JPH042721A - Production of double oriented silicon steel sheet having high magnetic flux density - Google Patents
Production of double oriented silicon steel sheet having high magnetic flux densityInfo
- Publication number
- JPH042721A JPH042721A JP2103180A JP10318090A JPH042721A JP H042721 A JPH042721 A JP H042721A JP 2103180 A JP2103180 A JP 2103180A JP 10318090 A JP10318090 A JP 10318090A JP H042721 A JPH042721 A JP H042721A
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- magnetic flux
- flux density
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- hot
- annealing
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Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、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 [Field of Industrial Application] The present invention provides a steel plate having an easy magnetization axis <001> orientation in the longitudinal direction of the steel sheet and in a direction perpendicular to the longitudinal direction, and a (100) plane appearing on the rolled surface. (with Miller index (100
) The present invention relates to a method of manufacturing a so-called bidirectional electrical steel sheet composed of crystal grains (expressed as <001>).
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。Bidirectional electrical steel sheets have easy magnetization axes (<001> axes) in the rolling direction and in the direction perpendicular to the rolling direction, and have excellent magnetic properties in both directions, so they have excellent magnetic properties only in the rolling direction. It is advantageous to use it as a magnetic core material for devices that require magnetic flux to flow in two directions, such as large rotors, compared to unidirectional electrical steel sheets. In addition, in the field of small static devices, non-oriented electrical steel sheets that do not have a high concentration of easily magnetized axes are generally used, but by using bidirectional electrical steel sheets, it is possible to achieve smaller size and higher efficiency. There is sex.
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−般に使用されるに至っ
ていない。As mentioned above, bidirectional electrical steel sheets have excellent properties, and although their commercialization has been long awaited, to date they have not been generally used as industrial products.
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 two main methods for manufacturing conventional bidirectional electrical steel sheets:
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。One method, as disclosed in Japanese Patent Publication No. 37-7110, is to perform high-temperature annealing in an atmosphere containing a polar gas, such as hydrogen sulfide, and utilize surface energy to
) This is a method of secondary recrystallization of <001> oriented grains.
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。However, this method requires strict control of the surface energy of the steel plate and is unsuitable for mass production processes.
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1.85TeSia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 method, as disclosed in Japanese Patent Publication No. 35-2657, involves cold rolling in one direction and then cold rolling in a direction that intersects with the above-mentioned cold rolling. "Cold rolling method". However, the magnetic flux density (B8) of the product obtained by this method is less than 1.85 TeSia, and it does not have excellent magnetic properties that are commensurate with the high cost due to the complexity of the manufacturing process. cannot compete with electromagnetic steel sheets.
一方向性電磁鋼板の磁束密度(B8)は、特公昭40−
15644号公報、特公昭51−13469号公報記載
の技術が発明されて以来、急速に進歩し、現在、磁束密
度(B6)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 (B8) of unidirectional electrical steel sheet is
Since the technology described in Japanese Patent Publication No. 15644 and Japanese Patent Publication No. 51-13469 was invented, rapid progress has been made, and products with a high magnetic flux density (B6) of 1.92 T are now 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 bidirectional electrical steel sheets, Japanese Patent Publication No. 35-17208 and Japanese Patent Publication No. 38-8213 are published to improve magnetic properties.
Although improved techniques have been proposed in the above publication, none of them have been able to stably produce products with high magnetic flux density that can compete with unidirectional electrical steel sheets and the like.
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 manufacturing technology that it is not possible to stably obtain products with high magnetic flux density from bidirectional electrical steel sheets.
本発明は上記課題を解決するために、重量%で、Si:
1.8〜6.7%、酸可溶性Aβ: 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30〜7
0%で冷間圧延し、次いで一次再結晶焼鈍し、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方法において、上記熱間圧
延の最終3パスの累積圧下率を80%以下とする二方向
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-mentioned problems, the present invention has been made to solve the above problems, in terms of weight%, Si:
1.8-6.7%, acid-soluble Aβ: 0.008-0,
048%, N≦0.010%, the balance Fe and unavoidable impurities, the hot rolled plate is cold rolled at a rolling reduction of 40 to 80%, and further rolled in a direction crossing the cold rolling at a rolling reduction of 30 to 7.
