JPH0733546B2 - High magnetic flux density bi-directional electrical steel sheet manufacturing method - Google Patents

High magnetic flux density bi-directional electrical steel sheet manufacturing method

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Publication number
JPH0733546B2
JPH0733546B2 JP2097718A JP9771890A JPH0733546B2 JP H0733546 B2 JPH0733546 B2 JP H0733546B2 JP 2097718 A JP2097718 A JP 2097718A JP 9771890 A JP9771890 A JP 9771890A JP H0733546 B2 JPH0733546 B2 JP H0733546B2
Authority
JP
Japan
Prior art keywords
steel sheet
annealing
magnetic flux
electrical steel
flux density
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.)
Expired - Fee Related
Application number
JP2097718A
Other languages
Japanese (ja)
Other versions
JPH04322A (en
Inventor
義行 牛神
聡 新井
洋三 菅
延幸 高橋
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 JP2097718A priority Critical patent/JPH0733546B2/en
Priority to KR1019910005878A priority patent/KR930010323B1/en
Priority to DE69129130T priority patent/DE69129130T2/en
Priority to EP91303278A priority patent/EP0452153B1/en
Publication of JPH04322A publication Critical patent/JPH04322A/en
Priority to US08/034,615 priority patent/US5346559A/en
Publication of JPH0733546B2 publication Critical patent/JPH0733546B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Soft Magnetic Materials (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、鋼板長手方向ならびに長手方向に直角な方向
に磁化容易軸<001>方位を有するとともに、圧延面に
{100}面が現れている(ミラー指数で{100}<001>
と表示される)結晶粒から構成される所謂二方向性電磁
鋼板の製造方法に関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention has an easy axis <001> orientation in the longitudinal direction of a steel sheet and a direction perpendicular to the longitudinal direction, and a {100} plane appears on the rolling surface. Yes (Mirror index {100} <001>
(Indicated by the following), a so-called bi-directional electrical steel sheet composed of crystal grains.

二方向性電磁鋼板は、圧延方向ならびに圧延方向と直角
な方向に磁化容易軸(<001>軸)を有し、二方向で磁
気特性が優れているので、圧延方向にのみ磁気特性が優
れている一方向性電磁鋼板に比べて二方向に磁束を流す
必要のある機器、例えば大型回転器用の磁芯材料として
用いると有利である。また、小型静止器の分野では一般
的に磁化容易軸を高度に集積させない無方向性電磁鋼板
が用いられているが、二方向性電磁鋼板を用いることに
より、小型化・高効率化への可能性がある。
Bi-directional electrical steel sheet has an easy axis of magnetization (<001> axis) in the rolling direction and in the direction perpendicular to the rolling direction, and has excellent magnetic properties in the two directions, so magnetic properties are excellent only in the rolling direction. It is advantageous to use it as a magnetic core material for equipment that needs to flow magnetic flux in two directions as compared with existing unidirectional electrical steel sheet, for example, a large rotating machine. Also, in the field of small static devices, non-oriented electrical steel sheets that do not highly integrate the easy axis of magnetization are generally used, but by using bi-directional electrical steel sheets, downsizing and higher efficiency can be achieved. There is a nature.

〔従来の技術〕 上記の如く、二方向性電磁鋼板は優れた特性を有してい
るところから、その製品化が待望されてきたにもかかわ
らず、今日まで工業製品として一般に使用されるに至っ
ていない。
[Prior Art] As described above, since the grain-oriented electrical steel sheet has excellent properties, it has been widely used as an industrial product until now, despite the long-awaited commercialization thereof. Not in.

従来の二方向性電磁鋼板の製造技術としては、主に次の
二つの方法がある。
There are mainly the following two methods as a conventional manufacturing technique for a grain-oriented electrical steel sheet.

その一つは、特公昭37−7110号公報に開示されているよ
うに極性ガス、たとえば硫化水素を含む雰囲気中で高温
焼鈍を行い、表面エネルギーを利用して{100}<001>
方位粒を二次再結晶させる方法である。しかしながら、
この方法は鋼板の表面エネルギーを厳密に制御する必要
があり、大量生産プロセスとしては不適である。
One of them is high temperature annealing in an atmosphere containing a polar gas such as hydrogen sulfide as disclosed in JP-B-37-7110, and {100} <001> using surface energy.
This is a method of secondarily recrystallizing oriented grains. However,
This method requires strict control of the surface energy of the steel sheet and is not suitable as a mass production process.

