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JP2011111658A - Method for producing non-oriented magnetic steel sheet having high magnetic flux density - Google Patents

Method for producing non-oriented magnetic steel sheet having high magnetic flux density Download PDF

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JP2011111658A
JP2011111658A JP2009270477A JP2009270477A JP2011111658A JP 2011111658 A JP2011111658 A JP 2011111658A JP 2009270477 A JP2009270477 A JP 2009270477A JP 2009270477 A JP2009270477 A JP 2009270477A JP 2011111658 A JP2011111658 A JP 2011111658A
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steel sheet
oriented electrical
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electrical steel
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JP5375559B2 (en
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Ryutaro Kawamata
竜太郎 川又
Takeshi Kubota
猛 久保田
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Nippon Steel Corp
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Abstract

【課題】低コストで高磁束密度を得ることの出来る無方向性電磁鋼板の製造法を提供する。
【解決手段】0.1%≦Si≦2.0%、Al≦1.0%かつ0.1%≦Si+2Al≦2.0%を満たし、C≦0.004%を含有する無方向性電磁鋼板の製造において、熱間圧延のスラブ加熱温度STを700℃≦ST≦1150℃、仕上圧延開始温度F0Tを650℃≦F0T≦850℃、仕上熱延終了温度FTを550℃≦FT≦800℃に定める。
【選択図】図3
A non-oriented electrical steel sheet manufacturing method capable of obtaining a high magnetic flux density at low cost is provided.
Nondirectional electromagnetic waves satisfying 0.1% ≦ Si ≦ 2.0%, Al ≦ 1.0% and 0.1% ≦ Si + 2Al ≦ 2.0%, and containing C ≦ 0.004% In the production of steel sheets, the hot rolling slab heating temperature ST is 700 ° C. ≦ ST ≦ 1150 ° C., the finish rolling start temperature F 0 T is 650 ° C. ≦ F 0 T ≦ 850 ° C., and the finish hot rolling end temperature FT is 550 ° C. ≦ FT ≦ 800 ° C. Stipulated in
[Selection] Figure 3

Description

本発明は、電気機器の鉄心材料として用いられる、磁束密度が高い無方向性電磁鋼板の製造方法に関するものである。   The present invention relates to a method for producing a non-oriented electrical steel sheet having a high magnetic flux density, which is used as an iron core material for electrical equipment.

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いる。
In recent years, in the fields of electrical machinery, especially rotating machines where non-oriented electrical steel sheets are used as iron core materials, and in the fields of medium and small transformers, global power conservation, energy conservation, and global environmental conservation such as CFC regulations Among these trends, the trend toward higher efficiency is spreading rapidly.
For this reason, there is an increasing demand for non-oriented electrical steel sheets to improve their characteristics, that is, to achieve high magnetic flux density and low iron loss.

無方向性電磁鋼板の低鉄損化は主としてSi、Al添加による電気抵抗率の増加により、使用時に鉄心を形成する各々の鋼板に流れる渦電流損によるジュール熱損失を低減することにより行われてきた。   The reduction of iron loss in non-oriented electrical steel sheets has been achieved mainly by reducing the Joule heat loss due to eddy current loss flowing in each steel sheet forming the iron core during use by increasing the electrical resistivity by adding Si and Al. It was.

一方、回転機、および鉄心を含む機器全体のエネルギー損失としては、鉄心に巻くコイ理屈ルを電流が流れることにより生ずるジュール熱損失である銅損の寄与も重要である。この銅損の低減のためには同じ磁界強度の励磁に必要な電流密度を減少することが有効であり、同一の励磁電流でより高い磁束密度を発現する素材の開発が欠かせない。   On the other hand, as an energy loss of the entire machine including the rotating machine and the iron core, the contribution of copper loss, which is a Joule heat loss caused by current flowing through the coil theory wound around the iron core, is also important. In order to reduce the copper loss, it is effective to reduce the current density required for excitation with the same magnetic field strength, and development of a material that exhibits a higher magnetic flux density with the same excitation current is indispensable.

すなわち、高磁束密度無方向性電磁鋼板の開発が必須である。高磁束密度無方向性電磁鋼板を用いると、励磁される磁束密度が高くなることにより、回転機や小型トランス等の電気機器の鉄心のサイズを小型軽量化することが可能になり、これらを積載した自動車、電車のような移動体においては系全体の重量が軽減されることにより稼働時のエネルギー損失を低減できるという利点もある。
また、回転機においてはトルクが増大し、より小型で高出力の回転機が実現できる。
That is, development of a high magnetic flux density non-oriented electrical steel sheet is essential. The use of high magnetic flux density non-oriented electrical steel sheets increases the magnetic flux density that is excited, making it possible to reduce the size and weight of the iron core of electrical equipment such as rotating machines and small transformers. In a moving body such as an automobile or a train, the energy loss during operation can be reduced by reducing the weight of the entire system.
Further, in the rotating machine, the torque is increased, and a smaller and higher output rotating machine can be realized.

このように、高磁束密度無方向性電磁鋼板が実現することにより、鉄心及び回転機の動作時のエネルギー損失を低減できるのみならず、それを含めた装置全体の系への波及効果も計り知れないものがある。   Thus, the realization of a high magnetic flux density non-oriented electrical steel sheet not only can reduce the energy loss during the operation of the iron core and the rotating machine, but also has a ripple effect on the entire system including it. There is nothing.

従来、低鉄損を目的として開発されてきた無方向性電磁鋼板では、主としてSi、Al等の電気抵抗率の高い元素が添加されてきたが、これらの元素の含有量が増加すると、無方向性電磁鋼板の飽和磁束密度が低下するため、電気機器として実際に使用する際の動作磁束密度を増加させるために励磁電流を増加させねばならず、銅損が増加するという難点があった。そのため、Si、Al等の電気抵抗率の高い元素を多く含有する無方向性電磁鋼板では動作磁束密度を下げざるをえず、その結果として、たとえば回転機では高トルクを発揮させることが困難になる問題点があった。   Conventionally, in non-oriented electrical steel sheets that have been developed for the purpose of low iron loss, elements having high electrical resistivity such as Si and Al have been mainly added, but if the content of these elements increases, non-oriented Since the saturation magnetic flux density of the heat-resistant electrical steel sheet is reduced, the excitation current has to be increased in order to increase the operating magnetic flux density when actually used as an electrical device, resulting in an increase in copper loss. Therefore, the non-oriented electrical steel sheet containing many elements having high electrical resistivity such as Si and Al has to reduce the operating magnetic flux density. As a result, for example, it is difficult to exert high torque in a rotating machine. There was a problem.

そこで、Si、Alの含有量を制限した無方向性電磁鋼板が提案されている。
特許文献1には、C≦0.02%、SiもしくはSiとAlの合計量が1.5%以下、Mn:1.0%以下、P:0.20%以下を含有し残部は不可避不純物からなる鋼の仕上圧延終了温度を600〜700℃の低温仕上げとし、500℃以下の温度で巻き取り、この鋼帯をA3変態点以下の温度域において30秒以上15分以下焼鈍することを特徴とする無方向性電磁鋼板の製造法が開示されている。
Then, the non-oriented electrical steel sheet which restricted content of Si and Al has been proposed.
Patent Document 1 discloses that C ≦ 0.02%, the total amount of Si or Si and Al is 1.5% or less, Mn: 1.0% or less, and P: 0.20% or less, with the balance being inevitable impurities. The finish rolling finish temperature is a low temperature finish of 600 to 700 ° C., wound at a temperature of 500 ° C. or less, and this steel strip is annealed for 30 seconds or more and 15 minutes or less in a temperature range below the A3 transformation point. A method for producing a conductive electrical steel sheet is disclosed.

しかしながら、この製造法においては、熱延終了後の熱延鋼帯に熱延板焼鈍を施す工程が必須であり、このためコスト上昇を招く課題があり、コスト削減要請の強い無方向性電磁鋼板の需要家には受け入れ難い技術であった。
さらに、実施例では、C含有量は質量%で0.004%以上となっており、後述するように、本発明で知見した熱延板焼鈍を省略する一回冷延法の無方向性電磁鋼板製造法において、C含有量を一定以下に制限することにより、熱延から始まる一貫プロセスの制御による集合組織制御を通じて、成品の磁束密度を向上させる効果を高めるとの技術的思想は見当らない。
However, in this manufacturing method, a step of subjecting the hot-rolled steel strip after hot-rolling to hot-rolled sheet annealing is indispensable. Therefore, there is a problem that causes an increase in cost, and a non-oriented electrical steel sheet with a strong demand for cost reduction. This technology was unacceptable to consumers.
Further, in the examples, the C content is 0.004% or more in mass%, and as described later, the non-directional electromagnetic of the single cold rolling method omitting the hot-rolled sheet annealing found in the present invention. In the steel plate manufacturing method, by limiting the C content to a certain value or less, there is no technical idea that the effect of improving the magnetic flux density of the product is enhanced through texture control by controlling an integrated process starting from hot rolling.

特許文献2には、SiとAlの合計量が1.5%以下の鋼を用い、その仕上熱延において、熱延終了温度を600℃以上700℃以下として仕上げ、これを圧下率75%以上85%以下で冷間圧延を施した後に仕上焼鈍を施す製造法が開示されている。
しかしながら、本発明者らの検討によれば、仕上熱延の終了温度を規定するのみでは成品の磁気特性が不安定であり、圧延開始温度を制御することが安定した磁気特性を得るために重要であることを見出した。加えて当該公報の実施例に示された0.006%、0.005%というC濃度では低温での熱間圧延の効果が不足し磁束密度の向上が不十分であるという課題があった。
In Patent Document 2, a steel having a total amount of Si and Al of 1.5% or less is used, and in the finish hot rolling, the hot rolling end temperature is finished at 600 ° C. or more and 700 ° C. or less, and the reduction ratio is 75% or more. A manufacturing method in which finish annealing is performed after cold rolling at 85% or less is disclosed.
However, according to the study by the present inventors, the magnetic properties of the product are unstable only by specifying the finish hot rolling end temperature, and it is important to control the rolling start temperature to obtain stable magnetic properties. I found out. In addition, the C concentrations of 0.006% and 0.005% shown in the examples of the publication have a problem that the effect of hot rolling at low temperature is insufficient and the improvement of the magnetic flux density is insufficient.

またさらに、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、特許文献3のごとくSn添加、特許文献4のごときSn、Cu添加、もしくは特許文献5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。
しかしながら、これらの集合組織制御元素であるSn,CuもしくはSb等の添加をもってしても昨今の需要家の高磁束密度低鉄損無方向性電磁鋼板を安価な供給の要求には応えることが充分出来なかった。
Furthermore, as a method of improving the magnetic properties of the non-oriented electrical steel sheet by improving the primary recrystallization texture, Sn addition as in Patent Document 3, Sn and Cu addition as in Patent Document 4, or Patent Document 5 For example, a method for producing a non-oriented electrical steel sheet having excellent magnetic properties by improving the texture by adding Sb is disclosed.
However, even with the addition of these texture control elements, such as Sn, Cu, or Sb, it is sufficient to meet the demand for low-cost supply of high magnetic flux density, low iron loss non-oriented electrical steel sheets of today's customers. I could not do it.

他にも、特許文献6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充分な向上がみられなかった。   In addition, although measures have been taken on the manufacturing process such as the finishing annealing cycle as described in Patent Document 6, the magnetic flux density is sufficient even if the iron loss is reduced. There was no improvement.

このように、従来技術では、昨今の需要家において開発要請の強い鉄心の小型化に有利な高磁束密度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。   Thus, in the prior art, it has not been possible to manufacture a high magnetic flux density non-oriented electrical steel sheet that is advantageous for downsizing of iron cores, which is strongly demanded by recent customers. I couldn't respond.

特開昭58−204126号公報JP 58-204126 A 特開昭59−104429号公報JP 59-104429 A 特開昭55−158252号公報JP-A-55-158252 特開昭62−180014号公報JP 62-180014 A 特開昭59−100217号公報Japanese Patent Laid-Open No. 59-100197 特開昭57−35265号公報JP-A-57-35265

本発明は、従来技術におけるこのような課題を解決し、高磁束密度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。   An object of the present invention is to solve such problems in the prior art and to provide a high magnetic flux density non-oriented electrical steel sheet.

本発明は、特定の条件下で仕上熱延工程を実施して熱延板の集合組織を予め造りこんでおくことで、熱延板焼鈍を省略しても、冷間圧延して、仕上焼鈍した後の再結晶集合組織を制御することが可能であることを新規に知見するとともに、さらに、この製造法を行う際に、鋼に含有される炭素の含有量が前記特定の条件下での仕上熱延工程の効果に顕著な影響を及ぼすことを新規に知見した結果なされたものである。これにより従来技術よりも安価な方法で高磁束密度である無方向性電磁鋼板の製造技術を提供するものである。   The present invention performs a finish hot rolling process under specific conditions to create a hot-rolled sheet texture in advance, so that even if hot-rolled sheet annealing is omitted, it is cold-rolled and finish-annealed. In addition to newly discovering that it is possible to control the recrystallized texture after the processing, the carbon content contained in the steel under the above specific conditions is further reduced when performing this production method. This is a result of a new finding that the effect of the finish hot rolling process is significantly affected. This provides a technique for producing a non-oriented electrical steel sheet having a high magnetic flux density by a method that is cheaper than the prior art.

