JP2000219916A - Manufacturing method of non-oriented electrical steel sheet with high magnetic flux density and low iron loss - Google Patents

Manufacturing method of non-oriented electrical steel sheet with high magnetic flux density and low iron loss

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Publication number
JP2000219916A
JP2000219916A JP2027599A JP2027599A JP2000219916A JP 2000219916 A JP2000219916 A JP 2000219916A JP 2027599 A JP2027599 A JP 2027599A JP 2027599 A JP2027599 A JP 2027599A JP 2000219916 A JP2000219916 A JP 2000219916A
Authority
JP
Japan
Prior art keywords
hot
oriented electrical
iron loss
electrical steel
steel sheet
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
JP2027599A
Other languages
Japanese (ja)
Inventor
Ryutaro Kawamata
竜太郎 川又
Takeshi Kubota
猛 久保田
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
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Filing date
Publication date
Application filed by Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP2027599A priority Critical patent/JP2000219916A/en
Publication of JP2000219916A publication Critical patent/JP2000219916A/en
Withdrawn legal-status Critical Current

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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P10/00Technologies related to metal processing
    • Y02P10/20Recycling

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  • Manufacturing Of Steel Electrode Plates (AREA)
  • Soft Magnetic Materials (AREA)

Abstract

(57)【要約】 【課題】 安定して低鉄損の無方向性電磁鋼板を製造法
を製造する。 【解決手段】 重量%で、0.1%≦Si≦2.5%、0.1%≦Mn≦
1.5%、C ≦0.004%、N ≦0.002%、S ≦0.002%、Ti≦0.00
3%、Nb≦0.003%、V ≦0.005%、Zr≦0.003%、Ca≦0.003
%、As≦0.003%、Cr≦0.05% 、Sn≦0.01% 、Cu≦0.05%
、O ≦0.02% を含有し、残部がFeおよび不可避的不純
物からなり、Q値が-4.70 以下でαγ変態を有するスラ
ブを熱間圧延して熱延板とし、次いで1回の冷間圧延工
程を施した後、仕上焼鈍を施し、その後にスキンパス圧
延工程を施すか或いは施さない無方向性電磁鋼板の製造
方法であって、熱延仕上温度をAr3 点以上とすること
を特徴とする磁束密度が高く鉄損の低い無方向性電磁鋼
板の製造法。
(57) [Problem] To provide a method for producing a non-oriented electrical steel sheet having stable and low iron loss. SOLUTION: In weight%, 0.1% ≦ Si ≦ 2.5%, 0.1% ≦ Mn ≦
1.5%, C ≤ 0.004%, N ≤ 0.002%, S ≤ 0.002%, Ti ≤ 0.00
3%, Nb ≦ 0.003%, V ≦ 0.005%, Zr ≦ 0.003%, Ca ≦ 0.003
%, As ≦ 0.003%, Cr ≦ 0.05%, Sn ≦ 0.01%, Cu ≦ 0.05%
, O ≤ 0.02%, the balance consisting of Fe and unavoidable impurities, having a Q value of -4.70 or less and having an αγ transformation, is hot-rolled into a hot-rolled sheet, and then subjected to one cold rolling step. , A method of manufacturing a non-oriented electrical steel sheet which is subjected to finish annealing and then subjected to a skin pass rolling step or not to be applied, wherein the hot-rolling finishing temperature is Ar 3 points or more. A method for producing non-oriented electrical steel sheets with high density and low iron loss.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、電気機器の鉄心材
料として用いられる、磁束密度が高く、鉄損が低い優れ
た磁気特性を有する無方向性電磁鋼板の製造方法に関す
るものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for producing a non-oriented electrical steel sheet having excellent magnetic properties with high magnetic flux density and low iron loss, which is used as an iron core material of electric equipment.

【0002】[0002]

【従来の技術】近年、電気機器、特に無方向性電磁鋼板
がその鉄心材料として使用される回転機および中、小型
変圧器等の分野においては、世界的な電力、エネルギー
節減、さらにはフロンガス規制等の地球環境保全の動き
の中で、高効率化の動きが急速に広まりつつある。この
ため、無方向性電磁鋼板に対しても、その特性向上、す
なわち、高磁束密度かつ低鉄損化への要請がますます強
まってきている。ところで、無方向性電磁鋼板において
は、従来、低鉄損化の手段として一般に、電気抵抗増大
による渦電流損低減の観点からSiあるいはAl等の含
有量を高める方法がとられてきた。しかし、この方法で
は反面、磁束密度の低下は避け得ないという問題点があ
った。このような問題点の克服のために、熱延板結晶粒
径を粗大化することで磁束密度と鉄損の両方を改善させ
る方法が行われてきた。従来、変態を有する無方向性電
磁鋼板においては、α域の上限付近において熱延を終了
することにより冷延前結晶粒径を確保し、結果として成
品の磁束密度、鉄損を向上させることが行われてきた。
このような観点から、特開昭56−38420号公報に
は熱延仕上温度をAr3 点とAr1 点の中間温度以下と
して680℃以上の温度で巻き取ることにより熱延結晶
組織の粗大化を図る方法が開示されている。しかしなが
ら、熱延仕上温度がγ域に上昇することは、熱延終了後
にα相への変態が進行することから熱延組織が細粒化
し、結果として磁気特性が悪化するため、避けるべき事
とされてきた。
2. Description of the Related Art In recent years, in the fields of electric machines, especially rotating machines and medium-sized and small-sized transformers in which non-oriented electrical steel sheets are used as iron core materials, worldwide electric power and energy savings, as well as chlorofluorocarbon gas regulations. Among the movements for global environmental conservation, such as the above, the movement for higher efficiency is rapidly spreading. Therefore, there is an increasing demand for non-oriented electrical steel sheets to have improved properties, that is, high magnetic flux density and low iron loss. By the way, in the non-oriented electrical steel sheet, conventionally, as a means of reducing iron loss, a method of increasing the content of Si or Al or the like has been generally adopted from the viewpoint of reducing eddy current loss due to an increase in electric resistance. However, this method has a problem that the magnetic flux density cannot be reduced. In order to overcome such problems, a method of improving both magnetic flux density and iron loss by increasing the crystal grain size of a hot-rolled sheet has been performed. Conventionally, in a non-oriented electrical steel sheet having a transformation, it is possible to secure the crystal grain size before cold rolling by terminating hot rolling near the upper limit of the α region, and as a result, improve the magnetic flux density and iron loss of the product. Has been done.
From this point of view, JP-A-56-38420 discloses that the hot-rolled crystal structure is coarsened by winding at a temperature of 680 ° C. or more with the hot-rolling finishing temperature being lower than the intermediate temperature between the Ar 3 point and the Ar 1 point. Is disclosed. However, the fact that the hot-rolling finishing temperature rises to the γ region is to be avoided because the hot-rolled structure becomes finer due to the progression of transformation to the α-phase after the end of hot-rolling, and as a result the magnetic properties deteriorate. It has been.