他の一つは、特公昭35−2657号公報に開示されているよ
うに、一方向に冷間圧延を行った後、上記冷間圧延と交
叉する方向に冷間圧延を施す、いわゆる「交叉冷間圧延
法」である。しかしながら、この方法で得られる製品の
磁束密度(B8)は1.85Tesla以下であり、その製造工程
の煩雑さに起因するコスト高に見合うだけの優れた磁気
特性を有しないため、従来の一方向性電磁鋼板に対抗で
きない。
The other is, as disclosed in Japanese Patent Publication No. 35-2657, a so-called "crossover" in which cold rolling is performed in one direction and then cold rolling is performed in a direction intersecting with the cold rolling. Cold rolling method ". However, the magnetic flux density (B 8 ) of the product obtained by this method is 1.85 Tesla or less, and it does not have the excellent magnetic characteristics commensurate with the high cost due to the complexity of the manufacturing process, so it is one-way Can't compete with electrical magnetic steel sheet.

一方向性電磁鋼板の磁束密度(B8)は、特公昭40−1564
4号公報、特公昭51−13469号公報に開示された技術が発
明されて以来、急速に進歩し、現在、磁束密度(B8)が
1.92Tの高い磁束密度の製品も市販されている。
The magnetic flux density (B 8 ) of unidirectional electrical steel sheet is as follows.
Since the technology disclosed in Japanese Patent Publication No. 4 and Japanese Patent Publication No. 51-13469 was invented, it has made rapid progress, and the magnetic flux density (B 8 ) is currently increasing.
Products with a high magnetic flux density of 1.92T are also commercially available.

二方向性電磁鋼板についても、磁気特性向上のため特公
昭35−17208号公報、及び特公昭38−8213号公報に改良
技術が提案されたが、いずれも一方向性電磁鋼板等に対
抗できる高磁束密度の製品を安定して製造するに至って
いない。
Regarding bi-directional electrical steel sheets, improved technology was proposed in Japanese Patent Publication No. 35-17208 and Japanese Patent Publication No. 38-8213 in order to improve magnetic properties. Products with magnetic flux density have not been manufactured stably.

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

本発明は、二方向性電磁鋼板において高磁束密度の製品
を安定して得ることができないという製造技術上の課題
を解決するものである。
The present invention solves the problem in the manufacturing technology that a product having a high magnetic flux density cannot be stably obtained in a grain-oriented electrical steel sheet.

〔課題を解決するための手段〕[Means for Solving the Problems]

本発明は上記課題を解決するために、重量%で、Si;0.8
〜6.7%、酸可溶性Al;0.008〜0.048%、N≦0.010%、
残部Feおよび不可避的不純物からなる熱延板を、圧下率
40〜80%で冷間圧延し、更に前記冷間圧延と交叉する方
向に圧下率30〜70%で冷間圧延し、次いで一次再結晶焼
鈍後、焼鈍分離剤を塗布し、二次再結晶と純化を目的と
した仕上焼鈍を行う二方向性電磁鋼板の製造法におい
て、 熱延板表層部を厚さ方向両面よりそれぞれ全厚の1/10以
上除去することを特徴とする二方向性電磁鋼板の製造方
法を提供するものである。
In order to solve the above problems, the present invention provides Si; 0.8% by weight.
~ 6.7%, acid-soluble Al; 0.008-0.048%, N≤0.010%,
A hot rolled sheet consisting of the balance Fe and unavoidable impurities
Cold rolling at 40 to 80%, further cold rolling at a reduction rate of 30 to 70% in a direction intersecting with the cold rolling, then after primary recrystallization annealing, an annealing separator is applied, and secondary recrystallization is performed. In the manufacturing method of bi-directional electrical steel sheet that is subjected to finish annealing for the purpose of refining and refining, the bi-directional electromagnetic sheet is characterized by removing the hot-rolled sheet surface layer from both sides in the thickness direction by 1/10 A method for manufacturing a steel sheet is provided.