本発明の要旨とするところは、以下の通りである。
請求項1の発明は、
鋼中に質量%で0.1%≦Si≦2.0、%Al≦1.0%で、
かつ、0.1%≦Si+2Al≦2.0%の関係を満たし、
さらに、C≦0.004%、S≦0.003%、N≦0.003% を含有し、残部がFeおよび不可避的不純物からなる鋼をスラブとして、熱間圧延において粗圧延および引き続く仕上熱延を施し熱延板とし、酸洗し一回の冷間圧延工程を施し次いで仕上げ焼鈍を施す無方向性電磁鋼板の製造方法において、
仕上げ熱延のスラブ加熱温度ST、仕上熱延開始温度F0T、仕上熱延終了温度FTをそれぞれ、
700℃≦ST≦1150℃
650℃≦F0T≦850℃
550℃≦FT≦800℃
のように定めたことを特徴とする磁束密度の高い無方向性電磁鋼板の製造方法、であり、
The gist of the present invention is as follows.
The invention of claim 1
In steel, 0.1% ≦ Si ≦ 2.0,% Al ≦ 1.0% by mass%,
And 0.1% ≦ Si + 2Al ≦ 2.0% is satisfied,
Further, the steel containing C ≦ 0.004%, S ≦ 0.003%, N ≦ 0.003%, the balance being Fe and inevitable impurities is used as a slab for rough rolling and subsequent finishing heat in hot rolling. In the method for producing a non-oriented electrical steel sheet, the hot rolled sheet is subjected to rolling, pickled, subjected to a single cold rolling step, and then subjected to finish annealing.
Finishing hot rolling slab heating temperature ST, finishing hot rolling start temperature F0T, finishing hot rolling end temperature FT, respectively,
700 ℃ ≦ ST ≦ 1150 ℃
650 ℃ ≦ F0T ≦ 850 ℃
550 ℃ ≦ FT ≦ 800 ℃
A method for producing a non-oriented electrical steel sheet having a high magnetic flux density, characterized by being defined as follows:

また、請求項1の発明により製造した電磁鋼板に関する請求項2の発明は、
鋼板の表面から板厚方向10分の1層においてX線回折測定により作成した(100)極点図において、
α=80°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°における強度がすべて1.0以上であり、
かつ、鋼板の板厚方向中心層2分の1層においてX線回折測定により測定した(100)極点図において、
50°≦α≦70°かつβがそれぞれβ=0°、60°、120°、180°、240°、300°で定められるα、βの領域に強度が1.0以上である領域が存在することを特徴とする無方向性電磁鋼板、であり、
同じく請求項3の発明は、
鋼板の表面から板厚方向10分の1層においてX線回折測定により作成した(100)極点図において、
α=80°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°における強度がすべて1.0以上、かつ、同一極点図上において、α=90°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°における強度がすべて1.0以上であり、
かつ、鋼板の板厚方向中心層である2分の1層においてX線回折測定により作成した(100)極点図において、
50°≦α≦70°かつβがそれぞれβ=0°、60°、120°、180°、240°、300°で定められるα、βの領域に強度が1.0以上である領域が存在することを特徴とする無方向性電磁鋼板、であり、
さらに、同じく請求項4の発明は、
鋼板の表面から板厚方向10分の1層においてX線回折測定により得られた逆極点図における(100)面、(411)面、(111)面の強度をそれぞれI(100)、I(411)、I(111)とすると、
I(100)≧2.0
I(411)≧1.5
I(111)≦4.0
かつ、
{I(100)+I(411)}/I(111) ≧1.0
を満たすことを特徴とする無方向性電磁鋼板、である。
Further, the invention of claim 2 relating to the electrical steel sheet manufactured by the invention of claim 1
In the (100) pole figure created by X-ray diffraction measurement in 1 / 10th layer in the plate thickness direction from the surface of the steel plate,
α = 80 ° and β are respectively β = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, 330 °, and the strengths are all 1.0 or more,
And in the (100) pole figure measured by X-ray diffraction measurement in the half layer thickness direction center layer of the steel plate,
There is a region where the intensity is 1.0 or more in the regions of α and β where 50 ° ≦ α ≦ 70 ° and β is determined by β = 0 °, 60 °, 120 °, 180 °, 240 °, and 300 °, respectively. A non-oriented electrical steel sheet, characterized by
Similarly, the invention of claim 3
In the (100) pole figure created by X-ray diffraction measurement in 1 / 10th layer in the plate thickness direction from the surface of the steel plate,
α = 80 ° and β are β = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, 330 °, all of strengths of 1.0 or more, and on the same pole figure, α = 90 ° and β are respectively β = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, 330 °, and the strengths are all 1.0 or more,
And in the (100) pole figure created by X-ray diffraction measurement in the half layer which is the center layer in the plate thickness direction of the steel plate,
There is a region where the intensity is 1.0 or more in the regions of α and β where 50 ° ≦ α ≦ 70 ° and β is determined by β = 0 °, 60 °, 120 °, 180 °, 240 °, and 300 °, respectively. A non-oriented electrical steel sheet, characterized by
Furthermore, the invention of claim 4
The strengths of the (100), (411), and (111) planes in the reverse pole figure obtained by X-ray diffraction measurement at a 1 / 10th layer in the thickness direction from the surface of the steel sheet are I (100) and I ( 411), I (111)
I (100) ≧ 2.0
I (411) ≧ 1.5
I (111) ≦ 4.0
And,
{I (100) + I (411)} / I (111) ≧ 1.0
It is a non-oriented electrical steel sheet characterized by satisfying.

さらに、請求項5の発明は、
この無方向性電磁鋼板の磁気特性向上のために、冷間圧延工程における圧延率を85%以上95%以下とすることを特徴とする無方向性電磁鋼板の製造方法、である。
Furthermore, the invention of claim 5
In order to improve the magnetic properties of this non-oriented electrical steel sheet, a non-oriented electrical steel sheet manufacturing method is characterized in that the rolling rate in the cold rolling step is 85% or more and 95% or less.

さらに、請求項6の発明は、請求項1または5に記載の無方向性電磁鋼板の製造方法によって製造された電磁鋼板あるいは請求項2〜4のいずれかに記載の電磁鋼板を鉄心に加工する際の剪断時に、鉄心の磁束の流れる方向を鋼板の圧延方向から鋼板板面内で左右に45度傾いた方向に一致させる無方向性電磁鋼板の剪断方法、である。
さらに、請求項7の発明は、請求項6の方法により製造した無方向性電磁鋼板により製造した電磁部品であって、該電磁部品が、EIコア、回転機用分割コア、トランス用額縁鉄心、小型鉄心、リアクトル用鉄心、螺旋コアのいずれかであることを特徴とする電磁部品、である。
Furthermore, invention of Claim 6 processes the electromagnetic steel plate manufactured by the manufacturing method of the non-oriented electrical steel plate of Claim 1 or 5, or the electromagnetic steel plate of any one of Claims 2-4 into an iron core. This is a shearing method for a non-oriented electrical steel sheet in which the direction in which the magnetic flux flows in the iron core coincides with a direction inclined 45 degrees to the left and right within the steel sheet surface from the rolling direction of the steel sheet.
Furthermore, the invention of claim 7 is an electromagnetic component manufactured by the non-oriented electrical steel sheet manufactured by the method of claim 6, wherein the electromagnetic component includes an EI core, a split core for a rotating machine, a frame iron core for a transformer, An electromagnetic component characterized by being a small iron core, a reactor core, or a spiral core.

本発明によれば、磁束密度の高い無方向性電磁鋼板及びその電磁鋼板を用いた電磁部品を低コストで製造することが可能である。   ADVANTAGE OF THE INVENTION According to this invention, it is possible to manufacture the non-oriented electrical steel plate with a high magnetic flux density, and the electromagnetic components using the electromagnetic steel plate at low cost.

鋼板の板厚方向表層から10分の1層の(100)極点図において、強度を規定した位置を示す図であり、●:α=90°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°、◆:α=80°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°である点をそれぞれ示す。In the (100) pole figure of one-tenth layer from the surface layer in the plate thickness direction of the steel sheet, it is a diagram showing the position where the strength is defined, ●: α = 90 ° and β is β = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, 330 °, ◆: α = 80 ° and β is β = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, Each point is 330 °. 鋼板の板厚方向中心層2分の1層の(100)極点図において50°≦α≦70°かつβがそれぞれβ=0°、60°、120°、180°、240°、300°である本発明で強度を規定した6箇所の範囲(両端矢印部)を示す。In the (100) pole figure of the half-thickness center layer of the steel sheet, 50 ° ≦ α ≦ 70 ° and β is β = 0 °, 60 °, 120 °, 180 °, 240 °, 300 °, respectively. 6 shows a range (both end arrows) where the strength is defined by a certain present invention. 表層から板厚10分の1層における(100)極点図である。It is a (100) pole figure in 1 / 10th sheet thickness from a surface layer. 表層から板厚2分の1層における(100)極点図である。It is a (100) pole figure in a half layer thickness from a surface layer. 本発明例と比較例のEIコアの打ち抜き方法を示す図である。It is a figure which shows the punching method of EI core of this invention example and a comparative example. 本発明例と比較例の額縁コアの打ち抜き方法を示す図である。It is a figure which shows the punching method of the frame core of this invention example and a comparative example. 本発明例と比較例の分割コアの打ち抜き方法を示す図である。It is a figure which shows the punching method of the split core of the example of this invention and a comparative example. 本発明例と比較例の螺旋コアの打ち抜き方法を示す図である。It is a figure which shows the punching method of the spiral core of the example of this invention and a comparative example.

発明者らは、従来にない高磁束密度を達成する無方向性電磁鋼板の安価な製造方法について鋭意検討を重ねた結果、特定の条件下で仕上熱延工程を実施して熱延板の集合組織を予め造りこんでおくことで、熱延板焼鈍を省略しても、冷間圧延して、仕上焼鈍した後の再結晶集合組織を制御することが可能であることを新規に知見するとともに、さらに、この製造法を行う際に、鋼に含有される炭素の含有量が前記特定の条件下での仕上熱延工程の効果に顕著な影響を及ぼすことを新規に知見した。そして、これらの知見に基づいて、従来技術よりも安価な方法で高磁束密度である無方向性電磁鋼板の製造技術を提供するものである。   As a result of intensive studies on an inexpensive method for producing a non-oriented electrical steel sheet that achieves an unprecedented high magnetic flux density, the inventors have conducted a finish hot rolling process under specific conditions to collect a set of hot rolled sheets. By creating the structure in advance, it is newly discovered that it is possible to control the recrystallization texture after cold rolling and finish annealing even if hot-rolled sheet annealing is omitted. Furthermore, it has been newly found out that the content of carbon contained in steel has a significant effect on the effect of the finish hot rolling process under the specific conditions when performing this production method. And based on these knowledge, the manufacturing technique of the non-oriented electrical steel sheet which is high magnetic flux density by the method cheaper than a prior art is provided.

以下、本件発明について順次説明する。
まず、鋼の成分について説明する。
Hereinafter, the present invention will be sequentially described.
First, the components of steel will be described.

Siは、本発明においては、過度の添加は製品の磁束密度を低減させ有害であるから、その含有量を2.0%以下と制限する。一方、磁束密度の向上を妨げない範囲で電気抵抗率を確保して渦電流損を低減させる目的で0.1%以上の添加量が必要である。   In the present invention, excessive addition of Si is harmful because it reduces the magnetic flux density of the product, so its content is limited to 2.0% or less. On the other hand, an addition amount of 0.1% or more is required for the purpose of ensuring electric resistivity within a range not hindering improvement in magnetic flux density and reducing eddy current loss.

Alは、Siと同様に電気抵抗率を確保する目的で添加してもよい。本発明では、Alの添加は必須ではないので含有量の下限は定めない。一方、Siと同様に、過度の添加は製品の磁束密度を低減させ有害であるから、その含有量を1.0%以下と制限する。   Al may be added for the purpose of securing electrical resistivity in the same manner as Si. In the present invention, since the addition of Al is not essential, the lower limit of the content is not determined. On the other hand, like Si, excessive addition reduces the magnetic flux density of the product and is harmful, so its content is limited to 1.0% or less.

SiとAlは電気抵抗率を確保するのに添加されるため、(Si+2Al)の合計量を0.1%以上とする必要がある。一方、(Si+2Al)の合計量が2.0%超であると、製品の磁束密度を低減させ有害であるから、(Si+2Al)の合計量を2.0%以下と制限する。   Since Si and Al are added to ensure electrical resistivity, the total amount of (Si + 2Al) needs to be 0.1% or more. On the other hand, if the total amount of (Si + 2Al) exceeds 2.0%, the magnetic flux density of the product is reduced, which is harmful. Therefore, the total amount of (Si + 2Al) is limited to 2.0% or less.

Cは、その含有量を一定量以下に制御される。このことは、後述するように、仕上熱延から仕上焼鈍に至る一貫プロセスにおいて集合組織制御を行う効果を十分に発現させるために重要な新規知見である。
従来のように、無方向性電磁鋼板として使用中の磁気時効による損失の増加を防止する観点だけであれば、その含有量は0.004%以下であれば十分である。
しかし本発明では、Cの含有量が0.004%超であると、仕上焼鈍後の成品の再結晶集合組織の制御に成功せず、高磁束密度が得られなくなる。従って、C含有量は0.004%以下に定める。さらに、本発明における無方向性電磁鋼板の磁束密度向上効果を高めるためには、C含有量は0.003%以下であることが好ましく、さらに0.002%以下であることがより好ましい。
The content of C is controlled to a certain amount or less. As will be described later, this is an important new finding in order to sufficiently exhibit the effect of texture control in an integrated process from finish hot rolling to finish annealing.
If it is only a viewpoint which prevents the increase in the loss by the magnetic aging in use as a non-oriented electrical steel sheet like the past, it is enough if the content is 0.004% or less.
However, in the present invention, if the C content is more than 0.004%, the recrystallization texture of the product after finish annealing cannot be controlled successfully, and a high magnetic flux density cannot be obtained. Therefore, the C content is set to 0.004% or less. Furthermore, in order to enhance the effect of improving the magnetic flux density of the non-oriented electrical steel sheet in the present invention, the C content is preferably 0.003% or less, and more preferably 0.002% or less.

本発明ではS、Nの低減により高磁束密度が可能となる。
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、AlNの微細な析出物を再析出して仕上焼鈍時の結晶粒成長を抑制し、磁束密度、鉄損が悪化する原因となる。このためその含有量は共に0.003%以下とする必要がある。
In the present invention, a high magnetic flux density can be achieved by reducing S and N.
S and N are partly re-dissolved during slab heating in the hot rolling process, and fine precipitates of MnS and AlN are re-precipitated during hot rolling to suppress crystal grain growth during finish annealing, and magnetic flux It causes the density and iron loss to deteriorate. For this reason, both the contents must be 0.003% or less.

