JPH05263198A - Double-layered non-oriented silicon steel sheet excellent in magnetic property - Google Patents

Double-layered non-oriented silicon steel sheet excellent in magnetic property

Info

Publication number
JPH05263198A
JPH05263198A JP3345085A JP34508591A JPH05263198A JP H05263198 A JPH05263198 A JP H05263198A JP 3345085 A JP3345085 A JP 3345085A JP 34508591 A JP34508591 A JP 34508591A JP H05263198 A JPH05263198 A JP H05263198A
Authority
JP
Japan
Prior art keywords
steel sheet
surface layer
silicon steel
oriented silicon
frequency
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
JP3345085A
Other languages
Japanese (ja)
Inventor
Morio Shiozaki
守雄 塩崎
Takahide Shimazu
高英 島津
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nippon Steel Corp
Original Assignee
Nippon Steel Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP3345085A priority Critical patent/JPH05263198A/en
Publication of JPH05263198A publication Critical patent/JPH05263198A/en
Withdrawn legal-status Critical Current

Links

Abstract

PURPOSE:To provide a non-oriented silicon steel sheet simultaneously satisfying magnetic properties in low-frequency and high-frequency. CONSTITUTION:The objective double-layered non oriented silicon steel sheet excellent in magnetic properties is in which the components of the surface layer part are constituted of, by weight, <=0.005% C, 2.0 to 4.0% Si, 0.1 to 1.5% Mn, <=0.1% P, <=0.003% S, 0.05 to 2.0% Sol Al and <=0.003% N, and the balance Fe with inevitable impurities and the components of the internal layer part are constituted of <=0.005% C, <2.0% Si, 0.1 to 1.5% Mn, <=0.1% P, <=0.020% S, <=1.0% Sol Al and <=0.003% N, and the balance Fe with inevitable impurities, and in which the ratio of both surface layer part thickness internal layer part thickness is regulated to 0.1 to 0.6.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明はモータ及び小型トランス
用として一般に用いられる電気製品の素材であるが、特
に低周波〜高周波数での広い周波数領域で使われるイン
バータ用途および高周波用の無方向性電磁鋼板である。
この分野では例えば、インバータ制御エアコンや冷蔵庫
用モータ、電気自動車の駆動モータなどがある。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention is a material for electric products generally used for motors and small transformers, and is especially used for inverters used in a wide frequency range from low frequency to high frequency and non-directional for high frequencies. It is a magnetic steel sheet.
In this field, for example, there are inverter control air conditioners, refrigerator motors, drive motors for electric vehicles, and the like.

【0002】[0002]

【従来の技術】この分野は注目されており、インバータ
制御は電気機器のエネルギー効率向上に大いに利用され
ており、高周波用としての機器も増大している。これら
の電気機器に用いられる周波数は、20〜数kHz であり
中には高周波成分を重畳させて使っている。このよう
に、低周波〜高周波数の広い周波数領域に最適な無方向
性電磁鋼板は未だ市場にでていない。低周波に要求され
る特性は、小さなヒステリシス損と強い回転トルクを生
むための高い磁束密度である。また、高周波域に求めら
れるものは小さなうず電流損である。このように、一つ
の電気機器に要求される特性が周波数に応じて異なるが
ために従来、無方向性電磁鋼板に二つの特徴を兼ね備え
たものが不可能とされてきた。
2. Description of the Related Art In this field, attention has been paid to the fact that inverter control is widely used for improving the energy efficiency of electrical equipment, and the number of equipment for high frequencies is also increasing. The frequency used for these electric devices is 20 to several kHz, and high frequency components are superimposed and used. As described above, the non-oriented electrical steel sheet most suitable for a wide frequency range from low frequency to high frequency has not yet been put on the market. The characteristics required for low frequencies are a small hysteresis loss and a high magnetic flux density for producing a strong rotating torque. What is required in the high frequency range is a small eddy current loss. As described above, since the characteristics required for one electric device differ depending on the frequency, it has heretofore been impossible to use a non-oriented electrical steel sheet having two characteristics.