【0003】一方、実際の仕上熱延機においては、噛み
込み時の圧延速度と定常圧延状態の圧延速度が必然的に
異なることから、コイル長手方向の温度分布を解消する
ことが困難であり、α域の上限にて熱延を実施するため
には、圧延設定温度を低くせざるを得ないという不利益
があった。また、一般的な無方向性電磁鋼板の低級品で
はそのAr1 変態点が860℃付近であることから、熱
延仕上温度を上昇させて熱延結晶組織の成長を図ること
に限度があり、冷延前結晶組織の増大による磁気特性の
向上には限界があった。
On the other hand, in an actual finishing hot rolling mill, it is difficult to eliminate the temperature distribution in the longitudinal direction of the coil because the rolling speed during biting and the rolling speed in a steady rolling state are necessarily different. In order to perform hot rolling at the upper limit of the α region, there is a disadvantage that the set rolling temperature must be lowered. In addition, since the Ar 1 transformation point of a general low-grade non-oriented electrical steel sheet is around 860 ° C., there is a limit to increasing the hot-rolling finishing temperature to grow the hot-rolled crystal structure, There is a limit to the improvement of the magnetic properties due to the increase of the crystal structure before cold rolling.

【0004】このような制御熱延による冷延前結晶組織
粗大化の限界を打破する技術として、特開昭57−35
628号公報には熱延仕上温度をAr3 点以上として熱
延結晶組織の細粒化を図った上でA3 点以下の温度で熱
延板焼鈍を施し、冷延前結晶組織の粗大化を図る方法が
開示されている。また、熱延板焼鈍工程追加によるコス
トアップ上昇を抑え、冷延前結晶組織の粗大化を図る手
法として、高温で熱延板を巻取り、これをコイルの保有
熱で焼鈍する自己焼鈍法が特開昭54−76422号公
報、特開昭58−136718号公報に開示されてい
る。
As a technique for overcoming the limit of the coarsening of the crystal structure before cold rolling by such controlled hot rolling, Japanese Patent Laid-Open Publication No. Sho 57-35 discloses a technique.
No. 628 discloses that the hot-rolled crystal structure is refined by setting the hot-rolling finishing temperature to 3 points or more, and then the hot-rolled sheet is annealed at a temperature of 3 points or less to coarsen the crystal structure before cold rolling. Is disclosed. In addition, a self-annealing method, in which a hot-rolled sheet is wound at a high temperature and then annealed with the heat retained in the coil, is used as a method of suppressing the increase in cost due to the addition of the hot-rolled sheet annealing step and coarsening the crystal structure before cold rolling. It is disclosed in JP-A-54-76422 and JP-A-58-136718.

【0005】しかしながら熱延板焼鈍工程を追加するこ
とは製造コストの増加を招くため好ましくなく、変態を
有するローグレード無方向性電磁鋼板においては実際に
は殆ど実施されていない。また、自己焼鈍法においては
コイルを高温で巻き取ることによるコイル内温度不均一
によるコイル長手方向の磁気特性の変動が問題であっ
た。
[0005] However, the addition of a hot-rolled sheet annealing step is not preferable because it causes an increase in production cost, and is not practically carried out in a low-grade non-oriented electrical steel sheet having a transformation. Further, in the self-annealing method, there is a problem in that the magnetic characteristics in the longitudinal direction of the coil vary due to uneven temperature in the coil caused by winding the coil at a high temperature.

【0006】一方で、鉄損低減の為に、単にSiあるい
はAl等の含有量を高めるのみではなく、特公平6−8
0169号公報に記載されているように、Mn及びSの
低減による高純度鋼化により析出物の無害化を図る方法
が開示されている。しかしながら鋼の高純化のみでは上
述のごとき制御熱延による冷延前結晶組織粗大化の限界
を打破することが出来ず、高磁束密度化には限界があっ
た。
On the other hand, in order to reduce iron loss, it is necessary to not only increase the content of Si, Al, etc.
As described in Japanese Patent No. 0169, there is disclosed a method for making precipitates harmless by using high-purity steel by reducing Mn and S. However, pure purification of steel alone cannot overcome the above-mentioned limit of coarsening of the crystal structure before cold rolling by controlled hot rolling, and there is a limit to high magnetic flux density.

【0007】一次再結晶集合組織を改善することで無方
向性電磁鋼板の磁気特性を改善する方法として、特開昭
55−158252号公報のごとくSn添加、特開昭6
2−180014号公報のごときSn、Cu添加、もし
くは特開昭59−100217号公報のごときSb添加
による集合組織の改善による磁気特性の優れた無方向性
電磁鋼板の製造法が開示されているが、集合組織制御元
素であるSn, CuもしくはSb等の添加コストは決し
て低いものではなく、低コストな無方向性電磁鋼板の製
造法の提供には限界があった。また、特開昭57−35
626号公報に記載されているような仕上げ焼鈍サイク
ルの工夫等の製造プロセス上の処置もなされてきたが、
いずれも低鉄損化は図られても、磁束密度についてはそ
れほどの効果はなかった。
As a method for improving the magnetic properties of a non-oriented electrical steel sheet by improving the primary recrystallized texture, Sn is added as disclosed in JP-A-55-158252.
There is disclosed a method for producing a non-oriented electrical steel sheet having excellent magnetic properties by improving the texture by adding Sn and Cu as disclosed in Japanese Patent Application Publication No. 2-180014 or adding Sb as disclosed in Japanese Patent Application Laid-Open No. 59-100217. The cost of adding Sn, Cu or Sb, which is a texture control element, is not low at all, and there is a limit in providing a low-cost method for producing a non-oriented electrical steel sheet. Also, Japanese Patent Application Laid-Open No. 57-35
Although measures have been taken in the manufacturing process, such as devising a finish annealing cycle as described in Japanese Patent No. 626,
In each case, although the iron loss was reduced, the effect on the magnetic flux density was not so significant.

【0008】この様な従来技術の限界を打破するために
発明者等は特開平9−125144号公報において、不
純物元素の低減をはかるとともに仕上熱延をAr3 点以
上のγ相域とし、高温で巻取る事で低コストで高磁束密
度で低鉄損な無方向性電磁鋼板を製造する方法を開示し
た。
In order to overcome the limitations of the prior art, the inventors of the present invention disclosed in Japanese Patent Application Laid-Open No. Hei 9-125144 to reduce impurity elements and set the hot-rolled finish to a γ-phase region of 3 points or more of Ar, A method for manufacturing a non-oriented electrical steel sheet having a low cost, a high magnetic flux density and a low iron loss by winding at a low temperature has been disclosed.

【0009】しかしこれらの技術をもってしても、連続
して無方向性電磁鋼板の製鋼を行う際に、個々の条件は
満足しているにも関わらず、チャージ毎のバラツキが生
じやすく、安定して低鉄損の無方向性電磁鋼板を得る観
点からは若干の課題を残していた。
[0009] However, even with these techniques, when continuously producing non-oriented electrical steel sheets, even though the individual conditions are satisfied, variations are likely to occur for each charge, resulting in a stable operation. From the viewpoint of obtaining non-oriented electrical steel sheets with low iron loss, some problems remain.

【0010】このように、従来技術では、磁束密度が高
くかつ鉄損が低い無方向性電磁鋼板を製造できるには至
らず、無方向性電磁鋼板に対する前記の要請に応えるこ
とは出来なかった。発明者等はこの限界を克服すべく、
詳細に解析を行った結果、有害元素の総量と炭素との積
が一定以下であれば安定して低鉄損の無方向性電磁鋼板
を製造しうるという、新規な知見を見出した。
[0010] As described above, according to the prior art, it has not been possible to produce a non-oriented electrical steel sheet having a high magnetic flux density and a low iron loss, and it has not been possible to meet the above demand for a non-oriented electrical steel sheet. The inventors have tried to overcome this limitation
As a result of detailed analysis, a new finding was found that if the product of the total amount of harmful elements and carbon is equal to or less than a certain value, a non-oriented electrical steel sheet with low iron loss can be stably manufactured.

