JP2917776B2 - Non-oriented electrical steel sheet for high frequency - Google Patents

Non-oriented electrical steel sheet for high frequency

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Publication number
JP2917776B2
JP2917776B2 JP5295416A JP29541693A JP2917776B2 JP 2917776 B2 JP2917776 B2 JP 2917776B2 JP 5295416 A JP5295416 A JP 5295416A JP 29541693 A JP29541693 A JP 29541693A JP 2917776 B2 JP2917776 B2 JP 2917776B2
Authority
JP
Japan
Prior art keywords
less
steel sheet
thickness
sheet
texture
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
JP5295416A
Other languages
Japanese (ja)
Other versions
JPH07150310A (en
Inventor
善彦 尾田
邦和 冨田
俊治 飯塚
智良 大北
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.)
JFE Engineering Corp
Original Assignee
Nippon Kokan Ltd
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Filing date
Publication date
Application filed by Nippon Kokan Ltd filed Critical Nippon Kokan Ltd
Priority to JP5295416A priority Critical patent/JP2917776B2/en
Publication of JPH07150310A publication Critical patent/JPH07150310A/en
Application granted granted Critical
Publication of JP2917776B2 publication Critical patent/JP2917776B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
    • H01F1/14Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials metals or alloys
    • H01F1/147Alloys characterised by their composition
    • H01F1/14766Fe-Si based alloys
    • H01F1/14775Fe-Si based alloys in the form of sheets

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  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Chemical & Material Sciences (AREA)
  • Dispersion Chemistry (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Soft Magnetic Materials (AREA)

Description

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

【0001】[0001]

【産業上の利用分野】この発明は、高周波用無方向性電
磁鋼板に関し、特に鉄損が低く磁束密度が高い高周波用
無方向性電磁鋼板に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a high frequency non-oriented electrical steel sheet, and more particularly to a high frequency non-oriented electrical steel sheet having a low iron loss and a high magnetic flux density.

【0002】[0002]

【従来の技術】近年、省エネルギーの観点から電気機器
の高効率化が求められており、電気機器を高周波域で使
用することが多くなっている。このため、モーター等の
鉄心に用いられる電磁鋼板には優れた高周波磁気特性が
要求される。
2. Description of the Related Art In recent years, there has been a demand for higher efficiency of electric equipment from the viewpoint of energy saving, and electric equipment is often used in a high frequency range. For this reason, electromagnetic steel sheets used for iron cores of motors and the like are required to have excellent high-frequency magnetic properties.

【0003】しかし、電磁鋼板を高周波域で磁化する
と、渦電流損の増大に起因して、鉄損が急激に増大す
る。このため、鋼板の薄肉化及び鋼板の固有抵抗を上げ
ることにより渦電流損を減少させる試みがなされてき
た。すなわち、従来、高周波用途には、固有抵抗を上げ
る観点から、Si+Alを重量%で1.7〜6.5%程
度添加し、板厚を0.1〜0.25mmとした電磁鋼板が
用いられている。
[0003] However, when an electromagnetic steel sheet is magnetized in a high frequency range, iron loss increases sharply due to an increase in eddy current loss. For this reason, attempts have been made to reduce the eddy current loss by reducing the thickness of the steel sheet and increasing the specific resistance of the steel sheet. That is, conventionally, in the high frequency application, from the viewpoint of increasing the specific resistance, an electromagnetic steel sheet having a thickness of 0.1 to 0.25 mm, in which about 1.7 to 6.5% by weight of Si + Al is added, is used. ing.

【0004】例えば、特開平3−223445号公報に
はSi+Al量を2.0〜4.0%とし、板厚を0.1
〜0.25mmとした高周波用の無方向性電磁鋼板が開示
されている。
For example, JP-A-3-223445 discloses that the Si + Al content is set to 2.0 to 4.0% and the plate thickness is set to 0.1%.
A non-oriented electrical steel sheet for high frequency applications having a thickness of about 0.25 mm is disclosed.

【0005】[0005]

【発明が解決しようとする課題】ところで、NC工作機
械や研削盤に自動車に用いられるモーターは、高周波で
駆動されるとはいっても、周波数は700〜2000H
z程度である。このような用途に用いられる電磁鋼板は
低鉄損化による効率向上が重要であることはもちろんの
こと、高トルク化の観点から高磁束密度も要求されてい
る。このような用途に上述のSi+Alが1.7〜6.
5%程度含まれた鋼板を用いると、低鉄損化は達成され
るものの、飽和磁束密度の低下に起因する磁束密度の低
下は避けられず、高磁束密度化による高トルク化という
要望は満たせない状況にある。
By the way, motors used in automobiles for NC machine tools and grinders are driven at a high frequency, but have a frequency of 700-2000H.
about z. It is not only important for electromagnetic steel sheets used in such applications to improve efficiency by reducing iron loss, but also high magnetic flux density is required from the viewpoint of increasing torque. For such applications, the above-mentioned Si + Al is 1.7 to 6.
When a steel sheet containing about 5% is used, although a reduction in iron loss is achieved, a reduction in magnetic flux density due to a reduction in saturation magnetic flux density is inevitable, and the demand for higher torque by increasing the magnetic flux density can be satisfied. There is no situation.

【0006】この発明はかかる事情に鑑みてなされたも
のであって、高周波磁化領域において、鉄損が低くかつ
磁束密度が高い高周波用無方向性電磁鋼板を提供するこ
とを目的とする。
The present invention has been made in view of such circumstances, and has as its object to provide a high-frequency non-oriented electrical steel sheet having a low iron loss and a high magnetic flux density in a high-frequency magnetization region.

【0007】[0007]

【課題を解決するための手段及び作用】鋼板の磁束密度
を低下させないためには、鋼板中のSi,Al量を少な
くする必要があるが、Si,Al量の低下は当然のこと
ながら渦電流損の増大に伴う全鉄損の増大につながる。
このように相反する特性を両立させるべく本願発明者ら
が検討を重ねた結果、以下の知見を得るに至った。
In order to prevent the magnetic flux density of the steel sheet from lowering, it is necessary to reduce the amounts of Si and Al in the steel sheet. This leads to an increase in total iron loss with an increase in loss.
As a result of repeated studies by the inventors of the present invention in order to achieve such contradictory characteristics, the following findings have been obtained.