次にプロセス条件について説明する。
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。
Next, process conditions will be described.
The steel slab composed of the above components is melted in a converter and manufactured by continuous casting or ingot-bundling rolling. The steel slab is heated by a known method. The slab is hot rolled to a predetermined thickness.

熱間圧延では、スラブ加熱温度STが700℃未満であると成品の磁束密度が低下するのでスラブ加熱温度は700℃以上に定める。一方、スラブ加熱温度が1150℃超となると、鋼中のS等の不純物が再固溶し、仕上熱延中に微細に再析出して仕上焼鈍中の結晶粒成長を妨げ、鉄損が著しく悪化するとともに仕上焼鈍中の再結晶制御を妨げ、磁束密度も低下するので、スラブ加熱温度は1150℃以下に定める。   In hot rolling, if the slab heating temperature ST is less than 700 ° C., the magnetic flux density of the product decreases, so the slab heating temperature is set to 700 ° C. or higher. On the other hand, when the slab heating temperature exceeds 1150 ° C., impurities such as S in the steel re-dissolve and reprecipitates finely during finish hot rolling, preventing crystal grain growth during finish annealing, resulting in significant iron loss. The slab heating temperature is set to 1150 ° C. or lower because it deteriorates and hinders recrystallization control during finish annealing and lowers the magnetic flux density.

仕上熱延開始温度F0Tは、その温度が650℃未満となると仕上熱延時の圧延反力が増大して圧延が困難となるので、650℃以上に定める。一方、仕上熱延開始温度が850℃超になると、仕上熱延中の再結晶進行の速度が速くなりすぎ、仕上熱延を行いながら熱延鋼帯の集合組織を制御する本発明の効果が損なわれ、結果として成品の磁束密度が著しく低下するので、850℃以下に定める。   The finish hot rolling start temperature F0T is set to 650 ° C. or higher because when the temperature is less than 650 ° C., the rolling reaction force during finish hot rolling increases and rolling becomes difficult. On the other hand, when the finish hot rolling start temperature exceeds 850 ° C., the recrystallization progress rate during finish hot rolling becomes too high, and the effect of the present invention for controlling the texture of the hot rolled steel strip while performing finish hot rolling is effective. It is damaged, and as a result, the magnetic flux density of the product is remarkably lowered.

仕上熱延終了温度FTが550℃未満となると、板厚制御が困難になるとともに成品の磁束密度が低下するので仕上熱延終了温度は550℃以上に定める。仕上熱延終了温度が800℃超となると、仕上熱延中の再結晶進行の速度が速くなりすぎ、仕上熱延を行いながら熱延鋼帯の集合組織を制御する本発明の効果が損なわれ、結果として成品の磁束密度が著しく低下するので、仕上熱延終了温度は800℃以下に定める。   If the finish hot rolling end temperature FT is less than 550 ° C., the thickness control becomes difficult and the magnetic flux density of the product decreases, so the finish hot rolling end temperature is set to 550 ° C. or more. When the finish hot rolling finish temperature exceeds 800 ° C., the recrystallization progress rate during finish hot rolling becomes too high, and the effect of the present invention for controlling the texture of the hot rolled steel strip while performing finish hot rolling is impaired. As a result, the magnetic flux density of the product is remarkably lowered, so the finish hot rolling end temperature is set to 800 ° C. or less.

本発明では仕上熱延中に熱延鋼帯の集合組織を制御する必要があることから、スラブ加熱温度、仕上熱延開始温度、仕上熱延終了温度を制御する必要がある。これにより熱延鋼帯の集合組織を予め冷間圧延前に造りこんでおき、その後の冷間圧延および仕上焼鈍中の再結晶集合組織を制御して磁束密度を高める効果がある。   In the present invention, since it is necessary to control the texture of the hot-rolled steel strip during finish hot rolling, it is necessary to control the slab heating temperature, the finish hot rolling start temperature, and the finish hot rolling end temperature. Thereby, the texture of the hot-rolled steel strip is preliminarily formed before cold rolling, and the effect of increasing the magnetic flux density by controlling the recrystallization texture during the subsequent cold rolling and finish annealing.

この効果は成分の説明でも述べたように、C含有量を制御することで促進される。
この技術思想により従来よりも低鉄損が達成される理由は現在のところ鋭意検討中であるが、仕上熱延を低温域で実施することにより、熱延鋼帯の集合組織を改善することができ、このため冷間圧延、再結晶後の成品の再結晶集合組織中の結晶粒のうち、{100}面を板面に並行に持つ方位付近の結晶粒を鋼板の表層付近において富化可能であることが本発明の磁束密度向上の機構であると推察している。
This effect is promoted by controlling the C content as described in the explanation of the components.
The reason why low iron loss can be achieved by this technical idea is under intensive study at present. However, it is possible to improve the texture of hot-rolled steel strip by carrying out finish hot rolling in a low temperature range. Therefore, among the crystal grains in the recrystallized texture of the product after cold rolling and recrystallization, the grains near the orientation with the {100} plane parallel to the plate surface can be enriched near the surface layer of the steel plate This is presumed to be the mechanism for improving the magnetic flux density of the present invention.

さらに、熱延開始温度および熱延終了温度が高すぎると、α相域の仕上熱延により造りこんだ熱延鋼帯の集合組織が再結晶と粒成長の進行により消失し成品の磁束密度が低下することを発明者らは突き止めた。   Furthermore, if the hot rolling start temperature and hot rolling end temperature are too high, the texture of the hot rolled steel strip formed by finishing hot rolling in the α phase region disappears due to the progress of recrystallization and grain growth, and the magnetic flux density of the product is reduced. The inventors have found that it decreases.

また、従来技術で無方向性電磁鋼板の磁束密度を向上させるために用いられてきた熱延板焼鈍は、本発明で開示した方法で製造した熱延鋼帯内の集合組織を、熱延板焼鈍中に再結晶と粒成長により消失させる為、成品の磁束密度を充分向上させることができない。   Moreover, the hot-rolled sheet annealing that has been used in the prior art to improve the magnetic flux density of the non-oriented electrical steel sheet is the hot-rolled sheet in the texture in the hot-rolled steel strip manufactured by the method disclosed in the present invention. Since it disappears by recrystallization and grain growth during annealing, the magnetic flux density of the product cannot be sufficiently improved.

この従来の熱延版焼鈍を伴う製造方法による技術思想は、冷間圧延前の結晶粒径を粗大化させることにより、磁束密度の向上を妨げる{111}面を板面に並行に有する結晶粒の発達を抑制し、{110}<001>方位を有する結晶粒の存在量を増加させることにあった。
このため、仕上熱延により制御した熱延鋼帯の集合組織を直接活用することにより成品の磁束密度を向上させるという本発明の技術思想とは全く異なるものである。
The technical idea of the manufacturing method involving this conventional hot rolling annealing is that crystal grains having {111} planes in parallel with the plate surface that hinder the improvement of magnetic flux density by increasing the crystal grain size before cold rolling. It was to increase the abundance of crystal grains having {110} <001> orientation.
For this reason, it is completely different from the technical idea of the present invention in which the magnetic flux density of the product is improved by directly utilizing the texture of the hot-rolled steel strip controlled by finish hot rolling.

また、この目的を達成する熱延開始温度、熱延終了温度が低すぎても成品の磁束密度が低下することをも発明者らは明らかにした。
すなわち、本発明が意図する熱延鋼帯の集合組織の制御のためには、最適な熱延開始温度、熱延終了温度の範囲があることを発明者らは明らかにしたのである。
The inventors have also clarified that the magnetic flux density of the product decreases even if the hot rolling start temperature and hot rolling end temperature for achieving this object are too low.
That is, the inventors have clarified that there is a range of optimum hot rolling start temperature and hot rolling end temperature for controlling the texture of the hot rolled steel strip intended by the present invention.

また、鋼中のC量が本発明で規定する範囲を超過すると、仕上熱延により成品の磁束密度向上に適した集合組織を熱延鋼帯に造りこむことが著しく阻害され、成品の磁束密度が顕著に低下することも発明者らは新規知見として見出した。   In addition, when the amount of C in the steel exceeds the range specified in the present invention, it is significantly impeded to create a texture suitable for improving the magnetic flux density of the product by hot rolling in the hot rolled steel strip, and the magnetic flux density of the product. The inventors have also found as a new finding that the remarkably decreases.

仕上熱延終了後の熱延鋼帯は酸洗を施し、冷間圧延を施して最終板厚に仕上げる。冷間圧延後の冷延鋼帯は、仕上焼鈍により再結晶を行わせ、成品とする。この成品は歪取り焼鈍を施さずに使用するか、或いは施してから使用してもよく、また打ち抜き工程を経て整形した後に、歪取り焼鈍を施して使用してもよい。   The hot-rolled steel strip after finishing hot rolling is pickled and cold-rolled to the final thickness. The cold-rolled steel strip after cold rolling is recrystallized by finish annealing to obtain a finished product. This product may be used without being subjected to strain relief annealing, or may be used after being applied, or may be used after being subjected to strain relief annealing after being shaped through a punching process.

仕上焼鈍の温度域は、熱延鋼帯に造りこんだ集合組織から仕上焼鈍中に磁束密度を高めるのに適切な再結晶集合組織を形成させる必要があるため、α相域で行う必要がある。すなわち、仕上焼鈍温度がα相域の上限であるAc1点を超えると、成品の磁束密度が低下するので、仕上焼鈍温度はα相内であるAc1点以下で行う必要がある。   The temperature range of finish annealing needs to be performed in the α phase range because it is necessary to form an appropriate recrystallized texture to increase the magnetic flux density during finish annealing from the texture built into the hot-rolled steel strip. . That is, when the finish annealing temperature exceeds the Ac1 point which is the upper limit of the α phase region, the magnetic flux density of the product is lowered. Therefore, the finish annealing temperature needs to be performed at the Ac1 point or less within the α phase.

仕上げ焼鈍時間が10秒未満では再結晶が不十分となり高磁束密度が得られないので、10秒以上であることが好ましい。一方、仕上げ焼鈍時間が3分を超えると、生産性が悪化し、コストが上昇するので、仕上げ焼鈍時間は3分以内が好ましい。
これにより、磁束密度の高い無方向性電磁鋼板を従来よりも低コストで製造することが可能となる。
If the final annealing time is less than 10 seconds, recrystallization is insufficient and a high magnetic flux density cannot be obtained. On the other hand, when the finish annealing time exceeds 3 minutes, the productivity is deteriorated and the cost is increased. Therefore, the finish annealing time is preferably within 3 minutes.
Thereby, it becomes possible to manufacture a non-oriented electrical steel sheet having a high magnetic flux density at a lower cost than before.

本発明により得られた高磁束密度無方向性電磁鋼板は、小型軽量化を要求される電気機器、回転機の鉄心、小型トランスに最適であるが、他にも各種コンプレッサー、発電機、高出力を要求される電気自動車用モーター等の鉄心用途等に適している。   The high magnetic flux density non-oriented electrical steel sheet obtained by the present invention is most suitable for electrical equipment that is required to be small and light, iron cores of rotating machines, and small transformers, but also various compressors, generators, high output It is suitable for iron core applications such as motors for electric vehicles that require high power.

本発明では発明の規定に極点図を用いるが、その極点図中の位置を表す方法として、α、βを用いる。これらは角度であり、αは極点図中心から外周へ向かう方向、βは円周方向を示す。極点図上ではαは0°から90°の範囲を用い、βは0から360°の範囲を用いる。βの0°は後述のように360°と同一である。   In the present invention, a pole figure is used for the definition of the invention, and α and β are used as a method of representing the position in the pole figure. These are angles, α indicates a direction from the center of the pole figure toward the outer periphery, and β indicates a circumferential direction. On the pole figure, α uses a range of 0 ° to 90 °, and β uses a range of 0 to 360 °. 0 ° of β is the same as 360 ° as described later.

α角については、極点図中心をα=0°とし、極点図外周をα=90°とする。極点図中央を中心とする同心円上ではα角は同一である。極点図上のα角の分布はステレオ投影法により定められるため等間隔ではないので極点図の縦軸および横軸に10°ごとにその目盛りを示した。   For the α angle, the center of the pole figure is α = 0 °, and the outer periphery of the pole figure is α = 90 °. The α angle is the same on a concentric circle centered on the center of the pole figure. Since the distribution of α angles on the pole figure is determined by the stereo projection method and is not equidistant, the scale is shown every 10 ° on the vertical and horizontal axes of the pole figure.

β角については、極点図上の圧延方向であるRD方向を0°とし、極点図の中心を通る垂直線を回転軸として時計方向周りに均等に360分割する。これにより極点図上のβ角は極点図のRD方向から時計方向周りの角度で表す。β角の360°はRD方向から1周してもとのRD方向に到達した位置であるのでβ角の0°と同一である。   For the β angle, the RD direction, which is the rolling direction on the pole figure, is set to 0 °, and the vertical line passing through the center of the pole figure is divided into 360 parts evenly in the clockwise direction around the rotation axis. Accordingly, the β angle on the pole figure is expressed as an angle clockwise from the RD direction of the pole figure. The β angle of 360 ° is the same position as the β angle of 0 ° because it is the position reached in the original RD direction even after one round from the RD direction.

本発明では結晶方位を表す際にミラー指数を用い、その方法についてはカリティ著にて株式会社アグネより昭和55年6月(1980年6月)に発行された新版X線回折要論の第2章に記載された方法に従う。   In the present invention, the Miller index is used to represent the crystal orientation, and the second method of the new edition X-ray diffraction theory published in June 1980 by Agne Co., Ltd. was published by Karity. Follow the method described in the chapter.

次に図1及び図2を用いて請求項2及び請求項3の限定理由を述べる。
図1及び図2は実施例1にて示した本発明の方法にて製造した無方向性電磁鋼板をX線回折により測定して得られた(100)極点図である。
Next, reasons for limitation of claims 2 and 3 will be described with reference to FIGS.
1 and 2 are (100) pole figures obtained by measuring the non-oriented electrical steel sheet produced by the method of the present invention shown in Example 1 by X-ray diffraction.