【0003】[0003]

【発明が解決しようとする課題】本発明者等は上記の点
に鑑み、無方向性電磁鋼板の1枚の鋼板において、低周
波と高周波数の両者への要求特性を同時に満足させるべ
く、複層の思想を新たに導入して発明を完成させた。こ
の無方向性電磁鋼板の特徴は低周波〜高周波の広い範囲
に優れた磁気特性を有する。
SUMMARY OF THE INVENTION In view of the above points, the inventors of the present invention have made a single steel sheet of a non-oriented electrical steel sheet a composite sheet in order to simultaneously satisfy the required characteristics for both low frequency and high frequency. The idea of layers was newly introduced to complete the invention. The characteristic of this non-oriented electrical steel sheet is that it has excellent magnetic characteristics in a wide range from low frequency to high frequency.

【0004】[0004]

【課題を解決するための手段】すなわち本発明は、重量
比で表層部の成分がC≦0.005%、Si:2.0〜
4.0%、Mn:0.1〜1.5%、P≦0.1%、S
≦0.003%、SolAl:0.05〜2.0%、N
≦0.003%、残部Feおよび不可避的不純物からな
り、内層部の成分がC≦0.005%、Si:2.0
%、Mn:0.1〜1.5%、P≦0.1%、S≦0.
020%、SolAl≦1.0%、N≦0.003%を
含有し、残部Feおよび不可避的不純物からなる複層鋼
板であり、上記、両表層部厚/内層部厚の比率が0.1
〜0.6であることを特徴とする磁気特性の優れた複層
無方向性電磁鋼板である。
That is, according to the present invention, in the weight ratio, the component of the surface layer portion is C ≦ 0.005%, Si: 2.0 to
4.0%, Mn: 0.1 to 1.5%, P ≦ 0.1%, S
≦ 0.003%, SolAl: 0.05 to 2.0%, N
≤0.003%, balance Fe and unavoidable impurities, and inner layer component C≤0.005%, Si: 2.0
%, Mn: 0.1 to 1.5%, P ≦ 0.1%, S ≦ 0.
020%, SolAl ≦ 1.0%, N ≦ 0.003%, and a multi-layer steel sheet comprising the balance Fe and unavoidable impurities, wherein the ratio of both surface layer thickness / inner layer thickness is 0.1.
It is a multi-layered non-oriented electrical steel sheet having excellent magnetic properties, which is characterized by being ˜0.6.

【0005】この発明の基本思想は、表皮効果と複層構
造を利用するにある。周知の如く、高周波領域では外部
磁界の浸透が減少する現象があり、表皮効果として知ら
れている。この時、鋼板内部の磁束Bが鋼板表面磁束B
oに対しB/Bo=1/eになる深さを表皮厚みと称す
るが、表皮厚みは周波数、鋼板透磁率と鋼板電気抵抗に
依存して変化する。即ち、高周波領域では磁束が表層に
多く流れ、うず電流損も表層で強く発生するため電気抵
抗の高い、つまりSiやAlの量の多い鋼板が有利であ
る。一方、低周波領域では全鉄損に占めるうず電流損の
割合が小さくヒステリシス損が支配し、また表皮効果が
弱いため磁束は鋼板をほぼ一様に貫通している。このと
きは鋼板内部の磁束密度を高める、つまり鋼板内層を低
Si、低Alにする方が優れたモータ効率が得られる。
The basic idea of the present invention is to utilize the skin effect and the multilayer structure. As is well known, there is a phenomenon that the penetration of an external magnetic field is reduced in a high frequency region, which is known as a skin effect. At this time, the magnetic flux B inside the steel plate is the magnetic flux B on the steel plate surface.
The depth at which B / Bo = 1 / e with respect to o is called the skin thickness. The skin thickness changes depending on the frequency, the steel sheet permeability and the steel sheet electrical resistance. That is, a large amount of magnetic flux flows in the surface layer in the high frequency region, and eddy current loss also strongly occurs in the surface layer, so a steel sheet having a high electric resistance, that is, a large amount of Si or Al is advantageous. On the other hand, in the low frequency region, the ratio of eddy current loss to total iron loss is small, hysteresis loss is dominant, and the skin effect is weak, so the magnetic flux penetrates the steel sheet almost uniformly. At this time, it is possible to obtain better motor efficiency by increasing the magnetic flux density inside the steel sheet, that is, by making the inner layer of the steel sheet low Si and low Al.

【0006】つまり、高周波域での低鉄損と低周波域で
の高磁束密度の両者を同時に満足させるのに必要なイン
バータ用モータなどには、外層部と内層部の成分組成を
制御させた複層鋼板が有利である。
That is, the composition of the outer layer and the inner layer is controlled in an inverter motor or the like which is required to satisfy both the low iron loss in the high frequency range and the high magnetic flux density in the low frequency range at the same time. Multi-layer steel sheets are advantageous.