〔作 用〕[Work]

本発明者等は、交叉冷間圧延法によって製造した二方向
性電磁鋼板の製品の調査から、次の新たな知見を得た。
The present inventors have obtained the following new findings from a survey of products of the grain-oriented electrical steel sheet produced by the cross cold rolling method.

二方向性電磁鋼板の特徴とする結晶方位は{100}<001
>方位であるが、二次再結晶粒の中には、この方位粒と
あわせて{110}<uuw>方位のものが混在し、後者の方
位粒が磁束密度を低くする原因となっている。従って、
高磁束密度化を達成するためには、{110}<uuw>方位
粒の二次再結晶を抑制すれば良い。
The characteristic crystal orientation of the grain-oriented electrical steel sheet is {100} <001
> Orientation, but in the secondary recrystallized grains, the orientation grains and {110} <uuw> orientation are mixed, and the latter orientation grains cause the magnetic flux density to decrease. . Therefore,
In order to achieve a high magnetic flux density, secondary recrystallization of {110} <uuw> oriented grains may be suppressed.

本発明者等は、これらの方位粒に関する詳細な研究の結
果二次再結晶前の一次再結晶板は板厚方向に集合組織が
異なっており、{110}<uuw>方位粒は表面層から、
{100}<001>方位粒は中心層から発達することを見出
した。
As a result of detailed studies on these oriented grains, the present inventors have found that the primary recrystallized plate before secondary recrystallization has different textures in the thickness direction, and {110} <uuw> oriented grains are different from the surface layer. ,
It has been found that {100} <001> oriented grains develop from the central layer.

かかる事実は、次の実験によって得られたものである。This fact is obtained by the following experiment.

C;0.055%、Si;3.3%、酸可溶性Al;0.028%、N;0.007
%、残部Feおよび不可避的不純物からなる1.8mm厚の熱
延板を1125℃で2分間焼鈍し、熱延方向と同一方向に55
%の圧下率で冷延し、次いで前記圧延方向と直角方向に
55%の圧下率で交叉冷延し、0.35mmの最終板厚とした。
この冷延板に湿水素中810℃で210秒間脱炭を兼ねる一次
再結晶焼鈍を行った。この一次再結晶板の集合組織を調
査したところ、第1図に示すように表面部では{111}
<uvw>方位を主方位とし、中心部では{211}<124
>,{211}<231>方位を主方位とするものであり、板
厚方向で異なるものであることが判明した。二次再結晶
方位は、例えばK.T.Aust,J.W.Rutter;Trans.Met.Soc.AI
ME215(1959年)P119/127、牛神他 日本金属学会第96
回講演大会概要集P373に述べられているように、一次再
結晶集合組織の影響を強く受けるものである。この一次
再結晶集合組織が板厚方向に異なった組織を有する原因
を検討した結果、第2図に示すように熱延板における板
厚方向の集合組織の勾配に大きく影響されるものである
ことが分った。そこで、上記熱延板より表面部、中心部
をそれぞれ切り出し、上記と同様の条件で一次再結晶さ
せた後、MgOを主成分とする焼鈍分離剤を塗布し、仕上
焼鈍を行った。
C; 0.055%, Si; 3.3%, acid soluble Al; 0.028%, N; 0.007
%, The balance Fe and unavoidable impurities, and annealed a 1.8 mm thick hot-rolled sheet at 1125 ° C. for 2 minutes.
Cold rolling at a rolling reduction of
Cross cold rolling was performed at a rolling reduction of 55% to obtain a final plate thickness of 0.35 mm.
The cold-rolled sheet was subjected to primary recrystallization annealing in wet hydrogen at 810 ° C for 210 seconds which also serves as decarburization. When the texture of this primary recrystallized sheet was investigated, {111} was observed on the surface as shown in Fig. 1.
<Uvw> direction is the main direction and {211} <124 at the center
>, {211} <231> orientation is the main orientation, and it has been found that they are different in the plate thickness direction. The secondary recrystallization orientation is, for example, KTAust, JWRutter; Trans.Met.Soc.AI.
ME215 (1959) P119 / 127, Ushigami et al. Japan Institute of Metals 96th
As described in P373 of the Annual Meeting, it is strongly influenced by the primary recrystallization texture. As a result of investigating the cause of this primary recrystallization texture having different textures in the sheet thickness direction, it was found that it is greatly influenced by the texture gradient in the sheet thickness direction in the hot rolled sheet as shown in FIG. I understood. Therefore, the surface portion and the central portion were cut out from the hot-rolled sheet, respectively, and after primary recrystallization under the same conditions as above, an annealing separator containing MgO as a main component was applied and finish annealing was performed.