【0011】[0011]

【発明が解決しようとする課題】本発明は、従来技術に
おけるこのような問題点を解決し、高磁束密度かつ低鉄
損の無方向性電磁鋼板を提供することを目的とするもの
である。
SUMMARY OF THE INVENTION An object of the present invention is to solve such problems in the prior art and to provide a non-oriented electrical steel sheet having a high magnetic flux density and a low iron loss.

【0012】[0012]

【課題を解決するための手段】本発明の要旨とするとこ
ろは、以下の通りである。 (1) 重量%で、 0.1%≦Si≦3.5%、 0.1%≦Mn≦1.5%、 C ≦0.004%、 N ≦0.002%、 S ≦0.002%、 Ti≦0.003%、 Nb≦0.003%、 V ≦0.005%、 Zr≦0.003%、 Ca≦0.003%、 As≦0.003%、 Cr≦0.05%、 Sn≦0.01%、 Cu≦0.05%、 O ≦0.02% を含有し、残部がFeおよび不可避的不純物からなり、
式(1)で定めるQ値が−4.70以下でαγ変態を有
するスラブを熱間圧延して熱延板とし、次いで1回の冷
間圧延工程を施した後、仕上焼鈍を施し、その後にスキ
ンパス圧延工程を施すか或いは施さない無方向性電磁鋼
板の製造方法であって、熱延仕上温度をAr3 点以上と
することを特徴とする磁束密度が高く鉄損の低い無方向
性電磁鋼板の製造法。 Q=log[([Ti%]+[Nb%]+[V%]+[Zr%]+[Ca%]) ×[C%]] ・・・式(1) 但し、[Ti%] 、[Nb%] 、[V%]、[Zr%] 、[C%]、[Ca%]
は、それぞれTi、Nb、V、Zr、Ca、Cの成品中
の重量濃度 (2) スラブが、更に重量%で、 0.1%≦Al≦2% を含有することを特徴とする前記(1)記載の磁束密度
が高く鉄損の低い無方向性電磁鋼板の製造法。 (3) 仕上熱延後の熱延板を680℃以上の温度で巻
き取ることを特徴とする前記(1)又は(2)記載の磁
束密度が高く鉄損の低い無方向性電磁鋼板の製造法。
The gist of the present invention is as follows. (1) By weight%, 0.1% ≦ Si ≦ 3.5%, 0.1% ≦ Mn ≦ 1.5%, C ≦ 0.004%, N ≦ 0.002%, S ≦ 0.002 %, Ti ≦ 0.003%, Nb ≦ 0.003%, V ≦ 0.005%, Zr ≦ 0.003%, Ca ≦ 0.003%, As ≦ 0.003%, Cr ≦ 0.05% , Sn ≦ 0.01%, Cu ≦ 0.05%, O ≦ 0.02%, the balance being Fe and unavoidable impurities,
A slab having a α-γ transformation with a Q value determined by the formula (1) of -4.70 or less is hot-rolled into a hot-rolled sheet, then subjected to one cold rolling step, and then subjected to finish annealing, and thereafter A method for producing a non-oriented electrical steel sheet which is subjected to a skin pass rolling step or not, wherein a hot-rolling finishing temperature is set to 3 points or more, wherein the magnetic flux density is high and the iron loss is low. Steel sheet manufacturing method. Q = log [([Ti%] + [Nb%] + [V%] + [Zr%] + [Ca%]) × [C%]] Equation (1) where [Ti%], [Nb%], [V%], [Zr%], [C%], [Ca%]
(2) The weight concentration of Ti, Nb, V, Zr, Ca, and C in a product, respectively. (2) The slab further contains 0.1% ≦ Al ≦ 2% by weight. 1) A method for producing a non-oriented electrical steel sheet having a high magnetic flux density and a low iron loss as described above. (3) The production of a non-oriented electrical steel sheet having a high magnetic flux density and a low iron loss according to the above (1) or (2), wherein the hot-rolled sheet after the finish hot-rolling is wound at a temperature of 680 ° C. or more. Law.

【0013】[0013]

【発明の実施の形態】以下に、本発明を詳細に説明す
る。発明者らは、低鉄損と高磁束密度を同時に達成すべ
く従来技術における問題点を鋭意検討を重ねた結果、変
態を有する無方向性電磁鋼板にあって、無方向性電磁鋼
板において、Siを0.1%〜3.5%、Alを0.1
%〜2%、Mnを0.1%〜1.5%含有する鋼にあっ
て、C、S、N、Cr、Sn、Cu、O含有量を低減
し、さらに、Ti、V、Nb、Ca、Zr、As含有量
を特定の関係式を満たした上で低減し、高純度鋼化する
とともに、C含有量を同時に低減し、これをAr3 点以
上の温度で仕上げ熱延を終了し、高温で巻取る事によ
り、一回の冷間圧延で最終板厚とし焼鈍を施すフルプロ
セス無方向性電磁鋼板、あるいは中間焼鈍をはさむ二回
以上の冷間圧延により最終板厚とする無方向性電磁鋼板
製造法において磁束密度が高く、鉄損の低い無方向性電
磁鋼板を製造することが可能であることを見出し発明に
至った。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below in detail. The present inventors have conducted intensive studies on the problems in the prior art in order to simultaneously achieve a low iron loss and a high magnetic flux density, and as a result, in a non-oriented electrical steel sheet having a transformation, 0.1% to 3.5%, and 0.1% Al
% To 2% and Mn of 0.1% to 1.5%, the content of C, S, N, Cr, Sn, Cu, O is reduced, and further, Ti, V, Nb, Ca, Zr, reduced while satisfying the As content specific relationship, as well as high purity steel of, reducing the C content at the same time, which the finishing hot-rolled end with Ar 3 point or more temperature Full-process non-oriented electrical steel sheet that is annealed at the final thickness by one cold rolling by winding at high temperature, or non-oriented to the final thickness by two or more cold rollings with intermediate annealing The present inventors have found that it is possible to produce a non-oriented electrical steel sheet having a high magnetic flux density and a low iron loss in a method for producing a magnetic electrical steel sheet.