図1に鋼板の表層から板厚方向10分の1層の(100)極点図において、α=90°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°の点を●印で示した。これらの位置は(100)極点図外周にあたりbcc鉄の結晶の{100}面が鋼板面と平行である結晶方位に属する。   In FIG. 1, in the (100) pole figure from the surface layer of steel plate to 1 / 10th layer in the plate thickness direction, α = 90 ° and β are β = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, respectively. , 300 °, 330 ° points are indicated by ● marks. These positions belong to the crystal orientation in which the {100} plane of the bcc iron crystal is parallel to the steel plate surface on the periphery of the (100) pole figure.

この8箇所の位置の極点図での強度が全て1.0以上であると鋼板を磁化した際に板面内を流れる磁束とbcc鉄の結晶の磁化容易方向が一致する結晶方位が存在するため鋼板内の磁束の流れが改善され磁気特性が向上する。
すなわち、これら8箇所の位置の強度が全て1.0以上であることにより、鋼板内のより多くの方向の磁束の流れが改善され、同時に回転磁束下での磁気特性も向上するので全て1.0以上に規定する。
If all of the strengths in the pole figures at these eight positions are 1.0 or more, there is a crystal orientation in which the magnetic flux flowing in the plate surface coincides with the easy magnetization direction of the bcc iron crystal when the steel plate is magnetized. The flow of magnetic flux in the steel sheet is improved and the magnetic properties are improved.
That is, since the strengths of these eight positions are all 1.0 or more, the flow of magnetic flux in more directions in the steel sheet is improved, and at the same time the magnetic characteristics under the rotating magnetic flux are also improved. Specify 0 or more.

一方、これら8箇所の位置の一部もしくは全部の強度が1.0未満であると鋼板内での磁束の流れが困難になり磁束密度が低下するとともに鉄損が増加するので全て1.0以上に定める。   On the other hand, if the strength of some or all of these eight positions is less than 1.0, the flow of magnetic flux in the steel sheet becomes difficult, and the magnetic flux density decreases and the iron loss increases. Stipulated in

また、図1の(100)極点図にはα=80°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°の点を◆印で示した。これらの位置は{100}面が鋼板面に対し10°傾いているが、{100}面が鋼板面に平行な結晶方位に近く鋼板内の磁束の流れが良好な結晶方位に属する。
このため、(100)極点図上の8箇所のこの方位の位置の強度が全て1.0以上であると磁気特性が改善され磁束密度が向上し鉄損が低下するため、これら8箇所の位置の強度は全て1.0以上に規定する。
In addition, in the (100) pole figure of FIG. 1, α = 80 ° and β are β = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, 330 °, respectively. It showed in. In these positions, the {100} plane is inclined by 10 ° with respect to the steel plate surface, but the {100} plane is close to the crystal orientation parallel to the steel plate surface and belongs to a crystal orientation in which the flow of magnetic flux in the steel plate is good.
For this reason, if the strengths of the eight positions on the (100) pole figure are all 1.0 or more, the magnetic characteristics are improved, the magnetic flux density is increased, and the iron loss is reduced. The strength of all is specified to be 1.0 or more.

これら8箇所の位置の強度が全て1.0以上であることにより、鋼板内のより多くの方向の磁束の流れが改善され、同時に回転磁束下での磁気特性も向上するので全て1.0以上に規定する。
一方、これら8箇所の位置の一部もしくは全部の強度が1.0未満であると鋼板内での磁束の流れが困難になり磁束密度が低下するとともに鉄損が増加するので1.0以上に定める。
Since the strength of these eight positions is all 1.0 or more, the flow of magnetic flux in more directions in the steel sheet is improved, and at the same time, the magnetic characteristics under the rotating magnetic flux are also improved. Stipulate.
On the other hand, if the strength of some or all of these eight positions is less than 1.0, the flow of magnetic flux in the steel sheet becomes difficult, and the magnetic flux density decreases and the iron loss increases. Determine.

発明者らの検討によれば、本発明によれば成品の集合組織制御効果はまず(100)極点図上のα=80°かつβ=30°、60°、120°、150°、210°、240°、300°、330°の8点の強度が向上することにより現れ、次いでα=90°かつβ=30°、60°、120°、150°、210°、240°、300°、330°の8点の強度が向上する。   According to the study by the inventors, according to the present invention, the texture control effect of the product is firstly α = 80 ° and β = 30 °, 60 °, 120 °, 150 °, 210 ° on the (100) pole figure. , 240 °, 300 °, and 330 °, which are manifested by an increase in intensity, and then α = 90 ° and β = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, Strength of 8 points of 330 ° is improved.

α=80°である8箇所の方位の強度が全て1.0以上であれば磁気特性は向上するが、α=90°である8箇所の方位の強度が全て1.0以上であればより良好な磁気特性が得られる。   The magnetic characteristics are improved if the strength of all eight orientations where α = 80 ° is 1.0 or more, but more if the strength of all eight orientations where α = 90 ° is 1.0 or more. Good magnetic properties can be obtained.

磁性の向上効果はα=90°の8点の強度が向上する方が著しいが、実用的にはα=80°の8点の集積度向上がより容易であるため、まず請求項2ではα=80°の8点についてその強度を定め、次に請求項3ではより好ましい磁気特性が得られる集合組織としてα=80°の8点およびα=90°の8点についてその強度を定めた。   The effect of improving the magnetism is more remarkable when the strength at 8 points of α = 90 ° is improved. However, practically, it is easier to improve the degree of integration at 8 points of α = 80 °. The strengths were determined for 8 points of 80 ° = 80 °, and in claim 3, the strengths were determined for 8 points of α = 80 ° and 8 points of α = 90 ° as textures for obtaining more preferable magnetic properties.

また、無方向性電磁鋼板の加工性を改善するために、図2に示した鋼板の板厚方向中心層2分の1層の(100)極点図において50°≦α≦70°かつβがそれぞれβ=0°、60°、120°、180°、240°、300°で定められる6箇所のすべてにおいて強度が1.0以上である領域が存在する必要がある。   Further, in order to improve the workability of the non-oriented electrical steel sheet, 50 ° ≦ α ≦ 70 ° and β in the (100) pole figure of the half layer thickness direction center layer of the steel plate shown in FIG. It is necessary that there is a region having an intensity of 1.0 or more at all of the six locations defined by β = 0 °, 60 °, 120 °, 180 °, 240 °, and 300 °, respectively.

図2ではこれら6箇所の領域を両端矢印にて示した。これにより無方向性電磁鋼板の打ち抜き加工時のカエリの増加を抑制でき、打ち抜き後の真円度が向上し、曲げ加工、絞り加工などにおける形状凍結性、r値などが向上するので磁気特性と加工性の両方に優れた無方向性電磁鋼板が得られる。   In FIG. 2, these six regions are indicated by double-ended arrows. As a result, an increase in burrs during punching of a non-oriented electrical steel sheet can be suppressed, the roundness after punching can be improved, and the shape freezing property, r value, etc. in bending and drawing can be improved. A non-oriented electrical steel sheet excellent in both workability can be obtained.

この目的のため、本発明では鋼板の板厚方向中心層2分の1層の(100)極点図において50°≦α≦70°かつβがそれぞれβ=0°、60°、120°、180°、240°、300°で定められる6箇所すべての領域に強度が1.0以上の領域が存在すると定める。図2にこれら6箇所の領域を両端矢印で示した。   For this purpose, in the present invention, 50 ° ≦ α ≦ 70 ° and β is β = 0 °, 60 °, 120 °, 180 in the (100) pole figure of the half layer in the thickness direction center layer of the steel sheet. It is determined that there are regions having an intensity of 1.0 or more in all the six regions defined at °, 240 °, and 300 °. In FIG. 2, these six regions are indicated by double-ended arrows.

鋼板の板厚方向中心層2分の1層の(100)極点図上のこれら6箇所の一部もしくは全箇所の領域において強度が1.0に満たない場合は打ち抜き加工時のカエリが増大し、真円度が低下し、曲げ加工、絞り加工などにおける形状凍結性、r値が低下し加工が困難となるので6箇所全てにおいて1.0以上の値の領域が存在する必要がある。   If the strength is less than 1.0 in some or all of these six regions on the (100) pole figure of the (100) pole figure of the center layer in the plate thickness direction of the steel sheet, the burr at the time of punching increases. Further, since the roundness is lowered, the shape freezing property in bending work, drawing work, etc., and the r value is lowered to make the work difficult, it is necessary to have a region having a value of 1.0 or more in all 6 places.

本発明は無方向性電磁鋼板の表層付近の集合組織を鋼板内の磁束の流れを円滑にする方位が優位となるように制御することが磁気特性改善に有効であることを見出した点に特徴がある。その際、鋼板表層において{100}方位のみならず{411}方位、{310}方位の集積度向上が有効であることを見出した。   The present invention is characterized in that it is effective in improving magnetic properties to control the texture in the vicinity of the surface layer of a non-oriented electrical steel sheet so that the orientation that smoothes the flow of magnetic flux in the steel sheet is superior. There is. In that case, it discovered that the integration degree improvement of {411} azimuth | direction and {310} azimuth | direction was effective not only in {100} azimuth | direction in steel plate surface layer.

さらに、特定の方位の絶対強度のみならず、特定方位の強度の和と、他の特定方位の強度の和との比を一定範囲に制御することで無方向性電磁鋼板の磁性が改善される新規な知見を見出した。   Furthermore, the magnetic properties of non-oriented electrical steel sheets can be improved by controlling the ratio of the sum of the strengths of a specific orientation and the sum of the strengths of other specific orientations within a certain range as well as the absolute strength of a specific orientation. I found new findings.

すなわち、無方向性電磁鋼板において優れた磁気特性を達成する集合組織として、X線回折による逆極点図の測定にて(100)面、(411)面、(111)面の強度をそれぞれI(100)、I(411)、I(111)とすると、鋼板の表面から板厚方向10分の1層の集合組織において、I(100)≧2.0かつ、I(411)≧1.5かつ、I(111)≦4.0かつ、{I(100)+I(411)}/I(111)≧1.0を満たす場合に磁気特性が優れることを見出した。   That is, as a texture that achieves excellent magnetic properties in a non-oriented electrical steel sheet, the strengths of the (100) plane, (411) plane, and (111) plane are measured as I ( 100), I (411), and I (111), I (100) ≧ 2.0 and I (411) ≧ 1.5 in the texture of 1/10 layer from the surface of the steel plate in the thickness direction. In addition, it has been found that the magnetic properties are excellent when I (111) ≦ 4.0 and {I (100) + I (411)} / I (111) ≧ 1.0.

さらに、(310)面、(332)面、(211)面、(221)面の強度をそれぞれI(310)、I(332)、I(211)、I(221)とすると、鋼板の表面から板厚方向10分の1層の集合組織において、I(100)≧2.0かつ、I(411)≧1.5かつ、I(111)≦4.0かつ、{I(100)+I(411)+I(310)}/{I(111)+I(332)+I(211)+I(221)} ≧0.5を満たす場合に磁気特性が優れることを見出した。   Further, when the strengths of the (310) plane, (332) plane, (211) plane, and (221) plane are I (310), I (332), I (211), and I (221), respectively, In the texture of 1/10 layer from the sheet thickness direction, I (100) ≧ 2.0, I (411) ≧ 1.5, I (111) ≦ 4.0, and {I (100) + I It has been found that when (411) + I (310)} / {I (111) + I (332) + I (211) + I (221)} ≧ 0.5, the magnetic characteristics are excellent.

なお、bcc鉄では(100)面、(111)面、(221)面の構造因子が零となるため、2次の回折面である(200)面、(222)面、(442)面をそれぞれ測定する。面指数としてはそれぞれ(100)、(111)、(221)を用いる。   In bcc iron, the structural factors of the (100), (111), and (221) planes are zero, so the (200), (222), and (442) planes are the second-order diffraction planes. Measure each. As the surface index, (100), (111), and (221) are used, respectively.

鋼板の表面から10分の1層の集合組織において{I(100)+I(411)}/I(111)の値が1.0未満であると鉄損が増大し、磁束密度が低下するため{I(100)+I(411)}/I(111)の値は1.0以上であることが好ましい。   If the {I (100) + I (411)} / I (111) value is less than 1.0 in the 1/10 layer texture from the surface of the steel sheet, the iron loss increases and the magnetic flux density decreases. The value of {I (100) + I (411)} / I (111) is preferably 1.0 or more.

さらに、鋼板の表面から10分の1層の集合組織において{I(100)+I(411)+I(310)}/{I(111)+I(332)+I(211)+I(221)}の値が0.5未満であると、鉄損が増加し磁束密度が低下するため、0.5以上であることが好ましい。   Furthermore, {I (100) + I (411) + I (310)} / {I (111) + I (332) + I (211) + I (221)} in a 1/10 layer texture from the surface of the steel plate Is less than 0.5, the iron loss increases and the magnetic flux density decreases, so it is preferably 0.5 or more.

鋼板表面から10分の1層の集合組織においてI(100)およびI(411)の値がそれぞれ2.0未満および1.5未満であると磁束密度が低下するのでそれぞれ2.0以上および1.5以上であることが好ましい。また、I(111)の値が4.0超であると磁束密度が低下するので4.0以下であることが好ましい。   If the I (100) and I (411) values are less than 2.0 and less than 1.5 in the 1/10 layer texture from the surface of the steel sheet, the magnetic flux density decreases. .5 or more is preferable. Further, if the value of I (111) is more than 4.0, the magnetic flux density is lowered, so that it is preferably 4.0 or less.

これらの方位間の強度の関係が磁気特性に及ぼす効果については、表層付近の{100}、{411}および{310}方位の集積を高めることにより、表層付近の結晶粒が無方向性電磁鋼板の板面垂直方向の磁化を抑制し鋼板内の磁束の流れが円滑となるため、鉄損、磁束密度などの磁気特性が向上すると推察している。   Regarding the effect of the strength relationship between these orientations on the magnetic properties, by increasing the accumulation of {100}, {411} and {310} orientations near the surface layer, the crystal grains near the surface layer become non-oriented electrical steel sheets. It is assumed that the magnetic properties such as iron loss and magnetic flux density are improved because the magnetization in the direction perpendicular to the plate surface is suppressed and the flow of magnetic flux in the steel plate becomes smooth.