【0008】板厚0.1〜0.25mm程度の電磁鋼板を
100〜2000Hz程度で磁化した場合に、全鉄損中
ヒステリシス損の占める割合が30〜70%程度であ
る。従って、板厚0.1〜0.25mm程度の薄物電磁鋼
板における高周波鉄損の低減のためには、渦電流損を下
げる以外に、ヒステリシス損を下げることが有効である
と考えられる。
When an electromagnetic steel sheet having a thickness of about 0.1 to 0.25 mm is magnetized at about 100 to 2000 Hz, the ratio of the hysteresis loss to the total iron loss is about 30 to 70%. Therefore, in order to reduce high-frequency iron loss in a thin magnetic steel sheet having a thickness of about 0.1 to 0.25 mm, it is considered effective to reduce hysteresis loss in addition to reducing eddy current loss.

【0009】このヒステリシス損を下げるために、高周
波磁化時における板厚方向の磁束分布に着目した。すな
わち、高周波で鋼板を磁化した場合、磁束の表皮効果に
より、磁束の分布は鋼板板厚方向に均一にならず表層部
に集中する。このため、鋼板表層部の集合組織を制御す
ることにより磁束密度を向上させることができるのみな
らず、ヒステリシス損を低減することも可能となるので
ある。このようなヒステリシス損低減効果に起因して、
板厚0.1〜0.25mm程度の薄物電磁鋼板において
は、従来の成分よりも低Si、低Alの電磁鋼板でも高
周波域で低鉄損の電磁鋼板を得ることができ、しかも低
Si、低Alであることによる飽和磁束密度の向上と、
特定の集合組織の形成により低鉄損であるだけでなく、
磁束密度が高くなることを見出したのである。この発明
は本願発明者らのこのような知見に基づいてなされたも
のである。
In order to reduce the hysteresis loss, attention was paid to the magnetic flux distribution in the thickness direction during high-frequency magnetization. That is, when the steel sheet is magnetized at a high frequency, the distribution of the magnetic flux is not uniform in the thickness direction of the steel sheet but is concentrated on the surface layer due to the skin effect of the magnetic flux. Therefore, not only can the magnetic flux density be improved by controlling the texture of the surface layer of the steel sheet, but also the hysteresis loss can be reduced. Due to such hysteresis loss reduction effect,
In a thin magnetic steel sheet having a sheet thickness of about 0.1 to 0.25 mm, a magnetic steel sheet having a low iron loss in a high frequency region can be obtained even with a low Si and low Al magnetic steel sheet than conventional components. Improvement of saturation magnetic flux density due to low Al,
Not only low iron loss due to the formation of a specific texture,
They found that the magnetic flux density increased. The present invention has been made based on such findings of the present inventors.

【0010】すなわち、本発明は、重量%で、C:0.
005%以下、Si:1.0%超え2.0%以下、A
l:0.004%以下又は0.1〜0.5%、N:0.
005%以下を含み、板厚tが0.10〜0.25mm
であり、熱延板調圧率または焼鈍条件を調整することに
より、その板面内での(211)、(222)、(32
1)、(332)、(200)、(110)及び(31
0)面の各面についてのX線積分反射強度の理論強度に
対する比の値をP(hkl)とした場合に、以下の式で
表されるTP値が1.5以下となるような集合組織をそ
の各表面から板厚方向に板厚の3割以上含むことを特徴
とする高周波用無方向性電磁鋼板を提供するものであ
る。
That is, according to the present invention, C: 0.
005% or less, Si: more than 1.0% and 2.0% or less, A
l: 0.004% or less, or 0.1 to 0.5%;
005% or less, and the thickness t is 0.10 to 0.25 mm
It is necessary to adjust the hot-rolled sheet pressure regulation rate or annealing conditions.
More, in the plate plane (211), (222), (32
1), (332), (200), (110) and (31)
0) When the value of the ratio of the X-ray integrated reflection intensity to the theoretical intensity for each surface is P (hkl), the texture is such that the TP value represented by the following formula is 1.5 or less. From the respective surfaces in the thickness direction in a thickness direction of at least 30% of the thickness.

【0011】 TP=[P(211)+P(222)+P(321)+P(332)]/ [P(200)+P(110)+P(310)] また、重量%で、C:0.005%以下、Si:1.0
%超え2.0%以下、Mn:0.2〜1.0%、P:0.
2%以下、S:0.01%以下、Al:0.004%以
下又は0.1〜0.5%、N:0.005%以下を含
み、板厚tが0.10〜0.25mmであり、熱延板調
圧率または焼鈍条件を調整することにより、その板面内
での(211)、(222)、(321)、(33
2)、(200)、(110)及び(310)面の各面
についてのX線積分反射強度の理論強度に対する比の値
をP(hkl)とした場合に、上記式で表されるTP値
が1.5以下となるような集合組織をその各表面から板
厚方向に板厚の3割以上含むことを特徴とする高周波用
無方向性電磁鋼板を提供するものである。
TP = [P (211) + P (222) + P (321) + P (332)] / [P (200) + P (110) + P (310)] Also, C: 0.005% by weight%. Hereinafter, Si: 1.0
% To 2.0% or less, Mn: 0.2 to 1.0%, P: 0.
2% or less, S: 0.01% or less, Al: 0.004% or less or 0.1 to 0.5%, N: 0.005% or less, and the thickness t is 0.10 to 0.25 mm And hot rolled sheet
By adjusting the pressure ratio or the annealing conditions , (211), (222), (321), (33)
2) When the value of the ratio of the integrated X-ray reflection intensity to the theoretical intensity for each of the (200), (110), and (310) planes is P (hkl), the TP value represented by the above equation And a non-oriented electrical steel sheet for high frequency use, characterized in that the steel sheet contains a texture having a thickness of not more than 1.5 in the thickness direction from each surface thereof in the thickness direction.

【0012】さらに、上記いずれかの高周波用無方向性
電磁鋼板において、鋼板断面での平均結晶粒径Dが、
0.1t≦D≦0.7tを満足することを特徴とする高
周波用無方向性電磁鋼板を提供するものである。
Further, in any of the above non-oriented electrical steel sheets for high frequency use, the average crystal grain size D in the steel sheet cross section is:
An object of the present invention is to provide a high-frequency non-oriented electrical steel sheet satisfying 0.1t ≦ D ≦ 0.7t.

【0013】さらにまた、上記いずれかの高周波用無方
向性電磁鋼板において、周波数100〜2000Hzに
おいて、B10≧1.54T、W15/400≦35W/kgで
あることを特徴とする高周波用無方向性電磁鋼板を提供
するものである。
Further, in any of the above non-oriented electrical steel sheets for high frequency use, at a frequency of 100 to 2000 Hz, B 10 ≧ 1.54 T and W 15/400 ≦ 35 W / kg. It is intended to provide a conductive electrical steel sheet.

