JPS6149380B2 - - Google Patents

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Publication number
JPS6149380B2
JPS6149380B2 JP53020299A JP2029978A JPS6149380B2 JP S6149380 B2 JPS6149380 B2 JP S6149380B2 JP 53020299 A JP53020299 A JP 53020299A JP 2029978 A JP2029978 A JP 2029978A JP S6149380 B2 JPS6149380 B2 JP S6149380B2
Authority
JP
Japan
Prior art keywords
magnetization
magnetic
steel plate
present
steel sheet
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP53020299A
Other languages
Japanese (ja)
Other versions
JPS54112317A (en
Inventor
Yakichiro Kawaomo
Tosha Wada
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 JP2029978A priority Critical patent/JPS54112317A/en
Publication of JPS54112317A publication Critical patent/JPS54112317A/en
Publication of JPS6149380B2 publication Critical patent/JPS6149380B2/ja
Granted legal-status Critical Current

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  • Soft Magnetic Materials (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は新規な一次再結晶による電磁鋼板に関
するものである。 従来無方向性電磁鋼板のL(圧延方向)とC
(圧延面内で圧延方向と直角方向)および圧延面
内の各方向の磁化特性は、どちらかと云えば同等
であつた。このため従来の鋼板はワンパンチタイ
プの回転機用コアとしては適しているが、L特性
を重視するEIコアやセグメントタイプの回転機
コア、変圧器コアとしては最適とは云いがたい。 本発明は、EI、セグメントタイプの回転機、
変圧器等Lの磁化特性を特に重視するコア用とし
て、Lの磁化特性の優れた鋼板を安価に提供する
ことを目的にしている。 本発明の鋼板はC0.01〜0.001%、Si2.0〜3.5
%、Mn0.1〜0.4%、Al0.01〜0.70%、S0.02%以
下、残部鉄及び不可避不純物からなり、体心立方
格子結晶の三軸即ち〔100〕、〔010〕、〔001〕中、
Lとの角度がCとの角度より小さい軸方向の磁区
(軸方向と一致および180゜磁区)が、磁区全体積
の65%〜95%を占めることを特徴とする一次再結
晶による電磁鋼板で、本発明中特に優れた鋼板
は、結晶の三軸中Lへの磁化が最も容易な軸と同
方向および180゜方向への磁区が、三軸中Cへの
磁化も最も容易な軸方向への磁区の二倍以上にな
つているものである。 ここでL方向に近い磁区の%はトルク曲線、逆
極点図、磁歪曲線図、および代表的結晶の磁区構
造説明図(第1図)とから統計的に求めるもので
ある。 磁区全体積の65〜95%と限定した理由は60%程
度までは一般の電磁鋼板においても、ありうるた
めで、ほぼ95%までとしたのは、理論上からも又
実際上からも限界であるからである。 本発明の鋼板は、Lへ磁化する際に、180゜磁
壁の移動による磁化の割合が、磁壁移動に大きな
磁化力を要する90゜磁壁の移動の割合よりはるか
に多くなる。このためLに所望の磁束密度を得る
ための磁化力が少なくてすむ利益があり、Lの鉄
損も小くなる。また本発明の最も顕著な効果の一
つは、変圧器等の騒音の原因である磁歪が、Lに
おいて極めて少さいことである。 本発明の鋼板の実施例を成分、磁化回転力曲
線、逆極点図、磁化特性で以下に示す。 実施例 1 成分: C 0.003%、Si 3.0%、Mn 0.21% Al 0.56%、S 0.004%、 残部鉄及び不可避不純物 DH、CC、二回冷延法。 鋼板厚さ0.35mm、本発明における磁区約90%、
この鋼板の磁化回転力曲線を第2図に、逆極点図
を第3図に示す。 実施例 2 成分: C 0.0026%、Si 2.7%、Mn 0.21% Al 0.31%、S 0.005%、 残部鉄及び不可避不純物、 DH、CC、二回冷延法。 鋼板厚さ0.35mm、本発明における磁区約80%、
この鋼板の磁化回転力曲線を第4図に、逆極点図
を第5図に示す。 実施例 3 成分: C 0.005%、Si 2.8%、Mn 0.20% Al 0.41%、S 0.004%、 残部鉄及び下可避不純物、DH、CC、二回冷延
法。 鋼板厚さ0.50mm、本発明における磁区約80%、
この鋼板の磁化回転力曲線を第6図に示す。 比較例 成分: C 0.004%、Si 2.9%、Mn 0.20% Al 0.45%、S 0.004%、 残部鉄及び不可避不純物、常法による。 鋼板厚さ0.35mm、本発明における磁区約55%、
この鋼板の磁化回転力曲線を第7図に示す。 次に各実施例並びに比較材の磁化特性を第1表
に示す。
The present invention relates to a novel electrical steel sheet produced by primary recrystallization. L (rolling direction) and C of conventional non-oriented electrical steel sheet
The magnetization characteristics (in the direction perpendicular to the rolling direction within the rolling plane) and in each direction within the rolling plane were rather similar. For this reason, conventional steel plates are suitable as cores for one-punch type rotating machines, but they are not optimal for EI cores, segment-type rotating machine cores, or transformer cores, where L characteristics are important. The present invention is an EI, a segment type rotating machine,
The purpose of the present invention is to provide a steel plate with excellent L magnetization characteristics at a low cost for use in cores such as transformers where the L magnetization characteristics are particularly important. The steel plate of the present invention has C0.01~0.001%, Si2.0~3.5
%, Mn 0.1-0.4%, Al 0.01-0.70%, S 0.02% or less, the balance consisting of iron and unavoidable impurities, three axes of body-centered cubic lattice crystal, namely [100], [010], [001] During,