【0014】無方向性電磁鋼板の磁気特性は冷延前結晶
組織を粗大化することで改善することが可能である。こ
のため従来、仕上熱延において熱延仕上温度を上昇させ
て熱延組織の粗大化を図り、製品の磁束密度を高め、鉄
損を低減させることが行われてきた。しかしながら熱延
仕上温度を上昇させてα+γ2相域もしくはγ域に達す
ると、熱延終了後にγ相からα相への変態が進行するこ
とから熱延組織が細粒化し、結果として磁気特性が悪化
するため、避けるべき事とされてきた。このため、αγ
変態を有する無方向性電磁鋼板ではα域の上限にて熱延
を実施することが必須であるとされてきたが、Si含有
量の少ない無方向性電磁鋼板の低級品ではそのAr1
態点が900℃以下であることから、熱延仕上温度の上
昇による熱延結晶組織の粗大化には限度があり、結果と
して磁気特性の向上には限界があった。
The magnetic properties of the non-oriented electrical steel sheet can be improved by enlarging the crystal structure before cold rolling. For this reason, conventionally, in hot-rolling finishing, the hot-rolling finishing temperature has been increased to increase the size of the hot-rolled structure, increase the magnetic flux density of the product, and reduce iron loss. However, when the hot rolling finish temperature is increased to reach the α + γ2 phase region or the γ region, the transformation from the γ phase to the α phase proceeds after the end of the hot rolling, so that the hot rolled structure becomes finer and the magnetic properties deteriorate as a result. To be avoided. Therefore, αγ
It has been considered that it is essential to perform hot rolling at the upper limit of the α range for non-oriented electrical steel sheets having a transformation, but for low-grade non-oriented electrical steel sheets having a low Si content, the Ar 1 transformation point Is 900 ° C. or less, there is a limit to the coarsening of the hot-rolled crystal structure due to an increase in the hot-rolling finishing temperature, and as a result, there is a limit to the improvement of the magnetic properties.

【0015】発明者等は従来のこのような変態を有する
無方向性電磁鋼板の制御熱延の限界を打破すべく鋭意検
討を進めた結果、変態を有する無方向性電磁鋼板にあっ
て、Siを0.1%〜3.5%、Alを0.1%〜2
%、Mnを0.1%〜1.5%含有しαγ変態を有する
鋼にあって、C、S、N、Cr、Cu、Sn、O含有量
を低減し、さらに、Ti、V、Nb、Ca、Zr、As
含有量を特定の式を満たしつつ同時に低減することによ
り高純度鋼化すれば、熱延仕上温度をγ域まで高めても
変態後のα相の結晶組織が細粒化せず、熱延仕上温度の
上昇に伴って熱延結晶組織が粗大化するとともに、発明
者等が特開平9−125144号公報において開示した
技術の問題点であるチャージ毎のバラツキを解消し、安
定して高磁束密度低鉄損の無方向性電磁鋼板を得ること
が可能となった。
The present inventors have conducted intensive studies to overcome the limitations of the conventional hot-rolled non-oriented electrical steel sheet having such a transformation. 0.1% to 3.5%, Al 0.1% to 2%
%, Mn containing 0.1% to 1.5% and having αγ transformation, C, S, N, Cr, Cu, Sn, O content is reduced, and further, Ti, V, Nb , Ca, Zr, As
If the steel is made of high purity by simultaneously reducing the content while satisfying the specific formula, the crystal structure of the α phase after transformation will not be refined even if the hot rolling finish temperature is raised to the γ range, and the hot rolled finish As the temperature rises, the hot-rolled crystal structure becomes coarser, and the present inventors have solved the problem of the technology disclosed in Japanese Patent Application Laid-Open No. 9-125144. It has become possible to obtain non-oriented electrical steel sheets with low iron loss.

【0016】このような方法により得られた熱延板を出
発材とすることにより、仕上げ焼鈍後の製品における磁
束密度が高く、鉄損が良好な(鉄損値が低い)無方向性
電磁鋼板を安価に製造することに成功した。
By using the hot-rolled sheet obtained by such a method as a starting material, a non-oriented electrical steel sheet having a high magnetic flux density and a good iron loss (low iron loss value) in a product after finish annealing. Was successfully manufactured at low cost.

【0017】まず、成分について説明すると、Siは鋼
板の固有抵抗を増大させ渦流損を低減させ、鉄損値を改
善するために添加される。Si含有量が0.1%未満で
あると固有抵抗が十分に得られないので0.1%以上添
加する必要がある。一方、Si含有量が3.5%を越え
ると冷間圧延が困難となるので3.5%以下に定める。
First, the components will be described. Si is added to increase the specific resistance of the steel sheet, reduce the eddy current loss, and improve the iron loss value. If the Si content is less than 0.1%, sufficient resistivity cannot be obtained, so it is necessary to add 0.1% or more. On the other hand, if the Si content exceeds 3.5%, cold rolling becomes difficult, so the content is set to 3.5% or less.

【0018】Mnは、Siと同様に鋼板の固有抵抗を増
大させ渦電流損を低減させる効果を有する。このため、
Mn含有量は0.1%以上とする必要がある。一方、M
n含有量が1.5%を越えると熱延時の変形抵抗が増加
し熱延が困難となるとともに、冷延前結晶組織が微細化
しやすくなり、製品の磁気特性が悪化するので、Mn含
有量は1.5%以下とする必要がある。
Mn, like Si, has the effect of increasing the specific resistance of the steel sheet and reducing eddy current loss. For this reason,
The Mn content needs to be 0.1% or more. On the other hand, M
If the n content exceeds 1.5%, the deformation resistance during hot rolling increases and hot rolling becomes difficult, and the crystal structure before cold rolling tends to be finer, which deteriorates the magnetic properties of the product. Needs to be 1.5% or less.

【0019】鋼中のAlは不純物レベルであってもなん
ら問題はないが、AlはSiと同様に鋼板の固有抵抗を
増大させ渦電流損を低減させる効果を有するので、特に
低鉄損を得たい場合には0.1%以上2%以下添加する
のが好ましい。多量にAl添加した場合には、磁束密度
が低下し、コスト高ともなるので2%以下とする。
Although there is no problem even if Al in the steel is at the impurity level, Al has the effect of increasing the specific resistance of the steel sheet and reducing the eddy current loss as in the case of Si. If desired, it is preferable to add 0.1% or more and 2% or less. If a large amount of Al is added, the magnetic flux density decreases and the cost increases, so the content is set to 2% or less.

【0020】また、製品の機械的特性の向上、磁気的特
性、耐錆性の向上あるいはその他の目的のために、P、
B、Ni、Sbの1種または2種以上を鋼中に含有させ
ても本発明の効果は損なわれない。
In order to improve the mechanical properties, magnetic properties, and rust resistance of the product or for other purposes, P,
Even if one or more of B, Ni and Sb are contained in steel, the effect of the present invention is not impaired.

【0021】C含有量は、0.004%以下に制御する
ことが必要である。C含有量が0.004%を越える
と、成品の使用中に磁気時効が生じて鉄損が悪化するの
みならず、不純物元素と炭化物を生成して仕上げ焼鈍時
の結晶粒成長を阻害し、ひいては鉄損の悪化をもたらす
ので0.004%以下とする必要がある。
It is necessary to control the C content to 0.004% or less. If the C content exceeds 0.004%, not only magnetic aging occurs during the use of the product, iron loss is deteriorated, but also impurity elements and carbides are generated to inhibit crystal grain growth during finish annealing, As a result, iron loss deteriorates, so it is necessary to set the content to 0.004% or less.