【0014】以下、本発明について詳細に説明する。
(1)成分について各成分の限定理由は以下の通りであ
る。なお、以下%表示はいずれも重量%である。
Hereinafter, the present invention will be described in detail.
(1) Reasons for limiting each component are as follows. In the following, all percentages are by weight.

【0015】Si: Siは鋼板の固有抵抗を上げるた
めに有効な元素であり、この効果が本発明が想定する周
波数域で十分に発揮されるためには1.0%を超えて含
有することが必要である。一方、Siの添加に伴って飽
和磁束密度が低下し、2.0%を超えるとその値が許容
範囲よりも低くなってしまう。従って、Si量を1.0
%超え2.0%以下の範囲に規定する。
Si: Si is an element effective for increasing the specific resistance of the steel sheet. In order for this effect to be sufficiently exerted in the frequency range assumed by the present invention, it must be contained in an amount exceeding 1.0%. is necessary. On the other hand, the saturation magnetic flux density decreases with the addition of Si, and if it exceeds 2.0%, the value becomes lower than the allowable range. Therefore, the amount of Si is 1.0
% To 2.0% or less.

【0016】Al: Alは微量に添加した場合には微
細なAlNを形成し、磁気特性を阻害するため、その恐
れが少ない0.004%以下に規定する。一方、0.1
%を超えて添加した場合には、AlNが粗大になるため
磁気特性を劣化させず、固有抵抗の上昇に寄与するが、
0.5%以上になると、Si同様磁束密度を低下させて
しまう。従って、Al量を0.004%以下又は0.1
〜0.5%の範囲に規定する。
Al: When Al is added in a small amount, it forms fine AlN and impairs magnetic characteristics. On the other hand, 0.1
%, The AlN becomes coarse, thereby not deteriorating magnetic properties and contributing to an increase in specific resistance.
If it is 0.5% or more, the magnetic flux density is reduced as in the case of Si. Therefore, the amount of Al is set to 0.004% or less or 0.1% or less.
It is specified in the range of 0.5%.

【0017】C: Cは磁気時効の問題があるため、そ
のような問題が生じない0.005%以下に規定する。 N: Nは0.005%以上となると磁気特性を劣化さ
せるため、0.005%以下に規定する。
C: Since C has a problem of magnetic aging, it is specified to 0.005% or less where such a problem does not occur. N: When N is 0.005% or more, the magnetic properties are degraded.

【0018】以上がこの発明において重要な成分である
が、以下に示すMn,S,Pを以下のように規定するこ
とにより、さらに良好な特性を得ることができる。 Mn: Mnは熱間圧延時の赤熱脆性を防止するため
に、0.2%以上必要であるが、1.0%を超えると磁
気特性を劣化させる。従って、Mn量を0.2〜1.0
%の範囲に規定する。
Although the above are important components in the present invention, better characteristics can be obtained by defining Mn, S, and P shown below as follows. Mn: Mn is required to be 0.2% or more in order to prevent red hot brittleness during hot rolling, but if it exceeds 1.0%, the magnetic properties deteriorate. Therefore, the amount of Mn is 0.2-1.0
%.

【0019】S: Sは磁気特性を劣化させるMnS等
を形成するため、そのような恐れがない0.01%を上
限とする。 P: Pは鋼板の打ち抜き性を改善するために必要な元
素であるが、0.2%を超えて添加すると磁束密度の低
下を招く。従って、P量を0.2%以下とした。
S: Since S forms MnS or the like which degrades the magnetic properties, the upper limit is 0.01% which does not have such a possibility. P: P is an element necessary for improving the punching property of a steel sheet, but when added in excess of 0.2%, the magnetic flux density is reduced. Therefore, the P content is set to 0.2% or less.

【0020】なお、Sb、Sn、B、Cu、Zrを磁気
特性向上のために添加することは何等さしつかえない。
また、これら元素以外の不可避不純物元素は通常の鋼に
含有される程度の量は許容される。
It should be noted that addition of Sb, Sn, B, Cu, and Zr for improving the magnetic properties may not be any.
In addition, unavoidable impurity elements other than these elements are allowed in an amount that is contained in ordinary steel.

【0021】(2)板厚 次に板厚の限定理由について説明する。板厚を薄くする
ことは、高周波域での渦電流損の低減に非常に効果的で
ある。しかし、板厚が0.10mm未満であると、冷間圧
延が困難となるだけでなく、モーターのローター、ステ
ーター組立時の鋼板の積層数の増大につながり、生産効
率が低下してしまう。また、0.25mmを超えると渦電
流損が増大し、鉄損の増大につながる。従って、板厚を
0.10〜0.25mmとした。
(2) Plate Thickness Next, the reason for limiting the plate thickness will be described. Reducing the thickness is very effective in reducing eddy current loss in a high frequency range. However, when the sheet thickness is less than 0.10 mm, not only cold rolling becomes difficult, but also the number of stacked steel sheets at the time of assembling the rotor of the motor and the stator is increased, and the production efficiency is reduced. On the other hand, if it exceeds 0.25 mm, eddy current loss increases, leading to an increase in iron loss. Therefore, the plate thickness was set to 0.10 to 0.25 mm.

【0022】(3)集合組織 鋼板板面の集合組織は、鋼板を目標とする板厚まで減厚
した後、X線回折装置を用いて反射法に基づいてX線回
折パターンを測定し、(211)、(222)、(32
1)、(332)、(200)、(110)及び(31
0)面のX線積分反射強度Iから、以下の(1)式で定
義されるP値を求め、さらにこのP値から(2)式で示
すTP値を求め、このTP値の大小で評価する。
(3) Texture The texture of the steel sheet surface is measured by measuring the X-ray diffraction pattern based on the reflection method using an X-ray diffractometer after reducing the thickness of the steel sheet to a target thickness. 211), (222), (32)
1), (332), (200), (110) and (31)
From the X-ray integrated reflection intensity I of the 0) plane, a P value defined by the following equation (1) is obtained, and from this P value, a TP value expressed by the equation (2) is obtained. I do.