In the method for producing a bidirectional electrical steel sheet, the above-mentioned hot rolling The present invention provides a method for producing a bidirectional electrical steel sheet in which the cumulative rolling reduction rate of the final three passes is 80% or less.
以下、本発明について詳細に説明する。The present invention will be explained in detail below.
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 obtained the following new findings from an investigation of products of bidirectional electrical steel sheets manufactured 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) <uvw>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) <uVW>方位粒の二次再結晶を抑制すれば
良い。The characteristic crystal orientation of bidirectional electrical steel sheets is (100)
<001> orientation, but among the secondary recrystallized grains, there are also (110) <uvw> orientation grains in addition to this oriented grain, and the latter oriented grains are the cause of lowering the magnetic flux density. ing. Therefore, in order to achieve high magnetic flux density, (
110) Secondary recrystallization of <uVW> 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を行
った結果、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)<uVW >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 research on these oriented grains, the present inventors found that the texture of the primary recrystallized plate before secondary recrystallization differs in the thickness direction, and the (110)<uVW> oriented grains It was found that (100) <001> oriented grains develop from the central layer from the surface 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 was obtained through the following experiment.
C:0.055%、Si:3.3%、酸可溶性AA :
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11
25℃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。この冷延板を湿水素中810℃で210秒間脱炭を
兼ねる一次再結晶焼鈍を行った。この−次回結晶板の集
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>、 (21N<231
>方位を主方位とするものであり、板厚方向で異なるも
のであることが判肋した。二次再結晶方位は、例えばに
、T、Au5t、 J、W、Rutter ;Tran
s。C: 0.055%, Si: 3.3%, acid soluble AA:
0.028%, N: 0.007%, balance Fe and unavoidable impurities.
Annealed at 25°C for 2 minutes, cold rolled in the same direction as the hot rolling direction at a rolling reduction of 55%, and then rolled in the same direction as the hot rolling direction at a rolling reduction of 55%.
It was cross-cold rolled at a rolling reduction of 0.35 mm to a final thickness of 0.35 mm. This cold-rolled sheet was subjected to primary recrystallization annealing, which also served as decarburization, at 810° C. for 210 seconds in wet hydrogen. When the texture of this -next crystal plate was investigated, as shown in Figure 1, the main orientations were (111) and <uvw> at the surface, and (211) <124> and (21N<231) at the center.
> direction as the main direction, and it was determined that the direction differs in the thickness direction. The secondary recrystallization orientation is, for example, T, Au5t, J, W, Rutter; Tran
s.
Met、Sor、 AIME 215(1959年)
P119/127 、牛神他日本金属学会第96回講演
大会概要集373頁に述べられているように、−次再結
晶集合組織の影響を強く受けるものである。この−次再
結晶集合組織の板厚方向の差の原因を検討した結果第2
図に示す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。Met, Sor, AIME 215 (1959)
P119/127, as described in page 373 of the summary collection of the 96th Lecture Conference of the Japan Institute of Metals by Ushigami et al., it is strongly influenced by the -order recrystallization texture. As a result of examining the cause of the difference in the -order recrystallization texture in the sheet thickness direction, the second
It was found that this is greatly influenced by the gradient of the texture in the thickness direction of the hot rolled sheet shown in the figure. Therefore, a surface portion and a center portion were cut out from the hot-rolled sheet, and after primary recrystallization was performed under the same conditions as above, an annealing separator containing MgO as a main component was applied, and final 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)<uvt
v >方位粒は熱延板の表面部から切り出した試料(図
中(a))において、また(100) <001>方位
粒は、中心部より切り出した試料(図中(b))におい
てそれぞれ発達していることが分る。FIG. 3 shows the orientation distribution of secondary recrystallized grains of each sample thus obtained. From Figure 3, (110)<uvt
v > oriented grains are present in the sample cut from the surface of the hot rolled sheet ((a) in the figure), and (100) <001> oriented grains are present in the sample cut from the center ((b) in the figure). I can see that it is developing.
従って、磁束密度低下の原因となる(110 )<uv
w >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, (110) < uv, which causes a decrease in magnetic flux density.
w > oriented grains can be suppressed by removing the surface portion of the hot rolled sheet.
