速度で1200°Cに加熱
し、20時間の焼鈍をした。
(1) C: 0.055%, Si: 3.3%, Mn
: 0.14%, P: 0.030%, S:
0.007%, Ti: 0.0040%, Cr: 0
.. 12%, /l: 0.030%, N: 0.00
2. A slab of silicon steel consisting of 80% Fe and unavoidable impurities, with B added in the amount shown in the table below, was heated at 1150°C.2. We made Oam hot-rolled sheets. This is 1100”C
x 2 minutes of annealing and one cold rolling to 0.20u 85
Decarburization annealing was performed at 0°C for 90 seconds in a wet hydrogen-nitrogen mixed gas at 60°C. Next, annealing separator (a) containing 3% TiO□ and 5% by weight of ferromanganese nitride in MgO and Mg
It was coated with two types of annealing separator (b) containing only O and 0□3% Ti, heated to 1200°C at a temperature increase rate of 10°C/hr, and annealed for 20 hours.

この時の雰囲気ガスは1200℃までの昇温過程ではN
225%とH275%の混合ガスを使用し、1200℃
の均熱時はHzlOO%とした。焼鈍分離剤中に窒化源
となるフェロ窒化マンガンを添加したものはいずれも二
次再結晶をし、Bを添加した材料では、いずれも極めて
高い磁束密度が得られた。
At this time, the atmospheric gas is N during the heating process up to 1200℃.
Using a mixed gas of 225% and H275%, 1200℃
During soaking, the temperature was HzlOO%. All materials in which ferromanganese nitride, which serves as a nitriding source, was added to the annealing separator underwent secondary recrystallization, and all materials in which B was added obtained extremely high magnetic flux densities.

一方フエロ窒化マンガンを添加しないものはいずれも二
次再結晶不良となった。結果を下表に示す。
On the other hand, in all cases where ferromanganese nitride was not added, secondary recrystallization was defective. The results are shown in the table below.

(2)  C: 0.048  %、Si:3.25%
、Mn  : 0.12%、P  :  0.025 
 %、Cr:0.14%、Ti  :  0.0030
%、Al  :  0.028  %、N  :  0
.0070%、B  :  0.0030%残部Fe及
び不可避的不純物からなる珪素銅のSの含有量を(a)
 0.003%、(b)0.009%、(c) 0.0
18%に変えたスラブを1200℃で加熱し1.8龍の
熱延板を造った。これを1100°CX2分の焼鈍を行
い、1回の冷延で0.18鰭とし、830°C×90秒
の脱炭焼鈍を55°Cの湿水素窒素混合ガス中で行い、
MgO中に7重量%のフェロ窒化マンガンを添加した焼
鈍分離剤を塗布し、15℃/hrの昇温速度で1200
℃に加熱し、20時間の焼鈍を行なった。この時の雰囲
気ガスは実施例1と同じである。
(2) C: 0.048%, Si: 3.25%
, Mn: 0.12%, P: 0.025
%, Cr: 0.14%, Ti: 0.0030
%, Al: 0.028%, N: 0
.. 0070%, B: S content of silicon copper consisting of 0.0030% balance Fe and unavoidable impurities (a)
0.003%, (b) 0.009%, (c) 0.0
The 18% slab was heated at 1200°C to produce a hot-rolled sheet with a thickness of 1.8%. This was annealed at 1100°C for 2 minutes to obtain a 0.18 fin in one cold rolling, and decarburized at 830°C for 90 seconds in a wet hydrogen-nitrogen mixed gas at 55°C.
An annealing separator containing 7% by weight of ferromanganese nitride added to MgO was applied, and the temperature was heated to 1200°C at a heating rate of 15°C/hr.
℃ and annealed for 20 hours. The atmospheric gas at this time is the same as in Example 1.

結果を次に示す。The results are shown below.

Sの含有量が多いと高磁束密度が得られない。If the S content is high, high magnetic flux density cannot be obtained.

(3) C: 0.045%、Si:3.50%、Mn
:0.16%、P : 0.035%、/10.028
%、N : 0.0080%、Ti  : 0.004
0%、B : 0.0035%、残部Fe及び不可避的
不純物からなる溶鋼にSeを(a ) 0.0050%
、(b) 0.0100%、(c ) 0.0200%
添加したスラブを1150℃で加熱熱延し2. Oam
の熱延板を造った。
(3) C: 0.045%, Si: 3.50%, Mn
: 0.16%, P: 0.035%, /10.028
%, N: 0.0080%, Ti: 0.004
0%, B: 0.0035%, Se added to molten steel consisting of the balance Fe and unavoidable impurities (a) 0.0050%
, (b) 0.0100%, (c) 0.0200%
The added slab was heated and hot-rolled at 1150°C.2. Oam
A hot-rolled sheet was manufactured.

これを1150°CX2分+900°CX2分の熱延板
焼鈍した後急冷却し、酸洗し0.2(haまで冷延した
This hot-rolled sheet was annealed at 1150° C. for 2 minutes + 900° C. for 2 minutes, then rapidly cooled, pickled, and cold rolled to 0.2 (ha).