【0023】 P(hkl)=7×[I/I0 (hkl)]/[ΣI/I0 (hkl)] I(hkl) : (hkl)面におけるX線積分強度 I0 (hkl): (hkl)面における理論強度 ………(1) TP=[P(211)+P(222)+P(321)+P(332)]/ [P(200)+P(110)+P(310)] ………(2) すなわち、磁化容易軸である<100>方向を含まない
(211)、(222)、(321)、及び(332)
面のP値の和と、<100>方向を含む(200)、
(110)、及び(310)面のP値の和との比である
TP値が低いほど鋼板の磁気特性上良好な集合組織が形
成されていることとなる。
P (hkl) = 7 × [I / I 0 (hkl)] / [ΣI / I 0 (hkl)] I (hkl): X-ray integrated intensity on (hkl) plane I 0 (hkl): ( theoretical strength on hkl) plane (1) TP = [P (211) + P (222) + P (321) + P (332)] / [P (200) + P (110) + P (310)] (2) That is, (211), (222), (321), and (332) that do not include the <100> direction that is the easy axis of magnetization.
Including the sum of the P values of the surface and the <100> direction (200);
The lower the TP value, which is the ratio of the sum of the P values of the (110) and (310) planes, to the better the texture in the magnetic properties of the steel sheet.

【0024】ところで、高周波で鋼板を磁化した場合、
磁束の表皮効果により、磁束の分布は鋼板板厚方向に均
一にならず表層部に集中する。例えば、100Hzでは
磁束の約7割が各表面から板厚の3割以内の部分に集中
する。この傾向は、周波数が高くなるにつれて顕著にな
り。1000Hzにおいては表面から板厚の3割以内の
部分に8〜9割の磁束が集中するようになる。このこと
から鋼板の表層部に好ましい集合組織を形成すれば、磁
束密度を向上させることができ、かつヒステリシス損を
効率良く低減できることが理解される。
When a steel sheet is magnetized at a high frequency,
Due to the skin effect of the magnetic flux, the distribution of the magnetic flux is not uniform in the thickness direction of the steel sheet but is concentrated on the surface layer. For example, at 100 Hz, about 70% of the magnetic flux concentrates on a portion within 30% of the plate thickness from each surface. This tendency becomes more pronounced as the frequency increases. At 1000 Hz, 80 to 90% of the magnetic flux concentrates on a portion within 30% of the plate thickness from the surface. From this, it is understood that, when a favorable texture is formed in the surface portion of the steel sheet, the magnetic flux density can be improved and the hysteresis loss can be reduced efficiently.

【0025】ここで、所望の集合組織を形成する方法は
特に限定されないが、本発明では、鋼板表層部の集合組
織を制御することが重要であるから、熱延板に調圧を加
えた後に熱延板焼鈍を行う方法を適用することが好まし
い。この方法では、調圧率又は焼鈍温度を調整すること
により、鋼板表層部の所望の集合組織の深さを任意に調
整することができる。
Here, the method of forming the desired texture is not particularly limited. However, in the present invention, since it is important to control the texture of the surface layer portion of the steel sheet, after the pressure is applied to the hot-rolled sheet, It is preferable to apply a method of performing hot-rolled sheet annealing. In this method, the depth of the desired texture of the surface layer portion of the steel sheet can be arbitrarily adjusted by adjusting the pressure regulation rate or the annealing temperature.

【0026】本発明においては、以上のことに基づい
て、上記TP値が1.5以下となるような集合組織を各
表面から板厚方向に板厚の3割以上含むことを要件とす
る。その理由について以下に説明する。
In the present invention, based on the above, it is required that a texture such that the above-mentioned TP value is 1.5 or less is included in the thickness direction from each surface in the thickness direction by 30% or more of the thickness. The reason will be described below.

【0027】図1は、鋼種A(C:0.040%、S
i:1.05%、Mn:0.22%、P:0.10%、
S:0.004%、Al:tr、N:0.0031
%)、鋼種B(C:0.031%、Si:1.90%、
Mn:0.60%、P:0.03%、S:0.004
%、Al:0.40%、N:0.0030%)を用い、
熱延板調圧−焼鈍を行わない通常のプロセスを用いて作
製した電磁鋼板と、熱延板調圧−焼鈍条件を調整して集
合組織を制御した電磁鋼板とについて、鋼板表面から板
厚の3割の深さにおけるTP値と磁束密度B10との関係
を示す図である。なお、鋼種Aを用いて熱延板調圧−焼
鈍を行わない通常のプロセスで作製した鋼板は、板厚t
=0.20mm、平均結晶粒径D=50μmであり、熱
延板調圧−焼鈍を行ったものは、板厚t=0.20m
m、平均結晶粒径D=48μmであった。鋼種Bを用い
て通常のプロセスで作製した鋼板は、板厚t=0.20
mm、結晶粒径D=60μmであり、熱延板調圧−焼鈍
を行ったものは、板厚t=0.20mm、結晶粒径D=
56μmであった。ここで、鋼板表面から板厚の3割の
深さにおけるTP値によって集合組織を評価したのは、
周波数100〜2000Hzにおいては鋼板表面から板
厚の3割以内の領域に磁束の7〜9割が集中するためで
ある。また、B10で磁束密度を評価したのは、周波数1
00〜2000Hzで用いられる機器の励磁磁束密度が
高周波でありながら1.5T程度の比較的高磁束密度で
使用されることが多く、B10がほぼそれに相当するため
である。
FIG. 1 shows a steel type A (C: 0.040%, S
i: 1.05%, Mn: 0.22%, P: 0.10%,
S: 0.004%, Al: tr, N: 0.0031
%), Steel type B (C: 0.031%, Si: 1.90%,
Mn: 0.60%, P: 0.03%, S: 0.004
%, Al: 0.40%, N: 0.0030%),
Hot rolled sheet pressure control-For electrical steel sheets manufactured using a normal process that does not perform annealing, and for hot rolled sheet pressure control-for an electrical steel sheet whose texture is controlled by adjusting the annealing conditions, it is a diagram showing the relation between TP value and the magnetic flux density B 10 of definitive to 30% of the depth. In addition, the steel sheet manufactured by the normal process without performing the hot-rolled sheet pressure-annealing using the steel type A has a sheet thickness t.
= 0.20 mm, average grain diameter D = 50 μm, and the sheet thickness t = 0.20 m after hot-rolled sheet pressure-annealing
m, average crystal grain size D = 48 μm. A steel sheet manufactured by a normal process using steel type B has a thickness t = 0.20.
mm, the crystal grain size D = 60 μm, and the sheet thickness t = 0.20 mm and the crystal grain size D =
It was 56 μm. Here, the texture was evaluated by the TP value at a depth of 30% of the sheet thickness from the steel sheet surface,
At a frequency of 100 to 2000 Hz, 70 to 90% of the magnetic flux is concentrated in a region within 30% of the plate thickness from the surface of the steel plate. Further, the reason to evaluate the flux density B 10, the frequency 1
Often excitation magnetic flux density of the equipment used in 00~2000Hz are used in relatively high magnetic flux density of about 1.5T, yet high frequency, because the B 10 is substantially equivalent to it.