本発明者等は、上記知見を基に熱間圧延条件を詳細に検
討した結果、最終3パスの累積圧下率を80%以下にす
ること、また特に熱延終了温度を950℃以上とするこ
とにより、熱延板の集合組織を変え、表面部からの(1
10) <uVW>方位二次再結晶粒の発達を抑制し、
磁束密度の高い二方向性電磁鋼板を安定して製造できる
ことを見出した。As a result of detailed study of hot rolling conditions based on the above knowledge, the present inventors determined that the cumulative reduction rate of the final three passes should be 80% or less, and in particular, the hot rolling end temperature should be 950°C or higher. By changing the texture of the hot-rolled sheet, the (1
10) Suppressing the development of <uVW> oriented secondary recrystallized grains,
We have discovered that it is possible to stably produce bidirectional electrical steel sheets with high magnetic flux density.
その実験結果を説明する。前述と同一の40mm厚のス
ラブをパス・スケジュールを変え計6パスで2、0 m
m厚の熱延板に熱延した。熱延終了温度は900〜95
0℃であった。その後、1050℃で2分間焼鈍し、熱
延方向と同一方向に50%の圧下率で冷延し、次いで前
記圧延方向と直角方向に50%の圧下率で交叉冷間圧延
した。湿水素雰囲気中で800℃で90秒脱炭を兼ねる
一次再結晶焼鈍後、焼鈍分離剤を塗布し仕上焼鈍を行っ
た。The experimental results will be explained. The same 40 mm thick slab as mentioned above was processed by changing the pass schedule and was completed in 6 passes totaling 2.0 m.
It was hot-rolled into a hot-rolled sheet with a thickness of m. Hot rolling finish temperature is 900-95
It was 0°C. Thereafter, it was annealed at 1050° C. for 2 minutes, cold rolled in the same direction as the hot rolling direction at a rolling reduction of 50%, and then cross-cold rolled in a direction perpendicular to the rolling direction at a rolling reduction of 50%. After primary recrystallization annealing, which also serves as decarburization, at 800° C. in a wet hydrogen atmosphere for 90 seconds, an annealing separator was applied and final annealing was performed.
第4図に、熱間圧延の最終3パスの累積圧下率と製品の
磁気特性(B e値)を示す。この図より、累積圧下率
80%以下で1.90Tesla以上という高い磁束密
度の製品が得られることが分る。FIG. 4 shows the cumulative reduction ratio of the final three passes of hot rolling and the magnetic properties (B e value) of the product. From this figure, it can be seen that a product with a high magnetic flux density of 1.90 Tesla or more can be obtained with a cumulative reduction rate of 80% or less.
この知見を基に、最#3パスの累積圧下率50%の条件
下でパス間のデイレイタイムを変え熱延終了温度の影響
を検討したところ特に、熱延終了温度950℃以上で更
に、磁束密度が向上することが分った。Based on this knowledge, we investigated the influence of the hot rolling end temperature by changing the inter-pass delay time under the condition of a cumulative reduction rate of 50% in the #3 pass, and found that the magnetic flux further increased when the hot rolling end temperature was 950°C or higher. It was found that the density was improved.
熱延板の集合組織を調査したところ、磁束密度が高い場
合は、いずれも、熱延板の表面部の(110)面が少な
くなっていた。従って本発明に従い、最終の3パスの累
積圧下率を80%以下とした場合は、表面の剪断変形に
よる結晶回転を抑制し、また熱延終了温度を950℃以
上とした場合は、表面の剪断変形により、形成された(
110 )集合組織を再結晶等により低下させたものと
考えられる。When the texture of the hot-rolled sheets was investigated, it was found that in all cases where the magnetic flux density was high, the number of (110) planes on the surface of the hot-rolled sheets decreased. Therefore, according to the present invention, when the cumulative reduction rate of the final three passes is set to 80% or less, crystal rotation due to surface shear deformation is suppressed, and when the hot rolling end temperature is set to 950°C or higher, surface shear Due to deformation, the formed (
110) It is thought that the texture was reduced by recrystallization or the like.
以下、本発明の構成要件の限定理由を実施形態に従い、
説明する。Below, the reasons for limiting the constituent elements of the present invention will be explained according to the embodiments.
explain.
本発明で用いる溶鋼は、転炉、電気炉等その溶製方法を
問わないが、成分として次の含有範囲を必須のものとす
る。The molten steel used in the present invention may be produced by any method such as a converter or an electric furnace, but the following content ranges as components are essential.