また、{100}方位と{411}方位の強度が不足すると、磁気特性の改善に有効な方位を有する結晶の絶対的な集積量が不足し、本発明が目的とする磁気特性の改善効果が得られないと推察している。   Further, if the strength of {100} orientation and {411} orientation is insufficient, the amount of crystals that have an effective orientation for improving magnetic properties is insufficient, and the magnetic property improvement effect of the present invention is not achieved. I guess I can't get it.

また、これにより、インバータなどの高周波での励磁下において表皮効果により磁束が鋼板表層に偏在する場合においても、鋼板表層の集合組織が改善されたことにより鋼板内の磁束の流れが円滑となり、高周波で優れた磁気特性を実現することが可能になったと推察している。   In addition, even when magnetic flux is unevenly distributed on the steel sheet surface due to the skin effect under high frequency excitation such as an inverter, the flow of magnetic flux in the steel sheet becomes smooth due to the improved texture of the steel sheet surface layer. It is speculated that it has become possible to achieve excellent magnetic properties.

本発明の無方向性電磁鋼板の磁束密度をさらに高める方法として、発明者らは冷間圧延工程における圧延率を適切に制御することが有効であることを見出した。すなわち、磁束密度向上の効果は85%以上の冷間圧延率において著しく促進されるため、冷間圧延率は85%以上と定める。
一方、冷間圧延率を95%超とするためには冷間圧延設備の負担が大きくなり、コストが著しく上昇し不経済であるため、冷間圧延率の上限は95%以下と定める。
As a method for further increasing the magnetic flux density of the non-oriented electrical steel sheet of the present invention, the inventors have found that it is effective to appropriately control the rolling rate in the cold rolling process. That is, since the effect of improving the magnetic flux density is significantly promoted at a cold rolling rate of 85% or more, the cold rolling rate is set to 85% or more.
On the other hand, in order to make the cold rolling rate over 95%, the burden on the cold rolling equipment becomes large, the cost is remarkably increased, and it is uneconomical. Therefore, the upper limit of the cold rolling rate is set to 95% or less.

発明者らは、従来JIS(日本工業規格)で既定されてきたエプスタイン法では本発明の無方向性電磁鋼板の優れた特性を正確に測定していないことを見出した。すなわち、本発明ではエプスタイン法で採取する板の方向を圧延方向から鋼板板面内で左右に45度にした際に最もその磁気特性がすぐれ、かつ、左右の磁気特性がほぼ等しいことを見出したのである。   The inventors have found that the excellent properties of the non-oriented electrical steel sheet of the present invention are not accurately measured by the Epstein method that has been defined in JIS (Japanese Industrial Standard). That is, in the present invention, it has been found that when the direction of the plate collected by the Epstein method is 45 degrees to the left and right within the steel plate surface from the rolling direction, the magnetic properties are most excellent and the left and right magnetic properties are almost equal. It is.

従来のJIS規格のエプスタイン法では圧延方向とその直角方向から半々ずつ試料を切り出して圧延方向、直角方向、圧延方向、直角方向の順に閉磁路を作り、額縁状に重ね、電流法で励磁し磁気特性の測定を行う。しかしながら、本発明で製造された無方向性電磁鋼板は、鋼板の圧延方向とその直角方向は最も磁気特性の劣る方向であり、圧延方向から鋼板板面内で左右に45度それた方向が最も磁気特性が優れることを新規に見出した。   In the conventional JIS standard Epstein method, a sample is cut in half from the rolling direction and its perpendicular direction to create a closed magnetic path in the order of the rolling direction, the perpendicular direction, the rolling direction, and the perpendicular direction. Measure characteristics. However, in the non-oriented electrical steel sheet produced in the present invention, the rolling direction of the steel sheet and the direction perpendicular to the rolling direction are the directions in which the magnetic properties are inferior, and the direction deviated 45 degrees to the left and right within the steel sheet surface from the rolling direction is the most. It was newly found that the magnetic properties are excellent.

この新規の発見により、本発明では、鋼板を鉄心に加工する際の剪断時に、鉄心の磁束の流れる方向を鋼板の圧延方向から鋼板板面内で左右に45度傾いた方向に一致させる無方向性電磁鋼板の剪断を行う。   By this novel discovery, in the present invention, when shearing when processing a steel sheet into an iron core, the direction in which the magnetic flux of the iron core flows is non-directional to match the direction inclined 45 degrees to the left and right within the steel sheet surface from the rolling direction of the steel sheet Shears the electrical steel sheet.

鉄心内で磁束が流れる方向が鋼板の圧延方向から鋼板板面内で左右に45度傾いた方向からそれると、当該無方向性電磁鋼板を用いた製品の磁気特性を十分に活用することが出来ないので磁束が流れる方向と鋼板板面内で左右に45度傾いた方向は一致させるように鋼板を剪断する必要がある。   If the direction in which the magnetic flux flows in the iron core deviates from the rolling direction of the steel sheet from a direction inclined 45 degrees to the left and right within the steel sheet surface, the magnetic properties of the product using the non-oriented electrical steel sheet can be fully utilized. Since this is not possible, it is necessary to shear the steel sheet so that the direction in which the magnetic flux flows coincides with the direction inclined 45 degrees to the left and right within the steel sheet surface.

これにより製造した無方向性電磁鋼板を用い、磁束が流れる方向を鋼板の板面内で圧延方向から45度傾いた方向に合わせることにより、EIコア、回転機用分割コア、トランス用額縁鉄心、小型鉄心、リアクトル用鉄心、螺旋コアのヨークやティースの方向と本発明の無方向性電磁鋼板の磁化容易方向を一致させ、磁気特性の改善をはかることができる。   By using the non-oriented electrical steel sheet produced in this way, by adjusting the direction in which the magnetic flux flows to the direction inclined 45 degrees from the rolling direction within the plate surface of the steel sheet, the EI core, the rotary core split core, the transformer frame iron core, The direction of the small iron core, the core for the reactor, the yoke and teeth of the spiral core and the direction of easy magnetization of the non-oriented electrical steel sheet according to the present invention can be matched to improve the magnetic characteristics.

また、本発明で得られる無方向性電磁鋼板は圧延方向から板面内で左右に45度傾いた方向の磁気特性が最も優れているので、EIコア、回転機用分割コア、トランス用額縁鉄心、小型鉄心、リアクトル用鉄心、螺旋コアの内部の90度の角度をなすコーナー部にスムーズに磁束を流し、コーナー部の鉄損を減少させるとともに、90度の角度をなすヨークとティースの両方に同時にスムーズに磁束を流すことが可能になるという優れた性質を持つ。   Further, the non-oriented electrical steel sheet obtained by the present invention has the most excellent magnetic properties in a direction inclined 45 degrees to the left and right within the plate surface from the rolling direction. Therefore, the EI core, the split core for rotating machines, and the frame iron core for transformer Small magnetic cores, reactor cores, and smoothly flowing magnetic flux through the 90 ° corners inside the spiral core, reducing iron loss at the corners and reducing both the yoke and teeth at 90 ° angles At the same time, it has an excellent property of allowing a magnetic flux to flow smoothly.

これにより、本発明で製造した無方向性電磁鋼板を剪断する際に、鉄心の磁束が流れる方向に一致するように鋼板の圧延方向から板面内に左右に45度傾いた方向を一致させ、これを素材とすることにより、優れた磁気特性を持つEIコア、回転機用分割コア、トランス用額縁鉄心、小型鉄心、リアクトル用鉄心、螺旋コアを得ることが出来る。   Thereby, when shearing the non-oriented electrical steel sheet produced in the present invention, the direction inclined 45 degrees from side to side in the plate surface from the rolling direction of the steel sheet to match the direction in which the magnetic flux of the iron core flows, By using this as a raw material, it is possible to obtain an EI core having excellent magnetic properties, a split core for a rotating machine, a frame iron core for a transformer, a small iron core, a core for a reactor, and a spiral core.

本発明で得られた無方向性電磁鋼板の磁気特性が圧延方向から板面内で左右に45度傾いた方向で最も優れる理由については、図1の極点図からは現在のところ説明できない。この点については発明者らは鋭意調査中であるが、現在のところ以下のように推察している。   The reason why the magnetic properties of the non-oriented electrical steel sheet obtained in the present invention are most excellent in the direction inclined 45 degrees to the left and right within the plate surface from the rolling direction cannot be explained from the pole figure of FIG. The inventors have been diligently investigating this point, but currently infer as follows.

本発明で優れた磁気特性が得られる理由は図1の極点図に示したように表層の集合組織において板面に平行に近い方向に<100>軸が存在していることと発明者らは推察している。一方、中心層の集合組織は図2に示したように、難磁化方位である<111>が板面に平行に存在するため、本発明の磁気特性改善に対する寄与はほとんどないものと推察している。   The reason why excellent magnetic properties can be obtained in the present invention is that, as shown in the pole figure of FIG. 1, in the texture of the surface layer, the <100> axis exists in a direction almost parallel to the plate surface. I guess. On the other hand, as shown in FIG. 2, the texture of the central layer is inferior to the magnetic property improvement of the present invention because <111>, which is a hard magnetization orientation, exists in parallel to the plate surface. Yes.

ここで、極点図と多結晶体の磁化について説明を加えると、極点図は多結晶の結晶粒の方位分布を示すものであり、多結晶の鋼板内の個々の結晶粒内の磁束の流れを示すものではない。従って、図1で示された結晶方位分布の多結晶体からなる無方向性電磁鋼板では、個々の結晶の磁束の流れの総和として、未だ明らかでないが、磁化の静磁エネルギーの総和などが何らかの理由により45度方向が最小になるなどの理由で、板面内で45度方向の磁気特性が最も優れているものと推察している。   Here, when explaining the pole figure and the magnetization of the polycrystalline body, the pole figure shows the orientation distribution of the polycrystalline grains, and the flow of magnetic flux in the individual grains in the polycrystalline steel sheet is shown. It is not shown. Therefore, in the non-oriented electrical steel sheet made of the polycrystalline material having the crystal orientation distribution shown in FIG. 1, the total sum of the magnetic flux flows of the individual crystals is not yet clear, but the sum of the magnetostatic energy of magnetization is not It is presumed that the magnetic properties in the 45 degree direction are the best in the plate surface because the 45 degree direction is minimized for some reason.

次に、本発明の実施例について述べる。 Next, examples of the present invention will be described.

表1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800℃1時間加熱し、熱延により2.5mmに仕上げた。仕上熱延開始温度は750℃とした。圧延速度と熱延スタンド間の冷却速度を制御し仕上熱延終了温度を500℃から730℃の範囲で変化させた。なお、この鋼のAr1変態点は880℃である。
続いて酸洗を施し、冷間圧延により0.5mmに仕上げ、これを連続焼鈍炉にて750℃30秒の仕上焼鈍を施した。その後、エプスタイン試料に切断し、磁気特性を測定した。
A slab for non-oriented electrical steel having the components shown in Table 1 was heated at 800 ° C. for 1 hour by a normal method and finished to 2.5 mm by hot rolling. The finishing hot rolling start temperature was 750 ° C. The finishing hot rolling end temperature was changed in the range of 500 ° C. to 730 ° C. by controlling the rolling rate and the cooling rate between the hot rolling stands. The Ar1 transformation point of this steel is 880 ° C.
Subsequently, pickling was performed, and the product was finished to 0.5 mm by cold rolling, and this was subjected to finish annealing at 750 ° C. for 30 seconds in a continuous annealing furnace. Then, it cut | disconnected to the Epstein sample and measured the magnetic characteristic.

表1に成分を、表2に仕上熱延終了温度と磁気特性の関係の測定結果を示す。
表2より、仕上熱延終了温度を適切に制御することにより、熱延板焼鈍などのコストのかかる工程を省略して、高磁束密度の無方向性電磁鋼板を製造することが可能である。
Table 1 shows the components, and Table 2 shows the measurement results of the relationship between the finish hot rolling end temperature and the magnetic properties.
From Table 2, it is possible to manufacture a non-oriented electrical steel sheet having a high magnetic flux density by appropriately controlling the finishing hot rolling end temperature and omitting costly processes such as hot-rolled sheet annealing.

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

また、表2に示した本発明3の試料からX線回折用試料を作成し、表層から板厚方向10分の1層および、表層から板厚方向2分の1層を研磨により露出させX線回折測定を行い、(100)完全極点図を作成した。その結果を図3および図4にそれぞれ示す。
図3に示した鋼板の表層から10分の1層の(100)極点図では{411}<148>方位付近の集積が高い。
Further, a sample for X-ray diffraction was prepared from the sample of the present invention 3 shown in Table 2, and 1/10 layer in the plate thickness direction from the surface layer and 1/2 layer in the plate thickness direction were exposed by polishing to expose X layer. A line diffraction measurement was performed to create a (100) complete pole figure. The results are shown in FIGS. 3 and 4, respectively.
In the (100) pole figure of one-tenth layer from the surface layer of the steel plate shown in FIG. 3, the accumulation near the {411} <148> orientation is high.

さらに{411}<148>から極点図外周の{100}<012>方位付近に至るまで強度分布が高い領域が存在し、極点図外周において{100}<012>面付近の強度は1.0もしくは1.5に到達し、キューブ方位である{100}面が富化している。{411}<148>方位付近においてはその3箇所が最大強度2.5を越え、1箇所が最大強度2.0を越えている。   Further, there is a region having a high intensity distribution from {411} <148> to the vicinity of the {100} <012> orientation on the outer periphery of the pole figure, and the intensity near the {100} <012> plane is 1.0 on the outer periphery of the pole figure. Alternatively, it reaches 1.5 and the {100} plane that is the cube orientation is enriched. In the vicinity of the {411} <148> orientation, the three locations exceed the maximum strength of 2.5, and one location exceeds the maximum strength of 2.0.

図4に示した鋼板の中心層である2分の1層の(100)極点図では、ガンマファイバーと称される{111}面が鋼板面に平行でかつ鋼板面に垂直な<111>軸まわりに回転する結晶方位群により形成された集合組織が発達しており、極点図上ではα=54.7°付近に同心円状に強度の高い領域が現れている。その中でも特に6つの{111}<112>方位付近の集積が高く最大強度がいずれも1.0以上である特徴がある。   In the (100) pole figure of the half layer, which is the center layer of the steel sheet shown in FIG. 4, the {111} axis called gamma fiber is parallel to the steel sheet surface and perpendicular to the steel sheet surface. A texture formed by crystal orientation groups rotating around has developed, and on the pole figure, a high strength region appears concentrically around α = 54.7 °. Among them, there is a feature that the accumulation in the vicinity of the six {111} <112> orientations is particularly high and the maximum intensity is 1.0 or more.