【0028】この図1より、TP≦1.5とすることに
より、従来材よりも磁束密度が0.03T以上高くな
り、明らかに磁束密度の向上が確認される。次に、集合
組織を制御することによる鉄損低減効果の周波数による
影響について示す。ここでは、鋼種C(C:0.037
%、Si:1.10%、Mn:0.18%、P:0.1
1%、S:0.005%、Al:0.30%、N:0.
0035%)、鋼種D(C:0.045%、Si:1.
50%、Mn:0.25%、P:0.09%、S:0.
004%、Al:0.20%、N:0.0030%)を
用い、熱延板調圧−焼鈍を行わない通常のプロセスを用
いて作製した電磁鋼板と、熱延板調圧−焼鈍条件を調整
してTP値が1.5以下となるような集合組織を表層か
ら板厚方向に板厚の3割以上含むようにした本発明の電
磁鋼板とについて、各周波数における鉄損W15の値を求
めた。なお、本発明材としては、鋼種Cについてはt=
0.2mm、平均結晶粒径D=31μm、TP≦1.5
の領域深さ0.082mm(x/t=41%)、鋼種D
についてはt=0.1mm、平均結晶粒径D=23μ
m、TP≦1.5の領域深さ0.035mm(x/t=
35%)のものを用いた。また、従来材としては、鋼種
Cについてはt=0.2mm、平均結晶粒径D=30μ
m、鋼板表面から板厚の3割の深さにおけるTP=2.
7、鋼種Dについてはt=0.1mm、平均結晶粒径D
=21μm、鋼板表面から板厚の3割の深さにおけるT
P=2.6のものを用いた。図2は、本発明材のW15の
従来材のW15に対する比を周波数に対してプロットした
ものである。
From FIG. 1, when TP ≦ 1.5, the magnetic flux density becomes higher than that of the conventional material by 0.03 T or more, and it is confirmed that the magnetic flux density is clearly improved. Next, the influence of the frequency on the iron loss reduction effect by controlling the texture will be described. Here, steel type C (C: 0.037
%, Si: 1.10%, Mn: 0.18%, P: 0.1
1%, S: 0.005%, Al: 0.30%, N: 0.
0035%), steel type D (C: 0.045%, Si: 1.
50%, Mn: 0.25%, P: 0.09%, S: 0.
(004%, Al: 0.20%, N: 0.0030%), an electrical steel sheet manufactured using a normal process in which hot-rolled sheet pressure-annealing is not performed, and hot-rolled sheet pressure-annealing conditions. Of the iron loss W15 at each frequency with respect to the magnetic steel sheet of the present invention in which a texture having a TP value of 1.5 or less is included from the surface layer in the thickness direction by 30% or more of the thickness. I asked. As the material of the present invention, t =
0.2 mm, average crystal grain size D = 31 μm, TP ≦ 1.5
Depth of 0.082 mm (x / t = 41%), steel type D
T = 0.1 mm, average crystal grain size D = 23 μ
m, TP ≦ 1.5 region depth 0.035 mm (x / t =
35%). As a conventional material, t = 0.2 mm for steel type C and average crystal grain size D = 30 μm
m, TP at a depth of 30% of the plate thickness from the steel plate surface = 2.
7. For steel type D, t = 0.1 mm, average grain size D
= 21 μm, T at a depth of 30% of the sheet thickness from the steel sheet surface
The one with P = 2.6 was used. FIG. 2 is a plot of the ratio of W15 of the material of the present invention to W15 of the conventional material versus frequency.

【0029】この図2から、周波数100〜2000H
zの領域では鉄損の改善効果は大きいが、100Hz未
満及び2000Hz超えでは鉄損の改善効果は比較的小
さいことがわかる。これは、100Hz未満においては
磁束の表皮効果が小さいために、板厚表層部の板厚の3
割程度の集合組織の調整では効果が少なく、また200
0Hzを超えた場合には、全鉄損中に占めるヒステリシ
ス損の割合が小さくなるため、集合組織の調整によりヒ
ステリシス損を低下させたとしても全鉄損に及ぼす効果
が小さいためである。なお、図2からわかるように、周
波数100〜2000Hzの領域においては、本発明材
のW15の従来材のW15に対する比の値はほぼ一定であ
り、集合組織の調整による鉄損の改善効果はこの範囲に
おいて周波数によらないことがわかる。以上のことか
ら、本発明の電磁鋼板は100〜2000Hzで使用す
ることが好ましいことがわかる。
From FIG. 2, it can be seen that the frequency is 100 to 2000H.
It can be seen that the effect of improving iron loss is large in the region of z, but the effect of improving iron loss is relatively small below 100 Hz and above 2000 Hz. At less than 100 Hz, the skin effect of the magnetic flux is small, so that
Adjusting the texture at a relatively low level has little effect.
If the frequency exceeds 0 Hz, the ratio of the hysteresis loss to the total iron loss becomes small, so that even if the hysteresis loss is reduced by adjusting the texture, the effect on the total iron loss is small. As can be seen from FIG. 2, in the frequency range of 100 to 2000 Hz, the value of the ratio of W15 of the material of the present invention to W15 of the conventional material is almost constant, and the effect of improving the iron loss by adjusting the texture is this. It can be seen that the frequency does not depend on the frequency in the range. From the above, it is understood that the electromagnetic steel sheet of the present invention is preferably used at 100 to 2000 Hz.