【0022】S、Nは熱間圧延工程におけるスラブ加熱
中に一部再固溶し、熱間圧延中にMnS等の硫化物、A
lN等の窒化物を形成する。これらが存在することによ
り熱延後のγ相からα相への変態時にα相の核を提供す
ると共に変態後のα相結晶組織の粒成長を妨げるためそ
の含有量は共に0.002%以下とする必要がある。
S and N partially re-dissolve during the slab heating in the hot rolling step, and sulfides such as MnS and A
A nitride such as 1N is formed. The presence thereof provides the nucleus of the α phase during transformation from the γ phase to the α phase after hot rolling and hinders the grain growth of the α phase crystal structure after the transformation. It is necessary to

【0023】また、Ti含有量、V含有量、Nb含有
量、Zr含有量、Ca含有量、Cr含有量がそれぞれ
0.003%、0.005%、0.003%、0.00
3%、0.003%、0.05%を越えるとTi、V、
Nb、Zr、Ca、Crの炭化物の析出が顕著となり、
熱延結晶組織の粗大化が阻害されるとともに仕上焼鈍工
程での結晶粒成長が阻害され磁気特性が悪化する。この
ため、Ti含有量、V含有量、Nb含有量、Zr含有
量、Ca含有量、Cr含有量はそれぞれ0.003%以
下、0.005%以下、0.003%以下、0.003
以下%、0.003%、0.05%以下とする必要があ
る。
The Ti content, V content, Nb content, Zr content, Ca content and Cr content are 0.003%, 0.005%, 0.003% and 0.003%, respectively.
If it exceeds 3%, 0.003% or 0.05%, Ti, V,
Precipitation of carbides of Nb, Zr, Ca, Cr becomes remarkable,
The coarsening of the hot-rolled crystal structure is hindered, and the crystal grain growth in the finish annealing step is hindered, deteriorating the magnetic properties. Therefore, the Ti content, V content, Nb content, Zr content, Ca content, and Cr content are 0.003% or less, 0.005% or less, 0.003% or less, and 0.003% or less, respectively.
%, 0.003%, and 0.05% or less.

【0024】また、本発明では個々のTi、V、Nb、
Zr、Ca単独の含有量に加えて、全体を含めた総量
と、C含有量との間に特定の関係が成立する必要があ
る。すなわち、式(1)で定めるQ値において、 Q=log[([Ti%]+[Nb%]+[V%]+[Zr%]+[Ca%]) ×[C%]] ・・・式(1) 但し、[Ti%] 、[Nb%] 、[V%]、[Zr%] 、[C%]、[Ca%]
は、それぞれTi、Nb、V、Zr、Ca、Cの成品中
の重量濃度 式(1)のQ値が−4.70を超えると本発明が意図す
る低鉄損無方向性電磁鋼板を得ることが出来ない。従っ
て、式(1)のQ値は−4.70以下である必要があ
る。
In the present invention, each of Ti, V, Nb,
In addition to the content of Zr and Ca alone, a specific relationship needs to be established between the total amount including the entirety and the C content. That is, at the Q value determined by the equation (1), Q = log [([Ti%] + [Nb%] + [V%] + [Zr%] + [Ca%]) × [C%]] Equation (1) where [Ti%], [Nb%], [V%], [Zr%], [C%], [Ca%]
Is a weight concentration in a product of Ti, Nb, V, Zr, Ca, and C respectively. When the Q value of the formula (1) exceeds -4.70, a low iron loss non-oriented electrical steel sheet intended by the present invention is obtained. I can't do that. Therefore, the Q value in equation (1) needs to be -4.70 or less.

【0025】さらに、結晶粒成長を阻害する析出物の形
成に影響を及ぼす要因として、As含有量を抑制する必
要がある。Asは、それ自体では、本発明の成分範囲内
の鋼では、上記の硫化物や窒化物等の析出物を形成する
ことは無い。しかし、鋼中に、一定量以上のAsが含有
されると、硫化物サイズが微細になるため、熱延結晶組
織の粗大化を著しく阻害する。このような観点から、A
s含有量は0.003%以下にする必要がある。
Further, as a factor affecting the formation of precipitates that hinder crystal grain growth, it is necessary to suppress the As content. As itself does not form the above-mentioned precipitates such as sulfides and nitrides in steel within the composition range of the present invention. However, if a certain amount or more of As is contained in the steel, the sulfide size becomes fine, so that the coarsening of the hot-rolled crystal structure is significantly inhibited. From such a viewpoint, A
The s content needs to be 0.003% or less.

【0026】Sn、Cuは鋼の結晶粒界に偏析して粒成
長を妨げ、成品鉄損を悪化させるので、それぞれ含有量
は0.01%以下、0.05%以下とする必要がある。
Since Sn and Cu segregate at the crystal grain boundaries of the steel to hinder grain growth and worsen the iron loss of the product, their contents must be 0.01% or less and 0.05% or less, respectively.

【0027】O含有量が0.02%を超えるとSi
2 、Al2 3 等の酸化物系介在物の析出が顕著とな
り。結晶粒成長を妨げ、成品鉄損を悪化させるので、含
有量は0.02%以下とする必要がある。
If the O content exceeds 0.02%, Si
Precipitation of oxide inclusions such as O 2 and Al 2 O 3 becomes remarkable. The content needs to be 0.02% or less because it hinders crystal grain growth and worsens the iron loss of the product.

【0028】Pは、製品の打ち抜き性を良好ならしめる
ために0.1%までの範囲内において添加される。P≦
0.2%であれば、製品の磁気特性の観点から問題がな
い。
P is added in a range of up to 0.1% in order to improve the punchability of the product. P ≦
If it is 0.2%, there is no problem from the viewpoint of the magnetic properties of the product.

【0029】Bは熱間圧延時にBNを形成させてAlN
の微細析出を妨げ、Nを無害化させるために添加され
る。B含有量はNとの量のバランスが必要であり、その
含有量は両者の比B% /N% が0.5から1.5の範囲
を満たすことが好ましい。
B forms AlN by forming BN during hot rolling.
Is added to prevent fine precipitation of N and render N harmless. The B content needs to be balanced with the amount of N, and the content is preferably such that the ratio B% / N% of both satisfies the range of 0.5 to 1.5.

【0030】Ni、Sbは成品の一次再結晶集合組織を
改善して特に磁束密度を向上させる効果がある。この目
的のために添加する場合、Niは0.2以上2.5%以
下、Sbは0.05%以上0.5%以下の範囲を満たす
ことが好ましい。
Ni and Sb have the effect of improving the primary recrystallization texture of the product and, in particular, improving the magnetic flux density. When added for this purpose, Ni preferably satisfies the range of 0.2 to 2.5%, and Sb preferably satisfies the range of 0.05% to 0.5%.

【0031】次に本発明の成分範囲規定理由について説
明する。発明者らは鋭意検討を重ねた結果、C、N、
S、Cr、Cu、Sn、Oに加えTi、V、Nb、Z
r、As、Ca等の不純物含有量を総合的に制御するこ
とにより、製品における鉄損が著しく改善され得ること
を発見し本発明の完成に至った。
Next, the reasons for defining the component range of the present invention will be described. The inventors have conducted intensive studies and found that C, N,
Ti, V, Nb, Z in addition to S, Cr, Cu, Sn, O
It has been discovered that by comprehensively controlling the content of impurities such as r, As, and Ca, iron loss in products can be significantly improved, and the present invention has been completed.