極点図内の個別の強度分布の特徴について述べると、図3に示した鋼板の表面から板厚方向10分の1層の(100)極点図においては、α=80°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°における強度がすべて1.0以上であり、かつ、同一極点図上のα=90°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°における強度がすべて1.0以上であり、かつ、図4に示した鋼板の板厚方向中心層2分の1層の(100)極点図において、50°≦α≦70°かつβがそれぞれβ=0°、60°、120°、180°、240°、300°のα、βで定められる6箇所の全ての範囲に強度が1.0以上である領域が存在する特徴がある。   The characteristics of the individual intensity distribution in the pole figure will be described. In the (100) pole figure in the thickness direction of 1/10 from the surface of the steel sheet shown in FIG. 3, α = 80 ° and β is β = The strengths at 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, and 330 ° are all 1.0 or more, and α = 90 ° and β is β on the same pole figure, respectively. = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, 330 ° All strengths are 1.0 or more, and the thickness direction central layer 2 of the steel sheet shown in FIG. In the (100) pole figure of one-layer, 50 ° ≦ α ≦ 70 ° and β is defined by α and β of β = 0 °, 60 °, 120 °, 180 °, 240 °, and 300 °, respectively 6 There is a feature that a region having an intensity of 1.0 or more exists in the entire range of the portion.

このように本発明では鋼板の表層付近でキューブ方位付近に結晶方位が集積しているのに対し、鋼板中心層ではガンマファイバー集合組織が発達しており、鋼板表層と鋼板中心層の集合組織が大きく異なることが新規な特徴である。   As described above, in the present invention, the crystal orientation is accumulated near the cube orientation near the surface layer of the steel sheet, whereas the gamma fiber texture is developed in the steel sheet center layer, and the texture of the steel sheet surface layer and the steel sheet center layer is A big difference is a new feature.

本発明に開示した方法で製造した無方向性電磁鋼板と従来技術で製造した無方向性電磁鋼板の加工性について比較するため、表1に示した供試材のスラブを1150℃にて1時間加熱し、仕上げ熱延開始温度を1000℃とし、仕上熱延終了温度を860℃として2.5mmの熱延板に仕上げた。続いて酸洗を施し、冷間圧延により0.5mmに仕上げ、これを連続焼鈍炉にて750℃30秒の仕上焼鈍を施した。この試料を比較例2とした。その後、エプスタイン試料に切断し、磁気特性を測定した。   In order to compare the workability of the non-oriented electrical steel sheet produced by the method disclosed in the present invention and the non-oriented electrical steel sheet produced by the conventional technique, the slabs of the test materials shown in Table 1 were used at 1150 ° C. for 1 hour. Heating was performed, and the finish hot rolling start temperature was set to 1000 ° C. and the finish hot rolling end temperature was set to 860 ° C. to finish a 2.5 mm hot rolled sheet. Subsequently, pickling was performed, and the product was finished to 0.5 mm by cold rolling, and this was subjected to finish annealing at 750 ° C. for 30 seconds in a continuous annealing furnace. This sample was referred to as Comparative Example 2. Then, it cut | disconnected to the Epstein sample and measured the magnetic characteristic.

比較例1、比較例2の無方向性電磁鋼板および本発明により製造した無方向性電磁鋼板である本発明1から本発明5を用い真円の金型により直径100mmの形状に打ち抜き試験を行った所、打ち抜き回数50万回後に本発明の試料の端部のカエリ高さは20μm以下を示したのに対し、比較例1、比較例2では端部のカエリ高さは20μm超となった。   A non-oriented electrical steel sheet of Comparative Example 1 and Comparative Example 2 and a non-oriented electrical steel sheet manufactured according to the present invention were subjected to a punching test into a shape having a diameter of 100 mm using a perfect circle mold according to Inventions 1 to 5. On the other hand, the edge height of the edge of the sample of the present invention was 20 μm or less after 500,000 times of punching, whereas the edge height of the edge in Comparative Example 1 and Comparative Example 2 exceeded 20 μm. .

また同時に真円度を測定した所、比較例1、比較例2では真円度は35μm超の値を示したのに対し、本発明1から本発明5では35μm以下にとどまり良好な値を示した。真円度の測定は、打ち抜き回数50万回後に、打ち抜いた直径100mmの円形の試料に内接する真円と外接する真円の直径の差を単位をμmとして表した。
これらの結果を表2にあわせて示す。
Further, when the roundness was measured at the same time, in Comparative Examples 1 and 2, the roundness was more than 35 μm, while in the present invention 1 to the present invention 5, it was only 35 μm or less and showed a good value. It was. For the measurement of roundness, the difference between the diameters of a perfect circle inscribed and circumscribed in a round sample having a diameter of 100 mm after punching out of 500,000 times was expressed in μm.
These results are also shown in Table 2.

以上のように本発明により製造した無方向性電磁鋼板はSi添加量が0.3%の無方向性電磁鋼板としては極めて低いかえり高さと良好な真円度を示し優れた加工性を有している。   As described above, the non-oriented electrical steel sheet produced according to the present invention has extremely low burr height and good roundness and excellent workability as a non-oriented electrical steel sheet containing 0.3% of Si. ing.

本発明により鋼板表層においてキューブ方位付近の集積を高めることが可能であるため、鋼板を励磁した際に鋼板表面に対し垂直な磁化成分を減少させることが可能となり鉄損低減に有効であり、鋼板中心層でガンマファイバー集合組織の集積を高めることが可能であるため、加工性に優れた無方向性電磁鋼板を製造することが可能である。   According to the present invention, it is possible to increase the accumulation in the vicinity of the cube orientation in the steel sheet surface layer, so that when the steel sheet is excited, it is possible to reduce the magnetization component perpendicular to the steel sheet surface, which is effective in reducing iron loss. Since it is possible to increase the accumulation of gamma fiber texture in the central layer, it is possible to produce a non-oriented electrical steel sheet with excellent workability.

表3に示した鋼2の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750℃1時間加熱し、熱延により2.5mmに仕上げた。仕上熱延開始温度は600℃から740℃の範囲で変化させた。圧延速度と熱延スタンド間の冷却速度を制御し仕上熱延終了温度は560℃とした。
なお、この鋼のAr1変態点は867℃である。
The slab for non-oriented electrical steel having the components of Steel 2 shown in Table 3 was heated at 750 ° C. for 1 hour by a normal method, and finished to 2.5 mm by hot rolling. The finishing hot rolling start temperature was changed in the range of 600 ° C to 740 ° C. The finishing hot rolling finish temperature was set to 560 ° C. by controlling the rolling speed and the cooling speed between the hot rolling stands.
The Ar1 transformation point of this steel is 867 ° C.

sol-Alは製鋼段階でAl脱酸やAl添加を実施していないため検出限界以下であった。本実験で使用した分析機器ではsol-Alの検出限界は0.001%であり、この限界量以下と判定されたsol-Alについては表中において「tr.」と記載した。以下の実施例でも同様である。   Since sol-Al was not subjected to Al deoxidation or Al addition at the steelmaking stage, it was below the detection limit. In the analytical instrument used in this experiment, the detection limit of sol-Al was 0.001%, and sol-Al determined to be below this limit amount was described as “tr.” In the table. The same applies to the following embodiments.

続いて酸洗を施し、冷間圧延により0.5mmに仕上げ、これを連続焼鈍炉にて750℃30秒の仕上焼鈍を施した。その後、エプスタイン試料に切断し、磁気特性を測定した。   Subsequently, pickling was performed, and the product was finished to 0.5 mm by cold rolling, and this was subjected to finish annealing at 750 ° C. for 30 seconds in a continuous annealing furnace. Then, it cut | disconnected to the Epstein sample and measured the magnetic characteristic.

表3に成分を、表4に仕上熱延終了温度と磁気特性の関係の測定結果を示す。
表4より、仕上げ熱延開始温度を適切に制御することにより、熱延板焼鈍などのコストのかかる工程を省略して、高磁束密度の無方向性電磁鋼板を製造することが可能である。
Table 3 shows the components, and Table 4 shows the measurement results of the relationship between the finish hot rolling end temperature and the magnetic properties.
From Table 4, it is possible to manufacture a non-oriented electrical steel sheet having a high magnetic flux density by appropriately controlling the finishing hot rolling start temperature and omitting costly processes such as hot rolled sheet annealing.

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

表5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800℃1時間加熱し、熱延により2.5mmに仕上げた。仕上熱延開始温度は780℃とし、圧延速度と熱延スタンド間の冷却速度の制御により仕上熱延終了温度を640℃に制御した。
これらの鋼のAr1変態点は865℃から878℃である。
A slab for non-oriented electrical steel having the components shown in Table 5 was heated at 800 ° C. for 1 hour by a normal method and finished to 2.5 mm by hot rolling. The finishing hot rolling start temperature was 780 ° C., and the finishing hot rolling end temperature was controlled to 640 ° C. by controlling the rolling speed and the cooling rate between the hot rolling stands.
The Ar1 transformation point of these steels is 865 ° C to 878 ° C.

次に酸洗を施し、冷間圧延により0.5mmに仕上げ、これを連続焼鈍炉にて750℃30秒の仕上焼鈍を施した。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5に本発明と比較例の成分を、表6に各供試材の磁気特性の測定結果を示す。
Next, pickling was performed and the product was finished to 0.5 mm by cold rolling, and this was subjected to finish annealing at 750 ° C. for 30 seconds in a continuous annealing furnace. Then, it cut | disconnected to the Epstein sample and measured the magnetic characteristic.
Table 5 shows the components of the present invention and the comparative example, and Table 6 shows the measurement results of the magnetic properties of each test material.

このようにC含有量を0.004%以下に制御し、仕上げ熱延条件を適切に制御することにより、熱延板焼鈍などのコストのかかる工程を省略し、高磁束密度の無方向性電磁鋼板を製造することが可能である。
さらに、表6より、特にC含有量が0.003%以下の場合において、磁束密度B50が1.8T超のより高い値が得られていることがわかる。さらに、C含有量が0.002%以下の場合において、B50の値が1.815T以上のより高い磁束密度が得られていることがわかる。
Thus, by controlling the C content to 0.004% or less and appropriately controlling the finish hot rolling conditions, costly processes such as hot-rolled sheet annealing are omitted, and high magnetic flux density non-directional electromagnetic It is possible to produce a steel plate.
Furthermore, it can be seen from Table 6 that, in particular, when the C content is 0.003% or less, the magnetic flux density B50 is higher than 1.8T. Furthermore, it can be seen that when the C content is 0.002% or less, a higher magnetic flux density with a B50 value of 1.815 T or more is obtained.

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

表7に示した鋼11の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1150℃1時間加熱し、熱延により2.5mmに仕上げた。仕上熱延開始温度は600℃から870℃の範囲で変化させた。圧延速度と熱延スタンド間の冷却速度を制御し仕上熱延終了温度は560℃とした。
なお、この鋼のAr1変態点は865℃である。
The slab for non-oriented electrical steel having the components of Steel 11 shown in Table 7 was heated at 1150 ° C. for 1 hour by a normal method and finished to 2.5 mm by hot rolling. The finishing hot rolling start temperature was changed in the range of 600 ° C to 870 ° C. The finishing hot rolling finish temperature was set to 560 ° C. by controlling the rolling speed and the cooling speed between the hot rolling stands.
The Ar1 transformation point of this steel is 865 ° C.

続いて酸洗を施し、冷間圧延により0.5mmに仕上げ、これを連続焼鈍炉にて750℃30秒の仕上焼鈍を施した。その後、エプスタイン試料に切断し、磁気特性を測定した。   Subsequently, pickling was performed, and the product was finished to 0.5 mm by cold rolling, and this was subjected to finish annealing at 750 ° C. for 30 seconds in a continuous annealing furnace. Then, it cut | disconnected to the Epstein sample and measured the magnetic characteristic.

表7に成分を、表8に仕上熱延終了温度と磁気特性の関係の測定結果を示す。   Table 7 shows the components, and Table 8 shows the measurement results of the relationship between the finish hot rolling end temperature and the magnetic properties.

表8より、仕上げ熱延開始温度を適切に制御することにより、熱延板焼鈍などのコストのかかる工程を省略しつつ高磁束密度の無方向性電磁鋼板を製造することが可能である。   From Table 8, it is possible to produce a high-flux-density non-oriented electrical steel sheet while omitting costly processes such as hot-rolled sheet annealing by appropriately controlling the finishing hot-rolling start temperature.

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

表9に示した鋼12の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900℃1時間加熱し、熱延により2.5mmに仕上げた。仕上熱延開始温度は600℃から870℃の範囲で変化させた。圧延速度と熱延スタンド間の冷却速度を制御し仕上熱延終了温度は560℃とした。
なお、この鋼のAr1変態点は868℃である。
The slab for non-oriented electrical steel having the components of steel 12 shown in Table 9 was heated at 900 ° C. for 1 hour by a usual method, and finished to 2.5 mm by hot rolling. The finishing hot rolling start temperature was changed in the range of 600 ° C to 870 ° C. The finishing hot rolling finish temperature was set to 560 ° C. by controlling the rolling speed and the cooling speed between the hot rolling stands.
The Ar1 transformation point of this steel is 868 ° C.

続いて酸洗を施し、冷間圧延により0.5mmに仕上げ、これを連続焼鈍炉にて750℃30秒の仕上焼鈍を施した。その後、エプスタイン試料に切断し、磁気特性を測定した。   Subsequently, pickling was performed, and the product was finished to 0.5 mm by cold rolling, and this was subjected to finish annealing at 750 ° C. for 30 seconds in a continuous annealing furnace. Then, it cut | disconnected to the Epstein sample and measured the magnetic characteristic.