【0030】図3は、上述の鋼種A(板厚t=0.20
mm、平均結晶粒径D=60μm)及び鋼種E(C:
0.036%、Si:1.40%、Mn:0.17%、
P:0.13%、S:0.003%、Al:0.40
%、N:0.0040%、板厚t=0.20mm、平均
結晶粒径D=41μm)について、TP≦1.5の領域
の鋼板表面からの深さと磁束密度B10及び鉄損W15/100
との関係を示す図である。ここでTP≦1.5の領域の
深さは、鋼板表面から板厚方向に減厚しながら板面の集
合組織をX線回折によって測定していき、TP=1.5
となった深さxを用いた。なお、ここで周波数100H
zでの鉄損を把握したのは、上記図2で示した結果に基
づく。
FIG. 3 shows the above steel type A (plate thickness t = 0.20).
mm, average crystal grain size D = 60 μm) and steel type E (C:
0.036%, Si: 1.40%, Mn: 0.17%,
P: 0.13%, S: 0.003%, Al: 0.40
%, N: 0.0040%, plate thickness t = 0.20 mm, average crystal grain size D = 41 μm), the depth from the steel plate surface in the region of TP ≦ 1.5, the magnetic flux density B 10, and the iron loss W 15 / 100
FIG. Here, the depth of the region of TP ≦ 1.5 is obtained by measuring the texture of the plate surface by X-ray diffraction while reducing the thickness from the surface of the steel plate in the plate thickness direction.
Was used. Here, the frequency is 100H
The reason why the iron loss at z was ascertained is based on the results shown in FIG.

【0031】この図3より、磁束密度B10及び鉄損W15
/100のいずれも、TP≦1.5の領域が30%までは鋼
板表面から内部に入るに従って急激に上昇し、それより
TP≦1.5の領域が深くなっても大きく変化しないこ
とが確認される。これは、前述したように、100Hz
では磁束の約7割が鋼板表面から板厚の部分に集中する
ためである。この磁束密度の表皮効果は周波数が高くな
るほど顕著となり、磁束がより表層に集中するようにな
るため、これより高周波側でも板厚の3割以上をTP≦
1.5とすれば十分である。
[0031] From this Figure 3, the magnetic flux density B 10 and core loss W15
In all cases, it was confirmed that up to 30% of the area of TP ≦ 1.5 rapidly increased as the area from the steel sheet surface entered, and that the area of TP ≦ 1.5 did not change significantly even when the area of TP ≦ 1.5 became deeper. Is done. This is, as mentioned above, 100 Hz
In this case, about 70% of the magnetic flux is concentrated from the surface of the steel sheet to the thickness of the steel sheet. The skin effect of the magnetic flux density becomes more remarkable as the frequency increases, and the magnetic flux concentrates more on the surface layer.
A value of 1.5 is sufficient.

【0032】以上の結果により、本発明ではTP値が
1.5以下となるような集合組織を各表面から板厚方向
に板厚の3割以上含むことを要件としている。 (4)結晶粒径 図4は、前述の鋼種B及び鋼種Cを用いて作製した電磁
鋼板の結晶粒径と板厚との比D/tの鉄損W15/400に及
ぼす影響を示す図である。ここで鋼種Bを用いて作製し
た鋼板は、t=0.15mm、TP≦1.5の領域の鋼
板表面からの深さ0.05mm以上鋼種Cを用いて作製
した鋼板は、t=0.2mm、TP≦1.5の領域の鋼
板表面からの深さ0.07mm以上、とした。
Based on the above results, the present invention requires that a texture having a TP value of 1.5 or less be included in each of the surfaces in a thickness direction of 30% or more of the thickness. (4) Grain Size FIG. 4 is a view showing the effect of the ratio D / t between the crystal grain size and the thickness of the magnetic steel sheet produced using the steel type B and the steel type C on the iron loss W15 / 400. is there. Here, the steel sheet manufactured using the steel type B is t = 0.15 mm, and the steel sheet manufactured using the steel type C at a depth of 0.05 mm or more from the steel sheet surface in the region of TP ≦ 1.5 is t = 0.15 mm. The depth from the steel plate surface in the region of 2 mm and TP ≦ 1.5 was 0.07 mm or more.

【0033】この図4に示すように、D/tが0.1〜
0.7の範囲、すなわち結晶粒径Dが0.1t〜0.7
tの範囲で鉄損がより低下している。これは、結晶粒径
Dが0.1t〜0.7tの範囲である場合には鋼板表層
部に所望の集合組織が適度に発達するが、結晶粒径Dが
0.1t未満であると所望の集合組織が得られても粒界
が磁壁移動を妨げるためにヒステリシス損が増大し、逆
に結晶粒径Dが0.7tを超えるとヒステリシス損は小
さくなるものの渦電流損が増大し、全鉄損が増大するた
めである。
As shown in FIG. 4, D / t is 0.1 to
0.7, that is, the crystal grain size D is 0.1 t to 0.7.
Iron loss is further reduced in the range of t. This is because when the crystal grain size D is in the range of 0.1 t to 0.7 t, a desired texture is appropriately developed in the surface layer portion of the steel sheet, but when the crystal grain size D is less than 0.1 t, the desired texture is desired. Even if the texture of is obtained, the hysteresis loss increases because the grain boundaries hinder the domain wall movement. Conversely, when the crystal grain size D exceeds 0.7 t, the hysteresis loss decreases but the eddy current loss increases. This is because iron loss increases.

【0034】以上のことより結晶粒径Dは、0.1t≦
D≦0.7tの範囲が好ましい。次に、本発明の無方向
性電磁鋼板を製造する方法について説明する。本発明に
おいては、鋼板表層部の集合組織を制御することが重要
であり、適宜の手法を用いて鋼板表層部の集合組織を調
整する必要があるが、その手法に関しては何等制約はな
く、前述した熱延調圧−焼鈍プロセスの他どのような手
法でも用いることができる。
From the above, the crystal grain size D is 0.1t ≦
The range of D ≦ 0.7t is preferred. Next, a method for producing the non-oriented electrical steel sheet of the present invention will be described. In the present invention, it is important to control the texture of the surface layer of the steel sheet, it is necessary to adjust the texture of the surface layer of the steel sheet using an appropriate method, but there is no limitation on the method, Any technique other than the hot rolling pressure-annealing process described above can be used.

【0035】それ以外の工程に関しても、通常用いられ
るプロセスで良い。すなわち、製鋼に関しては、転炉で
吹錬した溶鋼を脱ガス処理して所定の成分に調整すれば
よい。また、熱間圧延も通常の条件でよい。冷間圧延に
関しては1回でも、中間焼鈍を挟んで2回以上行っても
いずれでもよく、最終的に所望の板厚となればよい。最
終焼鈍に関しても通常の焼鈍でよく、この最終焼鈍条件
を制御することにより、結晶粒径を所望のものとするこ
とが可能となる。
As for the other steps, a commonly used process may be used. That is, regarding steelmaking, molten steel blown in a converter may be degassed and adjusted to a predetermined component. Hot rolling may be performed under ordinary conditions. The cold rolling may be performed once or may be performed two or more times with intermediate annealing therebetween, as long as the desired thickness is finally obtained. For the final annealing, ordinary annealing may be used. By controlling the final annealing conditions, it becomes possible to obtain a desired crystal grain size.