Si は、含有量を多くすると、鉄損特性を向上するこ
とができるので望ましいが、逆に磁束密度を低下する。Increasing the content of Si is desirable because it can improve iron loss characteristics, but it conversely decreases magnetic flux density.
含有量が約6.5%前後で最低鉄損となり、それ以上増
加しても、改善効果はないので、上限を6.7%とした
。S1含有量を増加すると脆化が著しく、4.5%以上
で冷間割れが発生するが、温間圧延を行うことにより基
本的には圧延が可能である。一方、S1含有量が少なく
なると仕上焼鈍時にα→γ変態を生じ、結晶の方向性が
損なわれるので、実質的に影響を及ぼさない0.8%を
下限とする。The lowest iron loss is reached when the content is around 6.5%, and even if it increases further, there is no improvement effect, so the upper limit was set at 6.7%. When the S1 content is increased, embrittlement becomes significant, and when the S1 content exceeds 4.5%, cold cracking occurs, but rolling is basically possible by performing warm rolling. On the other hand, if the S1 content decreases, α→γ transformation will occur during final annealing, and the crystal orientation will be impaired, so the lower limit is set at 0.8%, which has no substantial effect.
酸可溶性Aβは、AβN、 (i 、 5i)N等の窒
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。Acid-soluble Aβ forms nitrides such as AβN, (i, 5i)N, and forms inhibitors. The limited range is 0.008% to 0.048%, preferably 0.018% to 0.036%, where the magnetic flux density of the product is high.
Nは、0.010%を超えて含有すると鋼板に、ブリス
ターと呼ばれる空孔を生じるので、0.010%を上限
とする。下限については、途中工程で窒化することによ
り調節することができるので、特に限定しない。If N is contained in an amount exceeding 0.010%, voids called blisters are formed in the steel sheet, so the upper limit is set at 0.010%. The lower limit is not particularly limited, as it can be adjusted by nitriding in an intermediate step.
他に、Mn、S、Se、B、Bi、Nb、Sn、T1C
r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, Mn, S, Se, B, Bi, Nb, Sn, T1C
Inhibitor constituent elements such as r can also be added.
上記成分からなるスラブは、加熱された後、所定の板厚
まで熱間圧延される。この際の最終の累積圧下率を80
%以下とすることが本発明の特徴とするところである。A slab made of the above components is heated and then hot rolled to a predetermined thickness. The final cumulative reduction rate at this time is 80
% or less is a feature of the present invention.
この熱延板は、直ちに、もしくは750〜1200℃の
温度域での30秒〜30分間の短時間焼鈍工程を経て冷
間圧延が施される。上記焼鈍は、製品の磁束密度を高め
るのに有用であり、望む製品の磁束密度の水準に応じて
焼鈍の採否を決めれば良い。This hot-rolled sheet is subjected to cold rolling immediately or through a short-time annealing process of 30 seconds to 30 minutes at a temperature range of 750 to 1200°C. The above-mentioned annealing is useful for increasing the magnetic flux density of the product, and whether or not to apply the annealing may be determined depending on the level of the desired magnetic flux density of the product.
交叉冷間圧延は、基本的に特公昭35−2657号公報
、或いは特公昭38−8213号公報に開示されたもの
と同じである。Cross cold rolling is basically the same as that disclosed in Japanese Patent Publication No. 35-2657 or Japanese Patent Publication No. 38-8213.
冷間圧延後の材料は、通常鋼中に含まれるCを除去する
ことも兼ね雰囲気露点を調節した雰囲気内で、750〜
1000℃の温度域において30秒から10分間焼鈍し
、−次男結晶させる。After cold rolling, the material is rolled in an atmosphere with a controlled dew point, which also serves to remove carbon contained in normal steel.
Annealing is performed in a temperature range of 1000° C. for 30 seconds to 10 minutes to form crystals.
その後MgOを主成分とする焼鈍分離剤を塗布した後、
二次再結晶と純化を目的とした仕上焼鈍を施す。After that, after applying an annealing separator mainly composed of MgO,
Final annealing is performed for the purpose of secondary recrystallization and purification.