表9に成分を、表10に仕上熱延終了温度と磁気特性の関係の測定結果を示す。
表10より、仕上げ熱延開始温度を適切に制御することにより、熱延板焼鈍などのコストのかかる工程を省略しつつ高磁束密度の無方向性電磁鋼板を製造することが可能である。
Table 9 shows the components, and Table 10 shows the measurement results of the relationship between the finish hot rolling finish temperature and the magnetic properties.
From Table 10, it is possible to manufacture a non-oriented electrical steel sheet having a high magnetic flux density while omitting costly processes such as hot-rolled sheet annealing by appropriately controlling the finish hot-rolling start temperature.

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

表11に示した鋼13の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870℃1時間加熱し、熱延により2.5mmに仕上げた。仕上熱延開始温度は600℃から860℃の範囲で変化させた。圧延速度と熱延スタンド間の冷却速度を制御し仕上熱延終了温度は565℃とした。
なお、この鋼のAr1変態点は866℃である。
The slab for non-oriented electrical steel having the components of Steel 13 shown in Table 11 was heated at 870 ° C. for 1 hour by a normal method and finished to 2.5 mm by hot rolling. The finishing hot rolling start temperature was changed in the range of 600 ° C to 860 ° C. The finishing hot rolling finish temperature was 565 ° C. by controlling the rolling speed and the cooling speed between the hot rolling stands.
The Ar1 transformation point of this steel is 866 ° C.

続いて酸洗を施し、冷間圧延により0.5mmに仕上げ、これを連続焼鈍炉にて750℃30秒の仕上焼鈍を施した。その後、エプスタイン試料に切断し、磁気特性を測定した。   Subsequently, pickling was performed, and the product was finished to 0.5 mm by cold rolling, and this was subjected to finish annealing at 750 ° C. for 30 seconds in a continuous annealing furnace. Then, it cut | disconnected to the Epstein sample and measured the magnetic characteristic.

表11に成分を、表12に仕上熱延終了温度と磁気特性の関係の測定結果を示す。
表12より、仕上げ熱延開始温度を適切に制御することにより、熱延板焼鈍などのコストのかかる工程を省略しつつ高磁束密度の無方向性電磁鋼板を製造することが可能である。
Table 11 shows the components, and Table 12 shows the measurement results of the relationship between the finish hot rolling end temperature and the magnetic properties.
From Table 12, it is possible to produce a high-flux-density non-oriented electrical steel sheet while omitting costly processes such as hot-rolled sheet annealing by appropriately controlling the finish hot-rolling start temperature.

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

表13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800℃1時間加熱し、熱延により2.5mmに仕上げた。仕上熱延開始温度は730℃とした。圧延速度と熱延スタンド間の冷却速度を制御し仕上熱延終了温度を620℃とした。
続いて酸洗を施し、冷間圧延により0.5mmに仕上げ、これを連続焼鈍炉にて各温度にて30秒の仕上焼鈍を施した。その後、エプスタイン試料に切断し、磁気特性を測定した。
A slab for non-oriented electrical steel having the components shown in Table 13 was heated at 800 ° C. for 1 hour by a usual method, and finished to 2.5 mm by hot rolling. The finishing hot rolling start temperature was 730 ° C. The finishing hot rolling end temperature was set to 620 ° C. by controlling the rolling speed and the cooling speed between the hot rolling stands.
Subsequently, pickling was performed, and it was finished to 0.5 mm by cold rolling, and this was subjected to a finish annealing for 30 seconds at each temperature in a continuous annealing furnace. Then, it cut | disconnected to the Epstein sample and measured the magnetic characteristic.

表13に本発明と比較例の成分を、表14に仕上焼鈍温度と磁気特性の関係の測定結果を示す。
表14より、本発明の成分範囲にSi、Al含有量を調節することにより高磁束密度の無方向性電磁鋼板を製造することが可能である。
Table 13 shows the components of the present invention and comparative examples, and Table 14 shows the measurement results of the relationship between the finish annealing temperature and the magnetic properties.
From Table 14, it is possible to produce a non-oriented electrical steel sheet having a high magnetic flux density by adjusting the Si and Al contents within the component ranges of the present invention.

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

表15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800℃1時間加熱し、熱延により2.5mmに仕上げた。仕上熱延開始温度は750℃とした。圧延速度と熱延スタンド間の冷却速度を制御し仕上熱延終了温度を630℃とした。
また、比較例3として、表15と同一成分のスラブを1150℃にて1時間加熱し、仕上げ熱延開始温度を1000℃とし、仕上熱延終了温度を860℃として2.5mmの熱延板に仕上げた。
The slab for non-oriented electrical steel having the components shown in Table 15 was heated at 800 ° C. for 1 hour by a usual method, and finished to 2.5 mm by hot rolling. The finishing hot rolling start temperature was 750 ° C. The finishing hot rolling end temperature was set to 630 ° C. by controlling the rolling rate and the cooling rate between the hot rolling stands.
As Comparative Example 3, a slab having the same components as in Table 15 was heated at 1150 ° C. for 1 hour, the finish hot rolling start temperature was 1000 ° C., the finish hot rolling end temperature was 860 ° C., and a 2.5 mm hot rolled plate. Finished.

続いて酸洗を施し、冷間圧延により0.5mmに仕上げ、これを連続焼鈍炉にて750℃30秒の仕上焼鈍を施した。その後、エプスタイン試料に切断し、磁気特性を測定した。
また、本発明例と比較例3の試料の表面から板厚方向10分の1層の集合組織をX線回折により逆極点図にて測定し各回折面の反射面強度を測定した。
Subsequently, pickling was performed, and the product was finished to 0.5 mm by cold rolling, and this was subjected to finish annealing at 750 ° C. for 30 seconds in a continuous annealing furnace. Then, it cut | disconnected to the Epstein sample and measured the magnetic characteristic.
Further, the texture of one-tenth layer in the thickness direction from the surface of the sample of the inventive example and the comparative example 3 was measured by an inverse pole figure by X-ray diffraction, and the reflection surface intensity of each diffraction surface was measured.

表15に本発明と比較例の成分を、表16に磁気特性測定結果を、表17にX線回折による集合組織の測定結果、表18および表19に集合組織の判定結果を示す。
表16より、本発明の製造方法により商用周波数で低鉄損高磁束密度であるとともに、商用周波数および高周波での鉄損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ことがわかる。
Table 15 shows the components of the present invention and comparative examples, Table 16 shows the magnetic property measurement results, Table 17 shows the texture measurement results by X-ray diffraction, and Tables 18 and 19 show the texture determination results.
From Table 16, it can be seen that the production method of the present invention can produce a non-oriented electrical steel sheet having low iron loss and high magnetic flux density at commercial frequencies and excellent iron loss at commercial frequencies and high frequencies. .

また、表18より、X線回折測定により得られた逆極点図における(100)面、(411)面、(111)面の強度をそれぞれI(100)、I(411)、I(111)とすると、本発明では鋼板の表面から板厚方向10分の1層の集合組織において、I(100)≧2.0かつ、I(411)≧1.5かつ、I(111)≦4.0かつ、{I(100)+I(411)}/I(111) ≧1.0を満たすことがわかる。   Also, from Table 18, the intensities of the (100) plane, (411) plane, and (111) plane in the inverted pole figure obtained by X-ray diffraction measurement are I (100), I (411), and I (111), respectively. Then, in the present invention, I (100) ≧ 2.0, I (411) ≧ 1.5, and I (111) ≦ 4. 0 and {I (100) + I (411)} / I (111) ≧ 1.0.

さらに、表19より、(310)面、(332)面、(211)面、(221)面の強度をそれぞれI(310)、I(332)、I(211)、I(221)とすると、本発明では鋼板の表面から板厚方向10分の1層の集合組織において、I(100)≧2.0かつ、I(411)≧1.5かつ、I(111)≦4.0かつ、{I(100)+I(411)+I(310)}/{I(111)+I(332)+I(211)+I(221)} ≧0.5を満たすことがわかる。   Furthermore, from Table 19, when the strengths of the (310) plane, (332) plane, (211) plane, and (221) plane are I (310), I (332), I (211), and I (221), respectively. In the present invention, I (100) ≧ 2.0, I (411) ≧ 1.5, and I (111) ≦ 4.0 in a 1/10 layer texture from the surface of the steel plate. {I (100) + I (411) + I (310)} / {I (111) + I (332) + I (211) + I (221)} ≧ 0.5.

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

表20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800℃1時間加熱し、熱延により2.0mmに仕上げた。仕上熱延開始温度は750℃とした。圧延速度と熱延スタンド間の冷却速度を制御し仕上熱延終了温度を630℃とした。
続いて酸洗を施し、冷間圧延により0.10mmから0.50mmに仕上げ、連続焼鈍炉にて750℃25秒の仕上焼鈍を施した。その後、エプスタイン試料に切断し、磁気特性を測定した。0.10mm以下の冷間圧延はコストが増加し採算性が低下するため実施しなかった。
The slab for non-oriented electrical steel having the components shown in Table 20 was heated by a normal method at 800 ° C. for 1 hour and finished to 2.0 mm by hot rolling. The finishing hot rolling start temperature was 750 ° C. The finishing hot rolling end temperature was set to 630 ° C. by controlling the rolling rate and the cooling rate between the hot rolling stands.
Subsequently, pickling was performed, finishing from 0.10 mm to 0.50 mm by cold rolling, and finish annealing at 750 ° C. for 25 seconds in a continuous annealing furnace. Then, it cut | disconnected to the Epstein sample and measured the magnetic characteristic. Cold rolling of 0.10 mm or less was not performed because the cost increased and the profitability decreased.

また、比較例4として、表20と同一成分のスラブを1150℃にて1時間加熱し、粗圧延後、仕上げ熱延開始温度を1000℃とし、仕上熱延終了温度を860℃として2.5mmの熱延板に仕上げ、これを冷間圧延率80%にて0.50mmに仕上げ、750℃25秒の仕上焼鈍を施した。その後、エプスタイン試料に切断し、磁気特性を測定した。   As Comparative Example 4, a slab having the same components as in Table 20 was heated at 1150 ° C. for 1 hour, and after rough rolling, the finish hot rolling start temperature was 1000 ° C., and the finish hot rolling end temperature was 860 ° C. and 2.5 mm. The hot-rolled sheet was finished to a thickness of 0.50 mm at a cold rolling rate of 80% and subjected to finish annealing at 750 ° C. for 25 seconds. Then, it cut | disconnected to the Epstein sample and measured the magnetic characteristic.

表21に磁気特性測定結果を示す。冷間圧延率を85%から95%に制御した本発明例では磁束密度B50の値が1.84T以上と優れた値を示している。また50Hzの商用周波数における鉄損であるW15/50の値も比較例よりも優れている。さらに高周波の400Hzかつ動作磁束密度が1.0Tでの鉄損であるW10/400の値もSi量0.15%の成分系の無方向性電磁鋼板としては優れた値を示している。
このような磁気特性の向上は、先に示した集合組織の測定結果から、成品の集合組織が従来技術よりも改善されたことが原因であると発明者らは推測している。
Table 21 shows the measurement results of magnetic characteristics. In the example of the present invention in which the cold rolling rate is controlled from 85% to 95%, the magnetic flux density B50 has an excellent value of 1.84 T or more. The value of W15 / 50, which is the iron loss at a commercial frequency of 50 Hz, is also superior to the comparative example. Furthermore, the value of W10 / 400, which is the iron loss at a high frequency of 400 Hz and an operating magnetic flux density of 1.0 T, is also an excellent value as a component-based non-oriented electrical steel sheet having a Si content of 0.15%.
The inventors speculate that the improvement in the magnetic properties is caused by the improvement of the texture of the product compared to the prior art based on the measurement results of the texture described above.

以上のように、表21より、冷間圧延率85%から95%において商用周波数で高磁束密度かつ低鉄損であるとともに、高周波においても鉄損の優れた無方向性電磁鋼板の製造が可能であることがわかる。   As described above, from Table 21, it is possible to produce a non-oriented electrical steel sheet with high magnetic flux density and low iron loss at commercial frequencies at a cold rolling rate of 85% to 95% and excellent iron loss at high frequencies. It can be seen that it is.

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

表22に示した成分を有する無方向性電磁鋼用スラブを用い、プロセスA鋼とプロセスB鋼を製造した。   Using a non-oriented electrical steel slab having the components shown in Table 22, process A steel and process B steel were produced.

プロセスA鋼として、表22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800℃1時間加熱し、熱延により2.0mmに仕上げた。仕上熱延開始温度は750℃とした。圧延速度と熱延スタンド間の冷却速度を制御し仕上熱延終了温度を630℃とした。
続いて酸洗を施し、冷間圧延により0.30mmに仕上げ、連続焼鈍炉にて750℃25秒の仕上焼鈍を施した。その後、圧延方向、圧延方向から22.5度左右に傾いた方向、圧延方向から左右に45度傾いた方向、圧延方向から67.5度の方向、圧延方向と直角に傾いた方向のエプスタイン試料に切断し、磁気特性を測定した。
As process A steel, a slab for non-oriented electrical steel having the components shown in Table 22 was heated by a normal method at 800 ° C. for 1 hour and finished to 2.0 mm by hot rolling. The finishing hot rolling start temperature was 750 ° C. The finishing hot rolling end temperature was set to 630 ° C. by controlling the rolling rate and the cooling rate between the hot rolling stands.
Subsequently, pickling was performed, and the film was finished to 0.30 mm by cold rolling, and finish annealing was performed at 750 ° C. for 25 seconds in a continuous annealing furnace. Thereafter, Epstein sample in the rolling direction, the direction inclined 22.5 degrees left and right from the rolling direction, the direction inclined 45 degrees left and right from the rolling direction, the direction 67.5 degrees from the rolling direction, and the direction inclined perpendicular to the rolling direction The magnetic properties were measured.