【0032】本発明の構成要件を確認するために、以下
のような実験を行った。表1、表2に示す成分の鋼を溶
製し仕上げ熱延を実施し、2.5mm厚に仕上げた。この
際に、熱延仕上温度は960℃のγ相域とした。これを
700℃でコイルに巻きとった。 次に熱延板を酸洗、
冷延し0.5mm厚とし、脱脂した後、750℃、30秒
焼鈍しエプスタイン試料を切断して磁気特性を測定し
た。
The following experiments were conducted to confirm the requirements of the present invention. Steel having the components shown in Tables 1 and 2 was melted and subjected to finish hot rolling to finish to a thickness of 2.5 mm. At this time, the hot rolling finishing temperature was in a γ phase region of 960 ° C. This was wound around a coil at 700 ° C. Next, pickling the hot rolled sheet,
After cold rolling to a thickness of 0.5 mm, degreased, and then annealed at 750 ° C. for 30 seconds, the Epstein sample was cut and the magnetic properties were measured.

【0033】[0033]

【表1】 [Table 1]

【0034】[0034]

【表2】 [Table 2]

【0035】表1、表2において、比較例1から3にお
いてはQ値が本発明の構成要件である−4.70以下を
満たしておらず、また、比較例4ではAs含有量が本発
明の構成要件である0.003%以下を満たしていない
ため、本発明例よりも鉄損が悪化していることがわか
る。このように不純物元素を制御することにより、製品
における鉄損を低減し、優れた磁気特性の無方向性電磁
鋼板を製造することが可能である。
In Tables 1 and 2, in Comparative Examples 1 to 3, the Q value did not satisfy the constituent requirement of the present invention, ie, -4.70 or less. It does not satisfy the constituent requirement of 0.003% or less, so that the iron loss is worse than that of the present invention. By controlling the impurity elements in this way, it is possible to reduce iron loss in products and to manufacture non-oriented electrical steel sheets having excellent magnetic properties.

【0036】前記成分からなる鋼スラブは、転炉で溶製
され連続鋳造あるいは造塊−分塊圧延により製造され
る。鋼スラブは公知の方法にて加熱される。本発明では
熱延板は、一回の冷間圧延と連続焼鈍により製品とす
る。またさらにスキンパス圧延工程を付加して製品とし
てもよい。また、中間焼鈍をはさむ2回以上の冷間圧延
により最終板厚としても良い。さらに、その後スキンパ
スを施して最終板厚としても良い。スキンパス圧延率は
2%未満ではその効果が得られず、20%以上では磁気
特性が悪化するため2%から20%とする。
The steel slab composed of the above components is produced in a converter and is produced by continuous casting or ingot-bulking rolling. The steel slab is heated by a known method. In the present invention, the hot-rolled sheet is made into a product by one cold rolling and continuous annealing. Further, a skin pass rolling step may be added to obtain a product. Further, the final thickness may be obtained by performing cold rolling two or more times with intermediate annealing. Furthermore, a skin pass may be performed thereafter to obtain a final thickness. If the skin pass rolling ratio is less than 2%, the effect cannot be obtained, and if the skin pass rolling ratio is 20% or more, the magnetic properties are deteriorated.

【0037】次に本発明のプロセス条件について説明す
る。従来の技術においては熱延板すなわち冷延前の結晶
粒径を極力粗大化することに主眼がおかれており、熱延
後のγ相からα相への変態は熱延板の結晶粒を微細化す
るために有害であるとみなされ、熱延仕上温度をAr1
点以上に上昇させると熱延結晶組織はかえって細粒化す
るため、本発明のごとき熱延仕上温度をγ域へと高める
方法の利用は省みられなかった。しかし発明者らは鋭意
検討を重ねた結果、C、N、S、Cr、Cu、Sn、O
に加えTi、V、Nb、Ca、Zr、As等の不純物含
有量を式(1)で定義されるQ値を一定以下に満足した
上で低減することにより熱間圧延工程において仕上圧延
をAr3 以上で終了した場合においても熱延結晶組織が
粗大化され、結果として製品における磁気特性が著しく
改善され得ることを発見し本発明の完成に至った。
Next, the process conditions of the present invention will be described. In the prior art, the main focus has been on increasing the grain size of the hot-rolled sheet, that is, before cold rolling, as much as possible, and the transformation from γ phase to α phase after hot rolling It is considered harmful for miniaturization, and the hot rolling finish temperature is set to Ar 1
When the temperature is raised to more than the point, the hot-rolled crystal structure is rather fine-grained, so that the use of the method of raising the hot-rolling finishing temperature to the γ region as in the present invention was not omitted. However, as a result of intensive studies, the inventors found that C, N, S, Cr, Cu, Sn, O
In addition, by reducing the content of impurities such as Ti, V, Nb, Ca, Zr, and As while satisfying the Q value defined by the formula (1) below a certain value, the finish rolling in the hot rolling process can be performed by Ar. It was discovered that even when the treatment was completed at 3 or more, the hot-rolled crystal structure was coarsened, and as a result, the magnetic properties of the product could be significantly improved, and the present invention was completed.

【0038】このような鋼の純度による熱延条件に対す
る熱延結晶組織形成の相違を調べるため、以下のような
実験を行った。表3に示す成分の鋼を溶製し仕上げ熱延
を実施した。熱延仕上温度は800℃から1000℃の
範囲とし、2.5mm厚に仕上げた。これを酸洗、冷延し
0.5mm厚とし、脱脂した後、720℃、30秒焼鈍し
エプスタイン試料を切断して磁気特性を測定した。熱延
仕上げ温度に対する熱延板結晶粒径の変化、製品鉄損、
製品磁束密度をそれぞれ図1、図2、図3に示した。
The following experiment was conducted to examine the difference in the hot rolled crystal structure formation under the hot rolling conditions depending on the purity of the steel. Steels having the components shown in Table 3 were melted and subjected to finish hot rolling. The hot-rolling finishing temperature was in the range of 800 ° C. to 1000 ° C., and was finished to a thickness of 2.5 mm. This was pickled, cold rolled to a thickness of 0.5 mm, degreased, and annealed at 720 ° C. for 30 seconds to cut the Epstein sample and measure its magnetic properties. Change in hot-rolled sheet crystal grain size to hot-rolling finishing temperature, product iron loss,
The product magnetic flux densities are shown in FIGS. 1, 2 and 3, respectively.

【0039】[0039]

【表3】 [Table 3]

【0040】成分1の高純度鋼では熱延仕上げ温度がA
3 点以上になっても熱延結晶組織が粗大化するが、成
分2の比較材では個々の成分は式(1)以外の条件を満
足するが、式(1)で定義されるQ値が−4.70超と
なっており、熱延仕上げ温度がAr1 点以上になると熱
延結晶組織が細粒化する。この結果、成分1の高純度鋼
では熱延仕上温度が上昇するに従い鉄損は低下し、磁束
密度は向上するが、成分2の比較例では鉄損の増大、磁
束密度の低下といった磁気特性の悪化がみられる。
In the high purity steel of the component 1, the hot rolling finish temperature is A
Although the hot-rolled crystal structure is coarsened even at r 3 or more, each component in the comparative material of the component 2 satisfies the conditions other than the formula (1), but the Q value defined by the formula (1) Is higher than -4.70, and when the hot-rolling finishing temperature is equal to or higher than the Ar 1 point, the hot-rolled crystal structure becomes finer. As a result, in the high-purity steel of the component 1, the iron loss decreases and the magnetic flux density increases as the hot-rolling finishing temperature increases, but in the comparative example of the component 2, the magnetic properties such as the increase of the iron loss and the decrease of the magnetic flux density are increased. Deterioration is seen.