特に、特願昭63−293645号公報に示すように、
二次再結晶と純化の工程を分離し、950〜1100℃
の温度域で二次再結晶を完了させた後、1100℃以上
で純化を行うことが磁束密度を高めるために有効である
。In particular, as shown in Japanese Patent Application No. 63-293645,
The secondary recrystallization and purification steps are separated, and the temperature is 950-1100℃.
After completing secondary recrystallization in a temperature range of 1,100° C. or higher, it is effective to perform purification at a temperature of 1100° C. or higher in order to increase the magnetic flux density.
実施例1
重量%で、C: 0.05%、Si:3.2%、Mn:
0.1%、酸可溶性/l:o、03%、 N : 0.
08%含有する26mm厚のスラブを1150℃の温度
に加熱した後、■ 26→20−18−15−8−4−
2 (mm)■26→15→7−3.5−3→2.5
→2 (mm)の条件下で熱延して2. Omm厚の熱
延板とした。熱延終了後は1秒間空冷し、その後550
℃迄水冷し1時間保持した後炉冷した。この熱延板を1
120℃で2分間焼鈍し、熱延方向に50%の圧下率で
冷間圧延し、次いで前記冷延方向と直角方向に50%の
圧下率で交叉冷間圧延を行った。その後800℃で21
0秒間、脱炭を兼ねる一次再結晶焼鈍を行い、焼鈍分離
剤を塗布し、二次再結晶と純化を目的とする仕上焼鈍を
行った。製品の磁気特性を第1表に示す。Example 1 In weight%, C: 0.05%, Si: 3.2%, Mn:
0.1%, acid soluble/l:o, 03%, N: 0.
After heating a 26 mm thick slab containing 0.08% to a temperature of 1150 °C, ■ 26 → 20-18-15-8-4-
2 (mm)■26→15→7-3.5-3→2.5
→ Hot rolled under the condition of 2 (mm) 2. It was made into a hot-rolled sheet with a thickness of 0 mm. After hot rolling, air cooling for 1 second, then 550
The mixture was cooled with water to ℃ and kept for 1 hour, then cooled in a furnace. This hot rolled plate is 1
It was annealed at 120° C. for 2 minutes, cold rolled in the hot rolling direction at a rolling reduction of 50%, and then cross-cold rolled in a direction perpendicular to the cold rolling direction at a rolling reduction of 50%. Then 21 at 800℃
Primary recrystallization annealing, which also serves as decarburization, was performed for 0 seconds, an annealing separator was applied, and final annealing was performed for the purpose of secondary recrystallization and purification. The magnetic properties of the product are shown in Table 1.
第 1 表
第2表
実施例2
実施例1と同一のスラブを用い、熱延開始温度■110
0℃■1000℃■900℃の条件で、次の6パス即ち
、26→15→6→3.2→2.8→2.4→2 (
mm)で熱延を行い、2.0釦の板厚とした。その後、
実施例1と同一の条件で仕上焼鈍迄行った。製品の磁気
特性を第2表に示す。Table 1 Table 2 Example 2 Using the same slab as Example 1, hot rolling start temperature ■110
Under the conditions of 0℃ ■ 1000℃ ■ 900℃, the following 6 passes, namely 26 → 15 → 6 → 3.2 → 2.8 → 2.4 → 2 (
mm) and was hot rolled to a plate thickness of 2.0 buttons. after that,
Finish annealing was carried out under the same conditions as in Example 1. The magnetic properties of the product are shown in Table 2.
以下余白
〔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。Blank space below [Effects of the Invention] As described above, the present invention enables industrially stable production of bi-grained electrical steel sheets with a high magnetic flux density equal to or higher than that of the current highest level uni-grained electrical steel sheets. The effect is enormous.
第1図は一次再結晶板の表面層(同図(a))と中心層
(同図(b))の集合組織を示す(200)極点図であ
り、
第2図は、熱延板の板厚方向における集合組織の面強度
を示す図であり、
第3図は、表面層(同図(a))と、中心層(同図b)
)のそれぞれの部位より切り出した材料の二次再結晶の
方位分布を示す(200)極点図であり、第4図は、熱
間圧延の最′#3バスの累積圧下率と製品の磁束密度の
関係を示す図である。Figure 1 is a (200) pole figure showing the texture of the surface layer ((a) in the same figure) and the center layer ((b) in the same figure) of the primary recrystallized plate, and Figure 2 is the (200) pole figure of the hot-rolled plate. FIG. 3 is a diagram showing the surface strength of the texture in the plate thickness direction, and FIG.