また、比較例として、プロセスB鋼を、表22と同一成分のスラブを1150℃にて1時間加熱し、粗圧延後、仕上げ熱延開始温度を1000℃とし、仕上熱延終了温度を860℃として2.0mmの熱延板に仕上げ、続いて酸洗を施し、0.30mmに仕上げ、750℃25秒の仕上焼鈍を施した。その後、上記と同じ角度のエプスタイン試料に切断し、磁気特性を測定した。   Further, as a comparative example, the process B steel was heated at 1150 ° C. for 1 hour with a slab having the same components as in Table 22, and after rough rolling, the finish hot rolling start temperature was 1000 ° C., and the finish hot rolling end temperature was 860 ° C. As a hot rolled sheet having a thickness of 2.0 mm, followed by pickling, finishing to 0.30 mm, and finishing annealing at 750 ° C. for 25 seconds. Then, it cut | disconnected to the Epstein sample of the same angle as the above, and measured the magnetic characteristic.

磁気特性の測定はJISに定められた圧延方向とその直角方向を用いた方法の他に、各剪断方向の試料のみを使った測定および、圧延方向から左右に45度傾いた試料を交互に重ね、測定した。試料の方向の表記は、22.5度の角度間隔で圧延方向に0°、右22.5°、左22.5°、右45°、左45°、右67.5°、左67.5°、90°で表した。   In addition to the method using the rolling direction specified by JIS and its perpendicular direction, the magnetic properties are measured using only samples in each shearing direction, and samples that are inclined 45 degrees to the left and right from the rolling direction are alternately stacked. ,It was measured. The notation of the direction of the sample is 0 °, 22.5 ° to the right, 22.5 ° to the left, 45 ° to the right, 45 ° to the left, 67.5 ° to the right and 67.5 ° to the left at an angle interval of 22.5 degrees. Expressed at 5 ° and 90 °.

予め調べたところ、右22.5°と左22.5°、右45°と左45°、右67.5°と左67.5°はほぼ同じ測定値を示し、圧延方向に対称であったので、右45°と左45°は個別に試料を採取したが、右22.5°と左22.5°は右22.5°、右67.5°と左67.5°は右67.5°の試料のみを採取し、右の表記は省略した。また、対辺に右45°、左45°を用い、JIS法の試料を45°回転させた状態での測定も行い、右45°+左45°と示した。   When examined beforehand, right 22.5 ° and left 22.5 °, right 45 ° and left 45 °, right 67.5 ° and left 67.5 ° showed almost the same measured values, and they were symmetrical in the rolling direction. Therefore, right 45 ° and left 45 ° samples were collected separately, right 22.5 ° and left 22.5 ° were right 22.5 °, right 67.5 ° and left 67.5 ° were right. Only a sample of 67.5 ° was collected, and the description on the right was omitted. In addition, measurement was performed with 45 ° right and 45 ° opposite to each other and a JIS sample rotated by 45 °, and the result was 45 ° right + 45 ° left.

表23に磁気特性測定結果を示す。
表23より本発明によれば優れた磁気特性が得られることがわかる。
Table 23 shows the measurement results of magnetic characteristics.
It can be seen from Table 23 that excellent magnetic properties can be obtained according to the present invention.

Figure 2011111658
Figure 2011111658

Figure 2011111658
Figure 2011111658

実施例10で製造したプロセスA鋼より、EIのIの向きを鋼板圧延方向と一致させて打ち抜いたEIコアと、EIのIの向きを鋼板圧延方向と45°の角度をなす方向から打ち抜いたEIコアを作成し、Eコアの3脚に励磁コイルを巻き、鉄損を測定した。真ん中の脚に接してHコイルを設置し、その上から励磁コイルを巻き、磁界を測定した。
本発明の方法で打ち抜いたEIコアと比較例の模式図を図5に示す。
From the process A steel produced in Example 10, the EI core was punched with the EI direction aligned with the steel plate rolling direction, and the EI I direction was punched from the direction forming an angle of 45 ° with the steel plate rolling direction. An EI core was prepared, and an exciting coil was wound around the three legs of the E core, and the iron loss was measured. An H coil was installed in contact with the middle leg, and an exciting coil was wound thereon to measure the magnetic field.
FIG. 5 shows a schematic diagram of an EI core punched by the method of the present invention and a comparative example.

また、トランス用額縁鉄心、小型トランス、リアクトル用鉄心、螺旋コアの磁気特性測定用に外形40mm×40mm、内側の開口部20mm×20mmの小型鉄心を打ち抜いた。その際、直角を成す鉄心の2方向の脚が鋼板の圧延方向とその板面内直角方向に一致する方法と、2方向の脚が鋼板圧延方向と45°を成す方向に打ち抜く2つの方法で鉄心を打ち抜いて2種類の鉄心を作成した。この鉄心に200ターンの巻き線を施して電流法で鉄損を測定した。
本発明の方法で打ち抜いた額縁コアと比較例の模式図を図6に示す。
Also, a transformer core iron, a small transformer, a reactor iron core, and a small iron core having an outer diameter of 40 mm × 40 mm and an inner opening of 20 mm × 20 mm were punched for measuring magnetic characteristics of the spiral core. At that time, the two-way leg of the iron core that forms a right angle coincides with the rolling direction of the steel sheet and the perpendicular direction in the plate surface, and the two-way leg punches in a direction that forms 45 ° with the rolling direction of the steel sheet. Two types of iron cores were created by punching the iron core. The iron core was wound with 200 turns, and the iron loss was measured by a current method.
FIG. 6 shows a schematic diagram of a frame core punched out by the method of the present invention and a comparative example.

次に、12スロットからなる外径150mmの分割コアを作成し、ティースに巻き線を施して組み立て、ロータを組み込み、一定の励磁磁界での鉄損を測定した。その際、分割コアのティースが鋼板の圧延方向と直角の方向に打ち抜いたものと、鋼板の圧延方向と45°の方向をなすように打ち抜いたものを用意した。
本発明の方法で打ち抜いた分割コアと比較例の模式図を図7に示す。
Next, a split core having an outer diameter of 150 mm consisting of 12 slots was prepared, and the teeth were wound and assembled, the rotor was incorporated, and the iron loss with a constant excitation magnetic field was measured. At that time, there were prepared one in which the teeth of the split core were punched in a direction perpendicular to the rolling direction of the steel sheet, and one in which the teeth were punched in a direction of 45 ° with the rolling direction of the steel sheet.
FIG. 7 shows a schematic diagram of a split core punched out by the method of the present invention and a comparative example.

次に、40スロットからなる外径120mm、積み厚15mmの螺旋コアを作成し、励磁時の鉄損を測定した。コアは40スロットからなるヨークを円形に加工した後、積層して製作した。打ち抜きの際はヨークが圧延方向、ティースが圧延方向と板面内で直角方向を成す打ち抜き方と、ヨーク、ティースともに圧延方向から板面内で45°の方向をなすうち抜きを行って磁気特性を比較した。
本発明の方法で打ち抜いた螺旋コアと比較例の模式図を図8に示す。
Next, a spiral core having an outer diameter of 120 mm and a stacking thickness of 15 mm consisting of 40 slots was prepared, and the iron loss during excitation was measured. The core was manufactured by processing a 40-slot yoke into a circular shape and then laminating it. When punching, magnetic properties are obtained by punching the yoke in the rolling direction, teeth forming a direction perpendicular to the rolling direction and the rolling direction, and both the yoke and teeth forming a 45 ° direction from the rolling direction to the plate surface. Compared.
FIG. 8 shows a schematic diagram of a spiral core punched out by the method of the present invention and a comparative example.

表24より、本発明の方法で打ち抜いた鉄心はいずれも優れた磁気特性を有することがわかる。   From Table 24, it can be seen that all iron cores punched by the method of the present invention have excellent magnetic properties.

Figure 2011111658
Figure 2011111658

Claims (7)

鋼中に質量%で、
0.1%≦Si≦2.0%、
Al≦1.0%、
かつ、0.1%≦Si+2Al≦2.0%を満たし、
C≦0.004%、
S≦0.003%、
N≦0.003%
を含有し、残部がFeおよび不可避的不純物からなる鋼をスラブとして、熱間圧延において粗圧延および引き続く仕上熱延を施して熱延板とし、酸洗し一回の冷間圧延工程を施し次いで仕上げ焼鈍を施す無方向性電磁鋼板の製造方法において、
熱間圧延のスラブ加熱温度ST、仕上熱延開始温度F0T、仕上熱延終了温度FTをそれぞれ以下のように定めることを特徴とする磁束密度の高い無方向性電磁鋼板の製造方法。
700℃≦ST≦1150℃
650℃≦F0T≦850℃
550℃≦FT≦800℃
% By weight in steel
0.1% ≦ Si ≦ 2.0%,
Al ≦ 1.0%,
And 0.1% ≦ Si + 2Al ≦ 2.0% is satisfied,
C ≦ 0.004%,
S ≦ 0.003%,
N ≦ 0.003%
Steel, the balance being Fe and unavoidable impurities as slabs, hot rolling to rough rolling and subsequent hot rolling to form hot rolled sheets, pickling and a single cold rolling step In the manufacturing method of the non-oriented electrical steel sheet that performs finish annealing,
A method for producing a non-oriented electrical steel sheet having a high magnetic flux density, characterized in that a slab heating temperature ST, a finishing hot rolling start temperature F0T, and a finishing hot rolling end temperature FT of hot rolling are determined as follows.
700 ℃ ≦ ST ≦ 1150 ℃
650 ℃ ≦ F0T ≦ 850 ℃
550 ℃ ≦ FT ≦ 800 ℃
鋼板の表面から板厚方向10分の1層においてX線回折測定により作成した(100)極点図において、
α=80°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°における強度がすべて1.0以上であり、
かつ、鋼板の板厚方向中心層2分の1層においてX線回折測定により測定した(100)極点図において、
50°≦α≦70°かつβがそれぞれβ=0°、60°、120°、180°、240°、300°で定められるα、βの領域に強度が1.0以上である領域が存在することを特徴とする無方向性電磁鋼板。
In the (100) pole figure created by X-ray diffraction measurement in 1 / 10th layer in the plate thickness direction from the surface of the steel plate,
α = 80 ° and β are respectively β = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, 330 °, and the strengths are all 1.0 or more,
And in the (100) pole figure measured by X-ray diffraction measurement in the half layer thickness direction center layer of the steel plate,
There is a region where the intensity is 1.0 or more in the regions of α and β where 50 ° ≦ α ≦ 70 ° and β is determined by β = 0 °, 60 °, 120 °, 180 °, 240 °, and 300 °, respectively. A non-oriented electrical steel sheet characterized by:
鋼板の表面から板厚方向10分の1層においてX線回折測定により作成した(100)極点図において、
α=80°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°における強度がすべて1.0以上、かつ、同一極点図上において、α=90°かつβがそれぞれβ=30°、60°、120°、150°、210°、240°、300°、330°における強度がすべて1.0以上であり、
かつ、鋼板の板厚方向中心層である2分の1層においてX線回折測定により作成した(100)極点図において、
50°≦α≦70°かつβがそれぞれβ=0°、60°、120°、180°、240°、300°で定められるα、βの領域に強度が1.0以上である領域が存在することを特徴とする無方向性電磁鋼板。
In the (100) pole figure created by X-ray diffraction measurement in 1 / 10th layer in the plate thickness direction from the surface of the steel plate,
α = 80 ° and β are β = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, 330 °, all of strengths of 1.0 or more, and on the same pole figure, α = 90 ° and β are respectively β = 30 °, 60 °, 120 °, 150 °, 210 °, 240 °, 300 °, 330 °, and the strengths are all 1.0 or more,
And in the (100) pole figure created by X-ray diffraction measurement in the half layer which is the center layer in the plate thickness direction of the steel plate,
There is a region where the intensity is 1.0 or more in the regions of α and β where 50 ° ≦ α ≦ 70 ° and β is determined by β = 0 °, 60 °, 120 °, 180 °, 240 °, and 300 °, respectively. A non-oriented electrical steel sheet characterized by:
鋼板の表面から板厚方向10分の1層においてX線回折測定により得られた逆極点図における(100)面、(411)面、(111)面の強度を、それぞれI(100)、I(411)、I(111)とすると、
I(100)≧2.0
I(411)≧1.5
I(111)≦4.0
かつ、
{I(100)+I(411)}/I(111) ≧1.0
を満たすことを特徴とする無方向性電磁鋼板。
The strengths of the (100) plane, (411) plane, and (111) plane in the inverse pole figure obtained by X-ray diffraction measurement at 1 / 10th layer in the thickness direction from the surface of the steel sheet are I (100) and I (411), I (111)
I (100) ≧ 2.0
I (411) ≧ 1.5
I (111) ≦ 4.0
And,
{I (100) + I (411)} / I (111) ≧ 1.0
A non-oriented electrical steel sheet characterized by satisfying
請求項1に記載の無方向性電磁鋼板の製造方法において、冷間圧延における圧延率を85%以上95%以下とすることを特徴とする無方向性電磁鋼板の製造方法。   The method for producing a non-oriented electrical steel sheet according to claim 1, wherein a rolling rate in cold rolling is 85% or more and 95% or less. 請求項1または5に記載の無方向性電磁鋼板の製造方法によって製造された電磁鋼板あるいは請求項2〜4のいずれかに記載の電磁鋼板を鉄心に加工する際の剪断時に、鉄心の磁束の流れる方向を鋼板の圧延方向から鋼板板面内で左右に45度傾いた方向に一致させることを特徴とする無方向性電磁鋼板の剪断方法。   The magnetic steel sheet produced by the method for producing a non-oriented electrical steel sheet according to claim 1 or 5 or the magnetic steel sheet according to any one of claims 2 to 4 at the time of shearing when the magnetic steel sheet is processed into an iron core, A shearing method for a non-oriented electrical steel sheet, wherein the flowing direction is made to coincide with a direction inclined 45 degrees to the left and right within the steel sheet surface from the rolling direction of the steel sheet. 請求項6に記載の方法により製造した無方向性電磁鋼板により製造した電磁部品であって、該電磁部品が、EIコア、回転機用分割コア、トランス用額縁鉄心、小型鉄心、リアクトル用鉄心、螺旋コアのいずれかであることを特徴とする電磁部品。   An electromagnetic component manufactured by a non-oriented electrical steel sheet manufactured by the method according to claim 6, wherein the electromagnetic component is an EI core, a split core for a rotating machine, a frame iron core for a transformer, a small iron core, a core for a reactor, An electromagnetic component that is one of a spiral core.
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