【0041】このようにC、N、S、Cr、Cu、S
n、Oに加えTi、V、Nb、Ca、Zr、As等の不
純物を低減するとともに式(1)で定義されるQ値を−
4.70以下に制御した上で、高純度鋼をAr3 点以上
の熱延仕上温度で仕上げることにより、製品における鉄
損を低減し、磁束密度の高め、優れた磁気特性の無方向
性電磁鋼板を製造することが可能である。
Thus, C, N, S, Cr, Cu, S
In addition to reducing impurities such as Ti, V, Nb, Ca, Zr and As in addition to n and O, the Q value defined by the equation (1) is reduced by-
High-purity steel is finished at a hot-rolling finishing temperature of at least three points of Ar under the control of 4.70 or less to reduce iron loss in products, increase magnetic flux density, and provide non-directional electromagnetic It is possible to manufacture steel sheets.

【0042】前記成分からなる鋼スラブは、転炉で溶製
され連続鋳造あるいは造塊−分塊圧延により製造され
る。鋼スラブは公知の方法にて加熱される。このスラブ
に熱間圧延を施し所定の厚みとする。この際、仕上げ熱
延の終了温度はAr3 点以上とする。巻取温度は680
℃以上であれば本発明における熱延結晶組織の粗大化を
一層促進することが可能である。
A steel slab composed of the above components is produced by melting in a converter and being manufactured by continuous casting or ingot-bulking rolling. The steel slab is heated by a known method. This slab is subjected to hot rolling to a predetermined thickness. At this time, the finishing temperature of the finish hot rolling is set to 3 points or more of Ar. Winding temperature is 680
When the temperature is at least ° C, the coarsening of the hot-rolled crystal structure in the present invention can be further promoted.

【0043】熱延仕上温度がAr3 点を下まわると、熱
延結晶組織の成長が不十分となり、本発明が目的とする
優れた磁気特性を有する無方向性電磁鋼板を得ることが
できない。このため熱延仕上温度はAr3 点以上である
ことが必要である。熱延仕上温度の上限は特に設けない
が、熱間圧延時のスラブ加熱温度の上限および熱間圧延
スケジュールにより必然的にその上限が決まる。
When the hot-rolling finishing temperature is lower than the Ar 3 point, the growth of the hot-rolled crystal structure becomes insufficient, and the non-oriented electrical steel sheet having excellent magnetic properties aimed at by the present invention cannot be obtained. For this reason, the hot rolling finishing temperature needs to be at least Ar 3 points. Although there is no particular upper limit on the hot rolling finish temperature, the upper limit is inevitably determined by the upper limit of the slab heating temperature during hot rolling and the hot rolling schedule.

【0044】また、巻取温度が680℃以下であると熱
延結晶組織の成長が不十分となり、優れた磁気特性を有
する無方向性電磁鋼板を得ることができない。このため
巻取温度は680℃以上、好ましくは700℃以上であ
ることが好ましい。
If the winding temperature is 680 ° C. or lower, the growth of the hot-rolled crystal structure becomes insufficient, and a non-oriented electrical steel sheet having excellent magnetic properties cannot be obtained. For this reason, the winding temperature is preferably at least 680 ° C, more preferably at least 700 ° C.

【0045】このようにして得られた熱延板は一回の冷
間圧延と連続焼鈍により製品とする。またさらにスキン
パス圧延工程を付加して製品としてもよい。スキンパス
圧延率は2%未満ではその効果が得られず、20%以上
では磁気特性が悪化するため2%から20%とする。
The hot rolled sheet obtained in this manner is made into a product by one cold rolling and continuous annealing. Further, a skin pass rolling step may be added to obtain a product. If the skin pass rolling ratio is less than 2%, the effect cannot be obtained, and if the skin pass rolling ratio is 20% or more, the magnetic properties are deteriorated.

【0046】[0046]

【実施例】次に、本発明の実施例について述べる。 [実施例1]表4に示した成分を有する無方向性電磁鋼
用スラブを通常の方法にて加熱し、熱延により2.5mm
に仕上げた。この時、熱延仕上げ温度は960℃とし、
すべてAr3 変態点以上のγ相域とした。熱延の巻取温
度は700℃とした。その後、酸洗を施し、冷間圧延に
より0.50mmに仕上げた。これを連続焼鈍炉にて73
0℃で30秒間焼鈍した。その後、エプスタイン試料に
切断し、磁気特性を測定した。表4中に本発明と比較例
の成分と鉄損測定結果をあわせて示す。
Next, an embodiment of the present invention will be described. [Example 1] A slab for non-oriented electrical steel having the components shown in Table 4 was heated by a usual method, and was hot-rolled to 2.5 mm.
Finished. At this time, the hot rolling finishing temperature is 960 ° C.
All were in the γ phase region at or above the Ar 3 transformation point. The winding temperature of hot rolling was 700 ° C. Then, it was pickled and finished to 0.50 mm by cold rolling. This is placed in a continuous annealing furnace 73
Annealed at 0 ° C. for 30 seconds. Thereafter, the sample was cut into Epstein samples, and the magnetic properties were measured. Table 4 also shows the components of the present invention and comparative examples and the results of iron loss measurement.

【0047】[0047]

【表4】 [Table 4]

【0048】比較例1はQ値の値が、比較例2はC含有
量が、比較例3はS含有量が、比較例4はTi含有量
が、比較例5はV含有量が、比較例6はNb含有量が、
比較例7はSとAs含有量が、比較例8はCr含有量
が、比較例9はSn含有量が、比較例10はCu含有量
が、比較例11はO含有量がそれぞれ本発明の構成要件
を満たしておらず、本発明の実施例に比べて磁束密度、
鉄損の値が劣っていることが分かる。
Comparative Example 1 had a Q value, Comparative Example 2 had a C content, Comparative Example 3 had an S content, Comparative Example 4 had a Ti content, Comparative Example 5 had a V content, Example 6 shows that the Nb content is
Comparative Example 7 has an S and As content, Comparative Example 8 has a Cr content, Comparative Example 9 has a Sn content, Comparative Example 10 has a Cu content, and Comparative Example 11 has an O content of the present invention. Does not meet the configuration requirements, compared to the embodiment of the present invention magnetic flux density,
It turns out that the value of iron loss is inferior.

【0049】このように鋼の純度を制御すれば、巻取り
温度をAr3 点以上にすることにより、磁束密度の値が
高く、鉄損値の低い磁気特性の優れた無方向性電磁鋼板
を得ることが可能である。
By controlling the purity of the steel as described above, the non-oriented electrical steel sheet having a high magnetic flux density and a low iron loss value and excellent magnetic properties can be obtained by setting the winding temperature to Ar 3 points or more. It is possible to get.

【0050】[実施例2]表5に示した成分の無方向性
電磁鋼用スラブを通常の方法にて加熱し、熱延により
2.5mmに仕上げた。この時、熱延仕上温度をAr3
以上の965℃と、Ar1 以下850℃の2水準とし、
冷却制御により巻取温度は700℃とした。
Example 2 A slab for non-oriented electromagnetic steel having the components shown in Table 5 was heated by a usual method and finished to 2.5 mm by hot rolling. At this time, the hot-rolling finishing temperature was set to two levels of 965 ° C. at 3 points or more of Ar and 850 ° C. at Ar 1 or less,
The winding temperature was set to 700 ° C. by cooling control.