【0007】以下、本発明を詳細に説明する。まず、成
分の限定理由について述べる。表層および内層のC量を
0.005%以下と限定したのは、これ以上のCでは磁
気時効劣化が生じるためである。表層のSi量を2.0
〜4.0%の範囲に限定したのは、うず電流損を抑え、
高周波での優れた鉄損を得るのに必要なSi量は少なく
とも2.0%以上であり、また、冷間脆性の問題から
4.0%が上限であるためである。一方、内層のSi量
を2.0%以下に限定したのは、低周波での優れた磁束
密度を得るために必要なためである。
The present invention will be described in detail below. First, the reasons for limiting the components will be described. The reason why the C content in the surface layer and the inner layer is limited to 0.005% or less is that the magnetic aging deterioration occurs at C content higher than this. The amount of Si in the surface layer is 2.0
Limiting the range to ~ 4.0% is to suppress eddy current loss,
This is because the Si amount required to obtain excellent iron loss at high frequencies is at least 2.0% or more, and 4.0% is the upper limit due to the problem of cold embrittlement. On the other hand, the reason for limiting the amount of Si in the inner layer to 2.0% or less is that it is necessary to obtain an excellent magnetic flux density at low frequencies.

【0008】表層と内層のMn量を0.1〜1.5%に
限定したのは、0.1%未満では微細なMnSが析出し
て鉄損を劣化させるためであり、また、添加コスト面か
ら1.5%を上限とした。表層と内層のP量を0.1%
以下に限定したのは、Pはうず電流損を低減する効果が
あるが添加コストの面から、0.1%を上限とした。表
層のS量を0.003%以下に限定したのは、硫化物が
高周波での鉄損を劣化させるからであり、0.003%
が上限である。また、内層のS量を0.020%以下に
限定したのは、硫化物が低周波での鉄損も劣化させるか
らである。
The amount of Mn in the surface layer and the inner layer is limited to 0.1 to 1.5% because if it is less than 0.1%, fine MnS is precipitated and iron loss is deteriorated. The upper limit was 1.5% from the viewpoint. 0.1% P content in the surface and inner layers
In the following, P has the effect of reducing the eddy current loss, but 0.1% was made the upper limit from the viewpoint of the addition cost. The amount of S in the surface layer is limited to 0.003% or less because sulfides deteriorate iron loss at high frequencies, and 0.003%
Is the upper limit. The reason for limiting the amount of S in the inner layer to 0.020% or less is that sulfides also deteriorate iron loss at low frequencies.

【0009】表層のSolAl量を0.05〜2.0%
に限定したのは、高周波での優れた鉄損を得るのに必要
なSolAl量は少なくとも0.05%以上であり、ま
た、添加コストの問題から2.0%が上限であるためで
ある。一方、内層のSolAl量を1.0%以下に限定
したのは、低周波域での鉄損をAlは改善するが、添加
コストの問題があるからである。表層と内層のN量を
0.003%以下に限定したのは、窒化物が鉄損を劣化
させるからであり0.003%が上限である。上記以外
の成分として、例えばAlNを減らすためBの添加や集
合組織改善の目的で粒界偏析型のSb,Snなどの添加
は本発明の趣旨を損なうものでない。次に、複層構造の
限定理由について述べる。両表層部厚/内層部厚の比率
を0.1〜0.6の範囲に限定したのは、比率が0.1
以下だと高周波領域で十分な低鉄損が得られないためで
ある。上限を0.6としたのは表層がこれ以上に厚い
と、比較的低周波数領域での用途に限定されるため複層
鋼板にまでする意味が少なくなるためである。ここでの
両表層部厚とは両面の表層部の厚みを足した値である。
The amount of SolAl in the surface layer is 0.05 to 2.0%
The reason for this is that the amount of SolAl required to obtain excellent iron loss at high frequencies is at least 0.05% or more, and 2.0% is the upper limit due to the problem of addition cost. On the other hand, the reason for limiting the amount of SolAl in the inner layer to 1.0% or less is that Al improves iron loss in the low frequency region, but there is a problem of addition cost. The reason why the N content in the surface layer and the inner layer is limited to 0.003% or less is that the nitride deteriorates the iron loss, and 0.003% is the upper limit. As components other than the above, for example, addition of B for reducing AlN or addition of grain boundary segregation type Sb, Sn, etc. for the purpose of improving texture does not impair the gist of the present invention. Next, the reasons for limiting the multilayer structure will be described. The ratio of both surface layer thickness / inner layer thickness is limited to the range of 0.1 to 0.6 because the ratio is 0.1.
This is because if it is below the range, sufficient low iron loss cannot be obtained in the high frequency region. The upper limit is set to 0.6 because if the surface layer is thicker than this, it is meaningless to make a multi-layer steel sheet because it is limited to applications in a relatively low frequency region. Here, the thickness of both surface layer portions is a value obtained by adding the thicknesses of the surface layer portions on both surfaces.