この後830℃×90秒の脱炭焼鈍をし、MgOに5重
量%のフェロ窒化マンガンを添加した焼鈍分離剤を塗布
し、10°C/hrの昇温速度で1200°Cに加熱し
、20時間の焼鈍を行なった。
After this, decarburization annealing was performed at 830°C for 90 seconds, an annealing separator containing 5% by weight of ferromanganese nitride added to MgO was applied, and the mixture was heated to 1200°C at a temperature increase rate of 10°C/hr. Annealing was performed for 20 hours.

この時の雰囲気ガスは1200℃までの昇温過程ではN
250%と8250%の混合ガスを使用し、1200℃
の均熱時は)(21oo%とした。
At this time, the atmospheric gas is N during the heating process up to 1200℃.
Using a mixed gas of 250% and 8250%, 1200℃
(during soaking) (21oo%).

磁気特性は次の如くであった。The magnetic properties were as follows.

Se含有量が多すぎると高磁束密度が得られない。If the Se content is too high, high magnetic flux density cannot be obtained.

(4)  C: 0.0/15%、Si:3.30%、
Mn  : 0.150%、S : 0.009%、P
:0.030%1.An! : 0.031%、N :
 0.0070%、Ti  : 0.0060%、残部
Fe及び不可避的不純物からなるスラブ(a)とこれに
更にBを0.0035%添加したスラブ(b)を110
0°Cで加熱熱延し2.3鰭の熱延板を造った。
(4) C: 0.0/15%, Si: 3.30%,
Mn: 0.150%, S: 0.009%, P
:0.030%1. An! : 0.031%, N:
Slab (a) consisting of 0.0070%, Ti: 0.0060%, balance Fe and unavoidable impurities, and slab (b) with further addition of 0.0035% B were prepared at 110%.
A hot-rolled plate with 2.3 fins was produced by heating and hot-rolling at 0°C.

これを(1)熱延板焼鈍なし、(2)熱延板焼鈍を90
0℃×5分した後急冷却したもの、(3)1150℃×
2分+900℃×2分熱延板焼鈍後急冷却したものの3
水準を準備した。
(1) No hot rolled sheet annealing, (2) Hot rolled sheet annealing at 90%
0℃×5 minutes and then rapidly cooled, (3) 1150℃×
3 after rapid cooling after hot-rolled plate annealing for 2 minutes + 900℃ x 2 minutes
Prepared the standard.

これを1回冷延で0.30鰭とし、830℃×150秒
の脱炭焼鈍を650℃の湿水素窒素混合ガス中で行い、
hBoにTiO□を添加した焼鈍分離剤を塗布し、15
°C/hrの昇温速度で1200℃に加熱し、20時間
の仕上焼鈍をした。
This was cold rolled once to a 0.30 fin, and decarburized annealed at 830°C for 150 seconds in a wet hydrogen-nitrogen mixed gas at 650°C.
Apply an annealing separator containing TiO□ to hBo, and
It was heated to 1200°C at a temperature increase rate of °C/hr, and final annealing was performed for 20 hours.

この昇温過程の雰囲気ガスには窒素25%、水素75%
の混合ガス中にNt13ガスをloppm添ノ川したも
用を用い、1200℃の均熱時は水素ガスのみに切替え
純化した。
The atmospheric gas during this heating process is 25% nitrogen and 75% hydrogen.
Nt13 gas was added to the mixed gas of 1,200° C. using a loppm Soenokawa gas filter, and during soaking at 1200° C., only hydrogen gas was used for purification.

磁気特性(B、)は次の如くであった。The magnetic properties (B,) were as follows.

Bを添加したものが添加しないものに比べ熱延板焼鈍の
有り無しに関係なく高Bが得られた。
A high B value was obtained with or without hot-rolled sheet annealing in the case where B was added, compared to the case where B was not added.

(5)  C: 0.056%、Si:3.40%、M
n  : 0.130%、S : 0.005%、P 
: 0.030%、AZ : 0.027%、N : 
0.0075%、Ti  : 0.0030%、B :
 0.0042%、残部Fe及び不可避的不純物からな
るスラブを1150℃で加熱熱延し2.5flと1.6
鰭の熱延板を造った。2.5鶴厚の熱延板は酸洗後1.
5 xyhまで冷延し、1.6鶴厚の熱延板と同時に1
120℃×2.5分の焼鈍後急冷処理をした。これを0
.150 +nまで冷延し、830℃×70秒の脱炭焼
鈍をし、MgOにTiO□とMnNを添加した焼鈍分離
剤を塗布し、1200”C20時間の仕上焼鈍を行なっ
た。
(5) C: 0.056%, Si: 3.40%, M
n: 0.130%, S: 0.005%, P
: 0.030%, AZ: 0.027%, N:
0.0075%, Ti: 0.0030%, B:
A slab consisting of 0.0042%, balance Fe and unavoidable impurities was heated and hot rolled at 1150°C to form 2.5 fl and 1.6 fl.
I made a hot-rolled fin plate. 2.5 mm thick hot-rolled sheet is 1. after pickling.
Cold-rolled to 5 xyh, 1
After annealing at 120° C. for 2.5 minutes, a rapid cooling treatment was performed. Set this to 0
.. It was cold rolled to 150 +n, decarburized annealed at 830°C for 70 seconds, coated with an annealing separator containing MgO with TiO□ and MnN, and final annealed at 1200"C for 20 hours.