【0036】例えば、1.4%Si−0.4%Al鋼に
おいては、熱延板調圧率を7.0%、熱延板焼鈍条件を
850℃×3時間とし、冷間圧延により板厚を0.2m
mとした後、最終焼鈍を850℃×2分間行うことによ
り所望の集合組織を得ることが可能となる。なお、本発
明において、Sb、Sn、B、Cu、Zr等の添加によ
り本発明の集合組織を得ることは何等問題はない。
For example, in a 1.4% Si-0.4% Al steel, the hot-rolled sheet pressure regulation is 7.0%, the hot-rolled sheet annealing condition is 850 ° C. × 3 hours, and the sheet is cold-rolled. 0.2m thick
Then, the final annealing is performed at 850 ° C. for 2 minutes to obtain a desired texture. In the present invention, there is no problem in obtaining the texture of the present invention by adding Sb, Sn, B, Cu, Zr, or the like.

【0037】[0037]

【実施例】表1に示した鋼種1〜13の組成を有する鋼
材を、板厚2.0mmに熱間圧延した後酸洗し、表2に
示す熱延板調圧条件及び熱延板焼鈍条件で熱延板調圧−
焼鈍を行った。これら鋼板を引き続き板厚0.1〜0.
25mmまで冷間圧延し、表2に示す条件で最終焼鈍を
行った。なお、熱延板焼鈍は100%H2 雰囲気で行
い、最終焼鈍は25%H2 −75%N2 雰囲気で行っ
た。
EXAMPLE A steel material having the composition of steel types 1 to 13 shown in Table 1 was hot-rolled to a thickness of 2.0 mm and then pickled, and then hot-rolled sheet pressure conditions and hot-rolled sheet annealing shown in Table 2 were performed. Hot rolled sheet pressure regulation
Annealing was performed. These steel sheets are successively provided with a thickness of 0.1 to 0.1.
The sample was cold-rolled to 25 mm and subjected to final annealing under the conditions shown in Table 2. The hot-rolled sheet annealing was performed in a 100% H 2 atmosphere, and the final annealing was performed in a 25% H 2 -75% N 2 atmosphere.

【0038】磁気特性は、各鋼板から外径45mm、内
径33mmのリング試験片を採取し、これら試験片につ
いて周波数400Hzで測定し、さらに結晶粒径を測定
した。
The magnetic properties were measured by taking ring test pieces having an outer diameter of 45 mm and an inner diameter of 33 mm from each steel sheet, measuring these test pieces at a frequency of 400 Hz, and further measuring the crystal grain size.

【0039】各鋼板板厚、平均結晶粒径、TP≦1.5
の領域の鋼板表面からの深さ、及び磁気特性を表3に示
す。なお、表1中、鋼種1〜10は組成が本発明の範囲
内のものであり、鋼種11〜13は組成が本発明の範囲
外のものである。また、表2及び表3の番号1〜29は
これら鋼種に対して種々の条件で熱延板調圧−焼鈍処理
して作製した鋼板の番号を示す。
Each steel plate thickness, average crystal grain size, TP ≦ 1.5
Table 3 shows the depth from the surface of the steel sheet and the magnetic properties in the region indicated by. In Table 1, the compositions of steel types 1 to 10 are within the range of the present invention, and the compositions of steel types 11 to 13 are outside the range of the present invention. The numbers 1 to 29 in Tables 2 and 3 indicate the numbers of the steel sheets produced by subjecting these steel types to hot-rolled sheet pressure-annealing treatment under various conditions.

【0040】[0040]

【表1】 [Table 1]

【0041】[0041]

【表2】 [Table 2]

【0042】[0042]

【表3】 [Table 3]

【0043】鋼の組成、板厚、及びTP値が1.5以下
となるような集合組織を有する領域深さがいずれも本発
明を満たす番号1、2、4、7〜9、11、13、15
〜20、23〜25はいずれも高周波域において鉄損が
低くかつ磁束密度が高く、高周波用無方向性電磁鋼板と
して優れていることが確認された。
Numbers 1, 2, 4, 7 to 9, 11, and 13 each having a steel composition, a plate thickness, and a domain depth having a texture such that the TP value is 1.5 or less satisfy the present invention. , 15
-20 and 23-25 all have low iron loss and high magnetic flux density in the high frequency range, and were confirmed to be excellent as non-oriented electrical steel sheets for high frequency use.

【0044】それに対して、組成、TP≦1.5の領域
深さ、及び板厚の少なくとも1つが外れる番号3、5、
10、12、14、21、27〜29は、鉄損が高い
か、又は磁束密度が低い値となることが確認された。
On the other hand, at least one of the composition, the region depth of TP ≦ 1.5, and the plate thicknesses of Nos. 3, 5,
It was confirmed that 10, 12, 14, 21, 27 to 29 have a high iron loss or a low magnetic flux density.

【0045】[0045]

【発明の効果】この発明によれば、組成、板厚及び鋼板
表層部の集合組織を調整することにより、高周波磁化領
域において鉄損が低くかつ磁束密度が高い高周波用無方
向性電磁鋼が提供される。
According to the present invention, there is provided a high-frequency non-directional electromagnetic steel having a low iron loss and a high magnetic flux density in a high-frequency magnetization region by adjusting the composition, the thickness, and the texture of the surface layer of the steel sheet. Is done.

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

【図1】熱延板調圧−焼鈍を行わない通常のプロセスを
用いて作製した電磁鋼板と、熱延板調圧−焼鈍条件を調
整して集合組織を制御した電磁鋼板とについて、鋼板表
面から板厚の3割の深さにおけるTP値と磁束密度B10
との関係を示す図。
FIG. 1 shows a steel sheet surface of an electrical steel sheet manufactured using a normal process in which hot-rolled sheet pressure-annealing is not performed, and an electrical steel sheet in which texture is controlled by adjusting hot-rolled sheet pressure-annealing conditions. Value and magnetic flux density B 10 at a depth of 30% of the plate thickness
FIG.

【図2】本発明材のW15の従来材のW15に対する比を周
波数に対してプロットした図。
FIG. 2 is a diagram in which the ratio of W15 of the material of the present invention to W15 of the conventional material is plotted against frequency.

【図3】TP≦1.5の領域の鋼板表面からの深さと磁
束密度B10及び鉄損W15/100との関係を示す図。
Figure 3 is a graph showing a relation between the depth and the magnetic flux density B 10 and core loss W15 / 100 from the steel sheet surface area of the TP ≦ 1.5.