第3図に、このようにして得られた各試料の二次再結晶
粒の方位分布を示す。第3図より、{110}<uuw>方位
粒は熱延板の表面部から切り出した試料より、また{10
0}<001>方位粒は、中心部より切り出した試料より発
達していることが分る。
FIG. 3 shows the orientation distribution of the secondary recrystallized grains of each sample thus obtained. From Fig. 3, the {110} <uuw> oriented grains are shown in the sample cut from the surface of the hot rolled sheet,
It can be seen that the 0} <001> oriented grains are developed in the sample cut out from the central portion.

従って、磁束密度低下の原因となる{110}<uuw>方位
粒は、熱延板における表面部を除去することにより、抑
制することができる。
Therefore, the {110} <uuw> oriented grains that cause a decrease in the magnetic flux density can be suppressed by removing the surface portion of the hot rolled sheet.

第4図に、熱延板の表面からグラインダーで除去した量
と、製品の磁束密度(B8値)の関係を示す。この結果よ
り、表面層より全厚の1/10以上、望ましくは1/5以上除
去することにより、高磁束密度の二方向性電磁鋼板が製
造できることが分る。
Fig. 4 shows the relationship between the amount removed by a grinder from the surface of the hot-rolled sheet and the magnetic flux density (B 8 value) of the product. From this result, it can be seen that a grain-oriented electrical steel sheet having a high magnetic flux density can be manufactured by removing 1/10 or more, preferably 1/5 or more of the total thickness from the surface layer.

なお、鋼板表面層よりの除去量が全厚の1/3程度になる
と磁気特性が飽和する。
The magnetic properties saturate when the amount removed from the steel sheet surface layer is about 1/3 of the total thickness.

次に、本発明の実施形態を説明する。Next, an embodiment of the present invention will be described.

本発明における鋼板の成分は、Si;0.8〜6.7%、酸可溶
性Al;0.008〜0.048%、N≦0.010%、残部Feおよび不可
避的不純物である。
The components of the steel sheet in the present invention are Si: 0.8 to 6.7%, acid-soluble Al: 0.008 to 0.048%, N ≦ 0.010%, balance Fe and unavoidable impurities.

Siは、4.8%を越えると冷間圧延時に割れが生じ易くな
る。温間圧延により圧延できる6.7%を上限とする。一
方Si量が少ないと、仕上焼鈍時にα→γ変態を生じ、結
晶の方向性を破壊するので、実質的に結晶の方向性に影
響を及ぼさない0.8%を下限とする。
If Si exceeds 4.8%, cracking tends to occur during cold rolling. The upper limit is 6.7% that can be rolled by warm rolling. On the other hand, when the amount of Si is small, α → γ transformation occurs during finish annealing and destroys the crystal orientation. Therefore, the lower limit is 0.8%, which does not substantially affect the crystal orientation.

酸化溶性AlはAlN,(Al,Si)N等として窒化物を形成
し、インヒビターを形成する。製品の磁束密度が高くな
る0.008〜0.048%、望ましくは0.018〜0.036%を限定範
囲とする。
Oxidizing Al forms a nitride as AlN, (Al, Si) N, etc., and forms an inhibitor. The limiting range is 0.008 to 0.048%, preferably 0.018 to 0.036%, which increases the magnetic flux density of the product.

Nは0.010%を超えて含有するとブリスターと呼ばれる
鋼板の空孔を生じるので、0.010%を上限とする。
If N is contained in excess of 0.010%, vacancies in the steel sheet called blisters occur, so the upper limit is 0.010%.

他に、Mn,S,Se,B,Bi,Nb,Sn,Ti等のインヒビター構成元
素を添加することもできる。
In addition, an inhibitor constituent element such as Mn, S, Se, B, Bi, Nb, Sn, or Ti can be added.