【0010】この複層鋼板の製造方法は、公知の方法で
ある鋳込み法、圧着法または爆着法などのいずれを用い
ても良い。なお、複層の製造方法によって異なるが、接
合部には多かれ少なかれ表層と内層成分が混合・拡散し
た層が存在する。この拡散層の存在は、本発明にはなん
ら本質的な問題はなく、拡散層を除く表層と内層の成分
が上記の請求範囲を満足すれば発明が完成するものであ
る。つまり、両表層部厚/内層部厚の比率は拡散層厚を
除外してカウントすればよい。
As a method for manufacturing the multi-layered steel sheet, any of known methods such as a casting method, a pressure bonding method and an explosive deposition method may be used. It should be noted that, depending on the manufacturing method of the multiple layers, there are more or less layers in which the surface layer and inner layer components are mixed and diffused in the joint portion. The existence of this diffusion layer does not cause any essential problem in the present invention, and the invention is completed if the components of the surface layer and the inner layer excluding the diffusion layer satisfy the above-mentioned claims. That is, the ratio of both surface layer thickness / inner layer thickness may be counted excluding the diffusion layer thickness.

【0011】また、製品の全体厚みは無方向性電磁鋼板
として多く用いられる0.15mm〜0.8mmが適当であ
る。さらに、上面と下面の表層部厚みの選択についてで
あるが高周波域での表皮効果は上下面対称なので上面と
下面で差をつける意味がない。このためその厚みはほぼ
同じでよい。以下に、本発明の実施例について具体的に
説明する。
Further, the total thickness of the product is preferably 0.15 mm to 0.8 mm which is often used as a non-oriented electrical steel sheet. Further, regarding the selection of the surface layer thickness of the upper surface and the lower surface, since the skin effect in the high frequency region is vertically symmetrical, there is no point in making a difference between the upper surface and the lower surface. Therefore, the thickness may be almost the same. Examples of the present invention will be specifically described below.

【0012】[0012]

【実施例】表層部と内層部に用いた材料の化学成分を表
1に示す。また、複層の比率を変えた実験内容と結果を
表2に示す。実験プロセスは、表1の成分を含む無方向
性電磁鋼板の冷延板を700℃に通電加熱し、20%圧
下にて圧着接合し、0.5mmの板厚としたものを、88
0℃で30秒焼鈍した後、磁気測定したものである。測
定に用いた密度は、Si+1.7Al量を内外層トータ
ルして平均して求め、ASTM A34(1983)に
準拠して計算した。
EXAMPLES Table 1 shows the chemical composition of the materials used for the surface layer and the inner layer. Table 2 shows the contents of the experiment and the results when the ratio of the multiple layers was changed. The experimental process was performed by heating a cold-rolled sheet of non-oriented electrical steel sheet containing the components of Table 1 to 700 ° C. by electric current heating, press-bonding under 20% pressure, and making a sheet thickness of 0.5 mm.
It is a magnetic measurement after annealing at 0 ° C. for 30 seconds. The density used for the measurement was obtained by averaging the total amount of Si + 1.7Al in the inner and outer layers, and was calculated according to ASTM A34 (1983).