【図4】鋼板の結晶粒径と板厚との比D/tの鉄損W15
/400に及ぼす影響を示す図。
FIG. 4 shows the iron loss W15 of the ratio D / t between the crystal grain size and the thickness of the steel sheet.
The figure which shows the effect on / 400.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 大北 智良 東京都千代田区丸の内一丁目1番2号 日本鋼管株式会社内 (56)参考文献 特開 平5−140646(JP,A) 特開 平5−5126(JP,A) 特開 平2−310316(JP,A) 特開 平2−141530(JP,A) 特開 平4−107216(JP,A) 特開 平4−325629(JP,A) (58)調査した分野(Int.Cl.6,DB名) C22C 38/00 303 C22C 38/06 H01F 1/16 ──────────────────────────────────────────────────続 き Continued on the front page (72) Inventor Tomoyoshi Ohkita 1-2-1 Marunouchi, Chiyoda-ku, Tokyo Inside Nippon Kokan Co., Ltd. (56) References JP-A-5-140646 (JP, A) JP-A-2-310316 (JP, A) JP-A-2-141530 (JP, A) JP-A-4-107216 (JP, A) JP-A-4-325629 (JP, A) A) (58) Field surveyed (Int. Cl. 6 , DB name) C22C 38/00 303 C22C 38/06 H01F 1/16

Claims (4)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 重量%で、C:0.005%以下、S
i:1.0%超え2.0%以下、Al:0.004%以
下又は0.1〜0.5%、N:0.005%以下を含
み、板厚tが0.10〜0.25mmであり、熱延板調
圧率または焼鈍条件を調整することにより、その板面内
での(211)、(222)、(321)、(33
2)、(200)、(110)及び(310)面の各面
についてのX線積分反射強度の理論強度に対する比の値
をP(hkl)とした場合に、以下の式で表されるTP
値が1.5以下となるような集合組織をその各表面から
板厚方向に板厚の3割以上含むことを特徴とする高周波
用無方向性電磁鋼板。 TP=[P(211)+P(222)+P(321)+P(332)]/ [P(200)+P(110)+P(310)]
(1) C: 0.005% or less in weight%, S
i: 1.0% to 2.0% or less, Al: 0.004% or less or 0.1 to 0.5%, N: 0.005% or less, and the sheet thickness t is 0.10 to 0.5%. 25mm, hot rolled sheet
By adjusting the pressure ratio or the annealing conditions , (211), (222), (321), (33)
2) When the value of the ratio of the integrated X-ray reflection intensity to the theoretical intensity for each of the (200), (110), and (310) planes is P (hkl), TP is represented by the following equation.
A non-oriented high-frequency electrical steel sheet for high frequency use, comprising a texture having a value of 1.5 or less in the thickness direction from each surface thereof in the thickness direction. TP = [P (211) + P (222) + P (321) + P (332)] / [P (200) + P (110) + P (310)]
【請求項2】 重量%で、C:0.005%以下、S
i:1.0%超え2.0%以下、Mn:0.2〜1.0
%、P:0.2%以下、S:0.01%以下、Al:
0.004%以下又は0.1〜0.5%、N:0.00
5%以下を含み、板厚tが0.10〜0.25mmであ
り、熱延板調圧率または焼鈍条件を調整することによ
り、その板面内での(211)、(222)、(32
1)、(332)、(200)、(110)及び(31
0)面の各面についてのX線積分反射強度の理論強度に
対する比の値をP(hkl)とした場合に、以下の式で
表されるTP値が1.5以下となるような集合組織をそ
の各表面から板厚方向に板厚の3割以上含むことを特徴
とする高周波用無方向性電磁鋼板。 TP=[P(211)+P(222)+P(321)+P(332)]/ [P(200)+P(110)+P(310)]
2. In% by weight, C: 0.005% or less, S
i: more than 1.0% and 2.0% or less, Mn: 0.2 to 1.0
%, P: 0.2% or less, S: 0.01% or less, Al:
0.004% or less or 0.1 to 0.5%, N: 0.00
5% or less, the sheet thickness t is 0.10 to 0.25 mm, and by adjusting the pressure regulation rate of the hot rolled sheet or the annealing condition.
Ri, the plate plane in the (211), (222), (32
1), (332), (200), (110) and (31)
0) When the value of the ratio of the X-ray integrated reflection intensity to the theoretical intensity for each surface is P (hkl), the texture is such that the TP value represented by the following formula is 1.5 or less. From the respective surfaces in the thickness direction in a thickness direction of at least 30% of the thickness. TP = [P (211) + P (222) + P (321) + P (332)] / [P (200) + P (110) + P (310)]
【請求項3】 鋼板断面での平均結晶粒径Dが、0.1
t≦D≦0.7tを満足することを特徴とする請求項1
又は2記載の高周波用無方向成電磁鋼板。
3. The steel sheet having an average grain size D in a cross section of 0.1%.
2. The structure according to claim 1, wherein t ≦ D ≦ 0.7t is satisfied.
Or the non-oriented electrical steel sheet for high frequency waves according to 2.
【請求項4】 周波数100〜2000Hzにおいて、
10≧1.54T、W15/400≦35W/kgであること
を特徴とする請求項1乃至3いずれか1項記載の高周波
用無方向成電磁鋼板。
4. At a frequency of 100 to 2000 Hz,
4. The high frequency non-oriented electrical steel sheet according to claim 1, wherein B 10 ≧ 1.54T and W 15/400 ≦ 35 W / kg.
JP5295416A 1993-11-25 1993-11-25 Non-oriented electrical steel sheet for high frequency Expired - Fee Related JP2917776B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5295416A JP2917776B2 (en) 1993-11-25 1993-11-25 Non-oriented electrical steel sheet for high frequency

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5295416A JP2917776B2 (en) 1993-11-25 1993-11-25 Non-oriented electrical steel sheet for high frequency

Publications (2)

Publication Number Publication Date
JPH07150310A JPH07150310A (en) 1995-06-13
JP2917776B2 true JP2917776B2 (en) 1999-07-12

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ID=17820327

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Country Link
JP (1) JP2917776B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100530047B1 (en) * 2001-03-05 2005-11-22 주식회사 포스코 A non-oriented electrical steel sheet having improved core loss after stress relief annealing and a method for manufacturing it
CN104237274A (en) * 2014-09-28 2014-12-24 国家电网公司 Method for measuring macroscopic texture of high-magnetic induction oriented electrical steel

Also Published As

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