上記成分からなる素材は、通常の工程を通し、熱延板と
される。この熱延板の両面より少なくとも全厚の1/10以
上ずつ除去することが、本発明の特徴とするところであ
る。この除去の方法については、特に限定しない。グラ
インダー等による機械的研削、塩酸等による化学的研磨
等、いずれの方法でも良い。
The raw material composed of the above components is made into a hot-rolled sheet through a usual process. It is a feature of the present invention to remove at least 1/10 or more of the total thickness from both surfaces of the hot rolled sheet. The method of this removal is not particularly limited. Either method such as mechanical grinding with a grinder or chemical polishing with hydrochloric acid may be used.

また、この表面層を除去する段階は、熱延板に限らず、
熱延板焼鈍後、冷延後、一次再結晶焼鈍後のいずれの段
階においてもその効果は発揮されるが、表面層を除去す
るコストより熱延板の段階が好ましいと考えられる。
Further, the step of removing this surface layer is not limited to the hot rolled sheet,
The effect is exhibited in any of the steps of annealing after hot rolling, cold rolling and after primary recrystallization annealing, but it is considered that the hot rolling step is preferable from the cost of removing the surface layer.

前記熱延板は、直ちに、もしくは焼鈍工程を経て冷間圧
延される。上記焼鈍は、750〜1200℃の温度域で30秒〜3
0分行なわれることが望ましい。この焼鈍は、製品の磁
束密度を高めるのに有効であり、望む磁束密度の水準と
コストを勘案して採否を決めると良い。
The hot rolled sheet is cold rolled immediately or after an annealing step. The above annealing is performed in the temperature range of 750 to 1200 ° C for 30 seconds to 3 seconds.
It is desirable to run for 0 minutes. This annealing is effective in increasing the magnetic flux density of the product, and it is advisable to decide whether or not to adopt it in consideration of the desired level of magnetic flux density and the cost.

冷間圧延工程は、基本的に、特公昭35−2657号公報、或
は特公昭38−8213号公報に開示されたものと同じであ
る。本発明においては、40〜80%の圧下率で一方向に冷
間圧延し、次いで前記方向と交叉する方向に30〜70%の
圧下率で冷間圧延を行う。特に、最初の冷間圧延と交叉
する方向に冷間圧延する場合、特公昭62−45007号公報
に開示されている方法によると、ストリップの形態のま
ま冷間圧延でき、経済面で効果的である。
The cold rolling process is basically the same as that disclosed in JP-B-35-2657 or JP-B-38-8213. In the present invention, cold rolling is performed in one direction at a reduction rate of 40 to 80%, and then cold rolling is performed at a reduction rate of 30 to 70% in a direction intersecting the direction. In particular, when cold rolling in a direction intersecting with the first cold rolling, according to the method disclosed in Japanese Patent Publication No. 62-45007, cold rolling can be carried out in the form of strip, which is economically effective. is there.

冷間圧延後の材料は、通常鋼中に含まれるCを除去する
ことを兼ね、必要に応じて湿潤雰囲気中750〜1000℃の
温度域で30秒から10分間、一次再結晶焼鈍を行う。
The material after cold rolling usually serves to remove C contained in steel, and if necessary, is subjected to primary recrystallization annealing in a wet atmosphere in a temperature range of 750 to 1000 ° C. for 30 seconds to 10 minutes.

このようにして得られた材料に、MgOを主成分とする焼
鈍分離剤を塗布し、乾燥した後、仕上焼鈍を行う。仕上
焼鈍は、二次再結晶と、純化を目的とし、通常900〜120
0℃の温度で焼鈍される。
The material thus obtained is coated with an annealing separating agent containing MgO as a main component, dried, and then subjected to finish annealing. Finish annealing is usually 900-120 for the purpose of secondary recrystallization and purification.
Annealed at a temperature of 0 ° C.