) is a (200) pole figure showing the orientation distribution of secondary recrystallization of the material cut out from each part of the material, and Figure 4 shows the cumulative reduction ratio of the #3 bath of hot rolling and the magnetic flux density of the product. FIG.
Claims (2)
l: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4
0〜80%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
結晶焼鈍し、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方法
において、上記熱間圧延の最終3パスの累積圧下率を8
0%以下とすることを特徴とする磁束密度の高い二方向
性電磁鋼板の製造方法。(1) In weight%, Si: 1.8-6.7%, acid-soluble A
l: 0.008 to 0.048%, N≦0.010%, balance Fe and unavoidable impurities.
Cold rolling at 0 to 80%, further cold rolling at a reduction rate of 30 to 70% in the direction crossing the cold rolling, then primary recrystallization annealing, applying an annealing separator, and secondary recrystallization. In a method for manufacturing bidirectional electrical steel sheets in which finish annealing is performed for the purpose of purification, the cumulative reduction rate of the final three passes of the above hot rolling is set to 8.
A method for producing a bidirectional electrical steel sheet with a high magnetic flux density, characterized in that the magnetic flux density is 0% or less.
求項1記載の方法。(2) The method according to claim 1, wherein the hot rolling end temperature is 950°C or higher.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2103180A JPH0733547B2 (en) | 1990-04-20 | 1990-04-20 | Method of manufacturing bidirectional electrical steel sheet with 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 |
| KR1019910005878A KR930010323B1 (en) | 1990-04-12 | 1991-04-12 | Process for manufacturing double oriented electrical steel sheet having 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 |
|---|---|---|---|
| JP2103180A JPH0733547B2 (en) | 1990-04-20 | 1990-04-20 | Method of manufacturing bidirectional electrical steel sheet with high magnetic flux density |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH042721A true JPH042721A (en) | 1992-01-07 |
| JPH0733547B2 JPH0733547B2 (en) | 1995-04-12 |
Family
ID=14347311
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2103180A Expired - Fee Related JPH0733547B2 (en) | 1990-04-12 | 1990-04-20 | Method of manufacturing bidirectional electrical steel sheet with high magnetic flux density |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0733547B2 (en) |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH08223830A (en) * | 1995-02-10 | 1996-08-30 | Toshiba Corp | Iron cores and salient pole rotor cores for rotating electrical machines |
| JPH08223831A (en) * | 1995-02-10 | 1996-08-30 | Toshiba Corp | Iron cores and rotor cores for rotating electrical machines |
| JP2017222910A (en) * | 2016-06-16 | 2017-12-21 | 新日鐵住金株式会社 | Bidirectional electrical steel sheet and manufacturing method thereof |
| JP2017222911A (en) * | 2016-06-16 | 2017-12-21 | 新日鐵住金株式会社 | Iron core, cold re-rolled steel sheet, cold re-rolled steel sheet manufacturing method, and iron core manufacturing method |
| CN120060725A (en) * | 2025-04-28 | 2025-05-30 | 太原科技大学 | Double-oriented silicon steel and preparation method thereof |
-
1990
- 1990-04-20 JP JP2103180A patent/JPH0733547B2/en not_active Expired - Fee Related
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH08223830A (en) * | 1995-02-10 | 1996-08-30 | Toshiba Corp | Iron cores and salient pole rotor cores for rotating electrical machines |
| JPH08223831A (en) * | 1995-02-10 | 1996-08-30 | Toshiba Corp | Iron cores and rotor cores for rotating electrical machines |
| JP2017222910A (en) * | 2016-06-16 | 2017-12-21 | 新日鐵住金株式会社 | Bidirectional electrical steel sheet and manufacturing method thereof |
| JP2017222911A (en) * | 2016-06-16 | 2017-12-21 | 新日鐵住金株式会社 | Iron core, cold re-rolled steel sheet, cold re-rolled steel sheet manufacturing method, and iron core manufacturing method |
| CN120060725A (en) * | 2025-04-28 | 2025-05-30 | 太原科技大学 | Double-oriented silicon steel and preparation method thereof |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0733547B2 (en) | 1995-04-12 |
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