【0013】[0013]

【表1】 [Table 1]

【0014】[0014]

【表2】 [Table 2]

【0015】以上の如く、複層比率が本発明範囲外の実
験No.1と3は、それぞれ高周波鉄損と磁束密度が不満
足である。また表層のSi量が本発明範囲を外れる実験
No.7は、高周波鉄損が不満である。更に、成分が本発
明範囲外の実験No.8,9,10,11,12と13は
微小析出物が多いため低周波鉄損と高周波磁気特性が劣
化する。従来の単層鋼板である実験No.5と6は、鉄損
と磁束密度の両者を同時に満足さすことができない。本
発明範囲を満足する実験No.2と4の試料で、低周波で
の磁束密度と高周波鉄損の両者を満足するものが得られ
た。
As described above, the experiment No. in which the multilayer ratio was outside the range of the present invention. In Nos. 1 and 3, the high frequency iron loss and the magnetic flux density are unsatisfactory, respectively. Experiments in which the amount of Si in the surface layer is outside the range of the present invention
No. No. 7 is dissatisfied with high frequency iron loss. Furthermore, in Experiment No. in which the components were out of the scope of the present invention. Since 8, 9, 10, 11, 12 and 13 have many fine precipitates, low frequency iron loss and high frequency magnetic properties are deteriorated. Experiment No., which is a conventional single-layer steel sheet In Nos. 5 and 6, both iron loss and magnetic flux density cannot be satisfied at the same time. Experiment No. satisfying the range of the present invention. Samples 2 and 4 were obtained that satisfied both the magnetic flux density at low frequencies and the high frequency iron loss.

【0016】[0016]

【発明の効果】以上の如く本発明によれば、低周波と高
周波の磁気特性を同時に満足させる無方向性電磁鋼板を
製造することができ、特にインバータ用として極めて有
用な材料を提供できる。
As described above, according to the present invention, it is possible to manufacture a non-oriented electrical steel sheet which simultaneously satisfies low-frequency and high-frequency magnetic properties, and it is possible to provide a very useful material especially for an inverter.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 重量比で表層部の成分が C≦0.005%、 Si:2.0〜4.0%、 Mn:0.1〜1.5%、 P≦0.1%、 S≦0.003%、 SolAl:0.05〜2.0%、 N≦0.003%、 残部Feおよび不可避的不純物からなり、 内層部の成分が C≦0.005%、 Si<2.0%、 Mn:0.1〜1.5%、 P≦0.1%、 S≦0.020%、 SolAl≦1.0%、 N≦0.003% を含有し、残部Feおよび不可避的不純物からなる複層
鋼板であり、上記、両表層部厚/内層部厚の比率が0.
1〜0.6であることを特徴とする磁気特性の優れた複
層無方向性電磁鋼板。
1. A surface layer component in a weight ratio of C ≦ 0.005%, Si: 2.0 to 4.0%, Mn: 0.1 to 1.5%, P ≦ 0.1%, S ≦ 0.003%, SolAl: 0.05 to 2.0%, N ≦ 0.003%, balance Fe and unavoidable impurities, inner layer component C ≦ 0.005%, Si <2.0 %, Mn: 0.1 to 1.5%, P ≦ 0.1%, S ≦ 0.020%, SolAl ≦ 1.0%, N ≦ 0.003%, balance Fe and unavoidable impurities Is a multi-layer steel sheet having a ratio of both surface layer thickness / inner layer thickness of 0.
A multi-layer non-oriented electrical steel sheet having excellent magnetic properties, which is 1 to 0.6.
JP3345085A 1991-12-26 1991-12-26 Double-layered non-oriented silicon steel sheet excellent in magnetic property Withdrawn JPH05263198A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3345085A JPH05263198A (en) 1991-12-26 1991-12-26 Double-layered non-oriented silicon steel sheet excellent in magnetic property

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3345085A JPH05263198A (en) 1991-12-26 1991-12-26 Double-layered non-oriented silicon steel sheet excellent in magnetic property

Publications (1)

Publication Number Publication Date
JPH05263198A true JPH05263198A (en) 1993-10-12

Family

ID=18374185

Family Applications (1)

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Country Status (1)

Country Link
JP (1) JPH05263198A (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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JP2010063252A (en) * 2008-09-03 2010-03-18 Jfe Steel Corp Core for high-speed motor having excellent heat dissipation properties and core material for high-speed motor
JP2010062275A (en) * 2008-09-03 2010-03-18 Jfe Steel Corp Motor core and motor core material
JP2010132938A (en) * 2008-12-02 2010-06-17 Jfe Steel Corp Clad type electromagnetic steel sheet
WO2022070497A1 (en) * 2020-09-29 2022-04-07 株式会社日立製作所 Soft magnetic iron plate, method for manufacturing soft magnetic iron plate, and iron core and dynamo-electric machine in which soft magnetic iron plate is used

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