特に、特願昭63−293645号公報に示すように、二次再結
晶と純化を分離し、950〜1100℃の温度域で二次再結晶
させ、その後1100℃以上に昇温し純化を行うことが磁束
密度を高めるうえで望ましい。
In particular, as shown in Japanese Patent Application No. 63-293645, secondary recrystallization and purification are separated, secondary recrystallization is performed in a temperature range of 950 to 1100 ° C, and then the temperature is raised to 1100 ° C or higher for purification. Is desirable to increase the magnetic flux density.

〔実施例〕〔Example〕

実施例1. 重量%で、C;0.048%、Si;3.40%、Mn;0.14%、酸可溶
性Al;0.023%、N;0.0072%、残部Feおよび不可避的不純
物からなる1.8mm厚さの熱延鋼板を該鋼板の両面よりそ
れぞれ全厚の1/4ずつグラインダーで研削した試料
(A)と研削なしの試料(B)の2種類の試料とした。
これらの試料は熱間圧延と同一方向に55%、次いで前記
冷間圧延方向と交叉する方向に55%の冷間圧延を施こす
交叉圧延を行った。これらの冷延板を810℃で120秒間脱
炭を兼ねる一次再結晶焼鈍を行った。次いで、焼鈍分離
剤としてMgOを塗布した後、N225%+H275%の雰囲気中
で15℃/hrの昇温速度で1025℃迄昇温し、1025℃で20時
間保持して二次再結晶を完了させた。その後1200℃で20
時間H2100%の雰囲気中で純化焼鈍を行った。これらの
製品の磁気特性は第1表に示すとおりであった。
Example 1. By weight%, C; 0.048%, Si; 3.40%, Mn; 0.14%, acid soluble Al; 0.023%, N; 0.0072%, the balance of 1.8 mm thick hot-rolled Fe and inevitable impurities Two types of samples, a sample (A) and a sample (B) without grinding, were prepared by grinding the steel plate from both sides by 1/4 of the total thickness with a grinder.
These samples were cross-rolled by subjecting them to 55% cold rolling in the same direction as hot rolling and then 55% in a direction intersecting the cold rolling direction. These cold-rolled sheets were subjected to primary recrystallization annealing at 810 ° C for 120 seconds, which also serves as decarburization. Then, after applying MgO as an annealing separator, the temperature was raised to 1025 ° C at a temperature rising rate of 15 ° C / hr in an atmosphere of N 2 25% + H 2 75%, and the temperature was maintained at 1025 ° C for 20 hours for the second time. The recrystallization was completed. Then at 1200 ℃ 20
Purification annealing was performed in an atmosphere of H 2 100% for a time. The magnetic properties of these products were as shown in Table 1.

実施例2. 実施例1と同様の熱延鋼板を該鋼板の両面よりそれぞれ
全厚の1/4ずつグラインダーで研削した試料(A)と研
削なしの試料(B)の2種類の試料とした。これらの試
料を1070℃で2分間焼鈍し、以降実施例1と同一の工程
で処理した。
Example 2 A hot rolled steel sheet similar to that of Example 1 was used as two types of samples, a sample (A) ground from both sides of the steel sheet by 1/4 of the total thickness by a grinder and a sample (B) without grinding. . These samples were annealed at 1070 ° C. for 2 minutes and then processed in the same steps as in Example 1.

これらの製品の磁気特性は第2表に示すとおりであっ
た。
The magnetic properties of these products were as shown in Table 2.

〔発明の効果〕 本発明は、以上述べたように、現在最高レベルの一方向
性電磁鋼板と同等以上の高磁束密度の二方向性電磁鋼板
を工業的に安定して製造できるので、その効果は甚大で
ある。
[Advantages of the Invention] As described above, the present invention is capable of industrially stably producing a bidirectional electrical steel sheet having a high magnetic flux density equal to or higher than that of the currently highest level unidirectional electrical steel sheet. Is enormous.