この昇温過程の雰囲気ガスには窒素25%、水素75%
の混合ガスを用い、1200℃の均熱時は水素ガスのみ
に切換え純化した。磁気特性は次の如くであった。
The atmospheric gas during this heating process is 25% nitrogen and 75% hydrogen.
A mixed gas was used, and during soaking at 1200° C., only hydrogen gas was used for purification. The magnetic properties were as follows.

〔発明の効果〕〔Effect of the invention〕

本発明は上述した如く、普通銅皿の低温スラブ加熱で圧
延割れの少ない、しかも極めて高い磁束温度を得ること
ができるので、その工業的価値ζ工極めて高い。
As described above, the present invention is capable of obtaining an extremely high magnetic flux temperature with few rolling cracks by heating a plain copper pan at a low temperature, so its industrial value is extremely high.

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

第1図はMn/Sと熱延板端部割れ深さとの関係を示す
図、第2図(aHb)は第1図の熱延板端部の金属組織
を示す写真、第3図はBと脱炭焼鈍温度との関係を示す
図、第4図はTi、Bの複合添加した場合の磁束密度の
状態を示す図である。
Figure 1 is a diagram showing the relationship between Mn/S and the crack depth at the end of the hot rolled sheet, Figure 2 (aHb) is a photograph showing the metallographic structure of the end of the hot rolled sheet in Figure 1, and Figure 3 is B FIG. 4 is a diagram showing the relationship between the temperature and the decarburization annealing temperature, and FIG. 4 is a diagram showing the state of magnetic flux density when Ti and B are added in combination.

Claims (1)

【特許請求の範囲】[Claims] (1)重量%で、Si:1.5〜4.8% Al:0.012〜0.050% Ti:0.0020〜0.0120% N:0.0010〜0.0120% B:0.0005〜0.0080% S又はSeの1種又は2種を合 計で0.012%以下、 Mn/(S+Se):(重量比) ≧4.0、 残部Fe及び不可避的不純物 から成る珪素鋼熱延板を1回、又は2回以上の冷延工程
により最終板厚とし、次いで湿水素中で脱炭焼鈍し、焼
鈍分離剤を塗布し、二次再結晶と純化とを目的とした仕
上焼鈍を行うとともに最終冷延後から仕上焼鈍の二次再
結晶開始までの昇温段階の間に窒化処理を行うことを特
徴とする磁束密度の高い一方向性珪素綱板の製造方法。
(1) In weight%, Si: 1.5-4.8% Al: 0.012-0.050% Ti: 0.0020-0.0120% N: 0.0010-0.0120% B: 0 .0005 to 0.0080% A silicon steel containing one or two types of S or Se in a total of 0.012% or less, Mn/(S+Se): (weight ratio) ≧4.0, the balance being Fe and inevitable impurities. A hot rolled sheet is subjected to one or more cold rolling processes to achieve the final thickness, then decarburized annealed in wet hydrogen, coated with an annealing separator, and finished for the purpose of secondary recrystallization and purification. A method for producing a unidirectional silicon steel sheet having a high magnetic flux density, characterized in that annealing is performed and a nitriding treatment is performed during a temperature rising stage from the final cold rolling to the start of secondary recrystallization in finish annealing.
JP63109880A 1987-11-20 1988-05-07 Method for manufacturing unidirectional silicon steel sheet with high magnetic flux density Expired - Lifetime JPH0686630B2 (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP63109880A JPH0686630B2 (en) 1987-11-20 1988-05-07 Method for manufacturing unidirectional silicon steel sheet with high magnetic flux density
DE88118993T DE3882502T2 (en) 1987-11-20 1988-11-14 Process for the production of grain-oriented electrical steel sheets with high flux density.
EP88118993A EP0321695B1 (en) 1987-11-20 1988-11-14 Process for production of grain oriented electrical steel sheet having high flux density
US07/274,432 US4994120A (en) 1987-11-20 1988-11-18 Process for production of grain oriented electrical steel sheet having high flux density
KR1019880015250A KR930001330B1 (en) 1987-11-20 1988-11-19 Process for production of grain oriented electrical steel sheet having high flux density

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP62-291975 1987-11-20
JP29197587 1987-11-20
JP63109880A JPH0686630B2 (en) 1987-11-20 1988-05-07 Method for manufacturing unidirectional silicon steel sheet with high magnetic flux density

Publications (2)

Publication Number Publication Date
JPH01230721A true JPH01230721A (en) 1989-09-14
JPH0686630B2 JPH0686630B2 (en) 1994-11-02

Family

ID=26449587

Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JPH0686630B2 (en)

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