【0051】その後、酸洗を施し、冷間圧延により0.
50mmおよび0.55mmに仕上げた。板厚0.50mmの
ものは連続焼鈍炉にて730℃で30秒間焼鈍した。そ
の後、750℃2時間の需要家相当の焼鈍を施した。ま
た、板厚0.55mmのものは、連続焼鈍炉にて700℃
で20秒焼鈍を施し、圧下率9%のスキンパス圧延によ
り0.50mm厚に仕上げ、750℃2時間の需要家相当
の焼鈍を施した。これらの試料からエプスタイン試験片
を切り出しの磁気特性を測定した。
After that, it is pickled and then cold-rolled to a thickness of 0.1 mm.
Finished to 50 mm and 0.55 mm. The sheet having a thickness of 0.50 mm was annealed in a continuous annealing furnace at 730 ° C. for 30 seconds. Thereafter, annealing was performed at 750 ° C. for 2 hours corresponding to a customer. In addition, the one with a sheet thickness of 0.55 mm is 700 ° C in a continuous annealing furnace.
At 750 ° C. for 2 hours, followed by annealing at 750 ° C. for 2 hours. From these samples, Epstein test pieces were cut out to measure the magnetic properties.

【0052】[0052]

【表5】 表6、表7に実施例中で述べた本発明と比較例の熱延仕
上げ温度、巻取り温度と磁気測定結果をあわせて示す。
[Table 5] Tables 6 and 7 also show the hot rolling finish temperature, winding temperature, and magnetic measurement results of the present invention and the comparative examples described in the examples.

【0053】[0053]

【表6】 [Table 6]

【0054】[0054]

【表7】 [Table 7]

【0055】このように高純度鋼を用い、熱延仕上温度
をAr3 点以上にとることにより、1回法、スキンパス
圧延法とも磁束密度の値が高く、鉄損値の低い材料が得
られることがわかる。
As described above, by using a high-purity steel and setting the hot-rolling finishing temperature to 3 points or more of Ar, a material having a high magnetic flux density and a low iron loss value can be obtained in both the single pass method and the skin pass rolling method. You can see that.

【0056】[0056]

【発明の効果】このように本願発明によれば、磁束密度
が高く鉄損の低い、磁気特性の優れた無方向性電磁鋼板
を製造することが可能である。
As described above, according to the present invention, it is possible to manufacture a non-oriented electrical steel sheet having high magnetic flux density and low iron loss and excellent in magnetic properties.

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

【図1】本発明における熱延仕上温度と熱延板結晶粒径
の関係を示す図表である。
FIG. 1 is a chart showing a relationship between a hot-rolling finishing temperature and a hot-rolled sheet crystal grain size in the present invention.

【図2】本発明における熱延仕上温度と製品鉄損の関係
を示す図表である。
FIG. 2 is a chart showing a relationship between a hot rolling finish temperature and a product iron loss in the present invention.

【図3】本発明における熱延仕上温度と製品磁束密度の
関係を示す図表である。
FIG. 3 is a table showing a relationship between a hot rolling finish temperature and a product magnetic flux density in the present invention.

───────────────────────────────────────────────────── フロントページの続き Fターム(参考) 4K033 AA01 CA01 CA02 CA03 CA05 CA07 CA10 FA03 FA04 FA10 HA01 5E041 AA02 AA11 AA19 CA04 HB05 HB07 HB11 NN01 NN17 NN18 ────────────────────────────────────────────────── ─── Continued on the front page F term (reference) 4K033 AA01 CA01 CA02 CA03 CA05 CA07 CA10 FA03 FA04 FA10 HA01 5E041 AA02 AA11 AA19 CA04 HB05 HB07 HB11 NN01 NN17 NN18

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 重量%で、 0.1%≦Si≦3.5%、 0.1%≦Mn≦1.5%、 C ≦0.004%、 N ≦0.002%、 S ≦0.002%、 Ti≦0.003%、 Nb≦0.003%、 V ≦0.005%、 Zr≦0.003%、 Ca≦0.003%、 As≦0.003%、 Cr≦0.05%、 Sn≦0.01%、 Cu≦0.05%、 O ≦0.02% を含有し、残部がFeおよび不可避的不純物からなり、
式(1)で定めるQ値が−4.70以下でαγ変態を有
するスラブを熱間圧延して熱延板とし、次いで1回の冷
間圧延工程を施した後、仕上焼鈍を施し、その後にスキ
ンパス圧延工程を施すか或いは施さない無方向性電磁鋼
板の製造方法であって、熱延仕上温度をAr3 点以上と
することを特徴とする磁束密度が高く鉄損の低い無方向
性電磁鋼板の製造法。 Q=log[([Ti%]+[Nb%]+[V%]+[Zr%]+[Ca%]) ×[C%]] ・・・式(1) 但し、[Ti%] 、[Nb%]、[V%]、[Zr%] 、[C%]、[Ca%]
は、それぞれTi、Nb、V、Zr、Ca、Cの成品中
の重量濃度
1.% by weight: 0.1% ≦ Si ≦ 3.5%, 0.1% ≦ Mn ≦ 1.5%, C ≦ 0.004%, N ≦ 0.002%, S ≦ 0 0.002%, Ti ≦ 0.003%, Nb ≦ 0.003%, V ≦ 0.005%, Zr ≦ 0.003%, Ca ≦ 0.003%, As ≦ 0.003%, Cr ≦ 0. 0.05%, Sn ≦ 0.01%, Cu ≦ 0.05%, O ≦ 0.02%, with the balance being Fe and unavoidable impurities,
A slab having a α-γ transformation with a Q value determined by the formula (1) of -4.70 or less is hot-rolled into a hot-rolled sheet, then subjected to one cold rolling step, and then subjected to finish annealing, and thereafter A method for producing a non-oriented electrical steel sheet which is subjected to a skin pass rolling step or not, wherein a hot-rolling finishing temperature is set to 3 points or more, wherein the magnetic flux density is high and the iron loss is low. Steel sheet manufacturing method. Q = log [([Ti%] + [Nb%] + [V%] + [Zr%] + [Ca%]) × [C%]] Equation (1) where [Ti%], [Nb%], [V%], [Zr%], [C%], [Ca%]
Is the weight concentration of Ti, Nb, V, Zr, Ca, and C in the product, respectively.
【請求項2】 スラブが、更に重量%で、 0.1%≦Al≦2% を含有することを特徴とする請求項1記載の磁束密度が
高く鉄損の低い無方向性電磁鋼板の製造法。
2. A non-oriented electrical steel sheet having a high magnetic flux density and a low iron loss according to claim 1, wherein the slab further contains 0.1% ≦ Al ≦ 2% by weight. Law.
【請求項3】 仕上熱延後の熱延板を680℃以上の温
度で巻き取ることを特徴とする請求項1又は2記載の磁
束密度が高く鉄損の低い無方向性電磁鋼板の製造法。
3. The method for producing a non-oriented electrical steel sheet having a high magnetic flux density and a low iron loss according to claim 1, wherein the hot-rolled sheet after the finish hot rolling is wound at a temperature of 680 ° C. or higher. .
JP2027599A 1999-01-28 1999-01-28 Manufacturing method of non-oriented electrical steel sheet with high magnetic flux density and low iron loss Withdrawn JP2000219916A (en)

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