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

第1図は一次再結晶板の(a)表面層と(b)中心層の
集合組織を示す(200)極点図であり、 第2図は、熱延板の板厚方向の集合組織を示す図であ
り、 第3図は、(a)表面層と(b)中心層のそれぞれの部
位より切り出した試料の二次再結晶の方位分布を示す
(200)極点図であり、 第4図は、熱延板の表面からの減厚量と製品の磁束密度
の関係を示す図である。
FIG. 1 is a (200) pole figure showing the texture of the (a) surface layer and (b) center layer of the primary recrystallized sheet, and FIG. 2 shows the texture of the hot rolled sheet in the sheet thickness direction. FIG. 3 is a (200) pole figure showing the orientation distribution of the secondary recrystallization of the sample cut out from the respective parts of (a) the surface layer and (b) the central layer, and FIG. FIG. 3 is a diagram showing the relationship between the amount of reduction in thickness from the surface of the hot rolled sheet and the magnetic flux density of the product.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】重量%で、Si;0.8〜6.7%、酸可溶性Al;0.
008〜0.048%、N≦0.010%、残部Feおよび不可避的不
純物からなる熱延板を、圧下率40〜80%で冷間圧延し、
更に前記冷間圧延と交叉する方向に圧下率30〜70%で冷
間圧延し、次いで一次再結晶焼鈍後、焼鈍分離剤を塗布
し、二次再結晶と純化を目的とした仕上焼鈍を行う二方
向性電磁鋼板の製造法において、 熱延板表層部を厚さ方向両面よりそれぞれ全厚の1/10以
上除去することを特徴とする高磁束密度二方向性電磁鋼
板の製造方法。
1. Si: 0.8-6.7%, acid-soluble Al;
008 ~ 0.048%, N ≤ 0.010%, the hot rolled sheet consisting of balance Fe and unavoidable impurities is cold rolled at a reduction rate of 40 to 80%,
Further, cold rolling is performed at a reduction rate of 30 to 70% in a direction intersecting with the cold rolling, then after primary recrystallization annealing, an annealing separator is applied, and secondary annealing and finishing annealing for the purpose of purification are performed. A method for producing a bi-directional electrical steel sheet having a high magnetic flux density, which comprises removing the surface layer portion of the hot-rolled sheet from both sides in the thickness direction by 1/10 or more of the total thickness in the production method of the bi-directional electrical steel sheet.
【請求項2】冷間圧延前に750〜1200℃の温度範囲で30
秒〜30分間焼鈍する請求項1記載の方法。
2. Before cold rolling, the temperature is in the range of 750 to 1200 ° C.
The method according to claim 1, wherein annealing is performed for seconds to 30 minutes.
JP2097718A 1990-04-12 1990-04-16 High magnetic flux density bi-directional electrical steel sheet manufacturing method Expired - Fee Related JPH0733546B2 (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP2097718A JPH0733546B2 (en) 1990-04-16 1990-04-16 High magnetic flux density bi-directional electrical steel sheet manufacturing method
KR1019910005878A KR930010323B1 (en) 1990-04-12 1991-04-12 Process for manufacturing double oriented electrical steel sheet having high magnetic flux density
DE69129130T DE69129130T2 (en) 1990-04-12 1991-04-12 Process for producing double-oriented electrical sheets with high magnetic flux density
EP91303278A EP0452153B1 (en) 1990-04-12 1991-04-12 Process for manufacturing double oriented electrical steel sheet having high magnetic flux density
US08/034,615 US5346559A (en) 1990-04-12 1993-03-19 Process for manufacturing double oriented electrical steel sheet having high magnetic flux density

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2097718A JPH0733546B2 (en) 1990-04-16 1990-04-16 High magnetic flux density bi-directional electrical steel sheet manufacturing method

Publications (2)

Publication Number Publication Date
JPH04322A JPH04322A (en) 1992-01-06
JPH0733546B2 true JPH0733546B2 (en) 1995-04-12

Family

ID=14199675

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2097718A Expired - Fee Related JPH0733546B2 (en) 1990-04-12 1990-04-16 High magnetic flux density bi-directional electrical steel sheet manufacturing method

Country Status (1)

Country Link
JP (1) JPH0733546B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6786900B2 (en) * 2016-06-16 2020-11-18 日本製鉄株式会社 Bidirectional electromagnetic steel sheet and its manufacturing method
JP6844127B2 (en) * 2016-06-16 2021-03-17 日本製鉄株式会社 Iron core, re-cold-rolled steel sheet, steel core laminate, re-cold-rolled steel sheet manufacturing method, iron core laminate manufacturing method, and iron core manufacturing method

Also Published As

Publication number Publication date
JPH04322A (en) 1992-01-06

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