An electrical steel sheet produced by primary recrystallization, characterized in that axial magnetic domains whose angle with L is smaller than the angle with C (coincident with the axial direction and 180° magnetic domains) occupy 65% to 95% of the total domain area. , the particularly excellent steel sheet of the present invention has a magnetic domain in the same direction and 180° direction as the axis in which magnetization in the L direction of the crystal is easiest, and in the direction of the axis in which magnetization in the C direction is easiest in the triaxial direction. The number of magnetic domains is more than twice as large as that of the magnetic domain. Here, the percentage of magnetic domains close to the L direction is statistically determined from the torque curve, the inverse pole figure, the magnetostriction curve diagram, and the explanatory diagram of the magnetic domain structure of a typical crystal (FIG. 1). The reason why we limited it to 65% to 95% of the total area of the magnetic domain is that up to about 60% can occur even in general electrical steel sheets, and the reason we set it to almost 95% is the limit both theoretically and practically. Because there is. When the steel sheet of the present invention is magnetized in the L direction, the proportion of magnetization due to the movement of the 180° domain wall is much larger than the proportion of the movement of the 90° domain wall, which requires a large magnetizing force for domain wall movement. Therefore, there is an advantage that L requires less magnetizing force to obtain the desired magnetic flux density, and the iron loss of L is also reduced. Moreover, one of the most remarkable effects of the present invention is that magnetostriction, which is a cause of noise in transformers, etc., is extremely small in L. Examples of the steel plate of the present invention are shown below in terms of components, magnetization rotational force curves, inverse pole figures, and magnetization characteristics. Example 1 Ingredients: C 0.003%, Si 3.0%, Mn 0.21% Al 0.56%, S 0.004%, balance iron and inevitable impurities DH, CC, double cold rolling method. Steel plate thickness 0.35mm, magnetic domain approximately 90% in the present invention,
The magnetization torque curve of this steel plate is shown in FIG. 2, and the inverse pole figure is shown in FIG. Example 2 Ingredients: C 0.0026%, Si 2.7%, Mn 0.21% Al 0.31%, S 0.005%, balance iron and inevitable impurities, DH, CC, double cold rolling method. Steel plate thickness 0.35mm, magnetic domain approximately 80% in the present invention,
The magnetization torque curve of this steel plate is shown in FIG. 4, and the inverse pole figure is shown in FIG. Example 3 Ingredients: C 0.005%, Si 2.8%, Mn 0.20% Al 0.41%, S 0.004%, balance iron and inevitable impurities, DH, CC, double cold rolling method. Steel plate thickness 0.50mm, magnetic domain approximately 80% in the present invention,
The magnetization torque curve of this steel plate is shown in FIG. Comparative Example Components: C 0.004%, Si 2.9%, Mn 0.20% Al 0.45%, S 0.004%, balance iron and unavoidable impurities, by conventional method. Steel plate thickness 0.35mm, magnetic domain approximately 55% in the present invention,
The magnetization torque curve of this steel plate is shown in FIG. Next, Table 1 shows the magnetization properties of each example and comparative material.

【表】 第8図は実施例1の磁歪を磁束密度0.5(T)、
1.5(T)の場合について、測定した結果を示
す。
[Table] Figure 8 shows the magnetostriction of Example 1 at a magnetic flux density of 0.5 (T) and
The measurement results for the case of 1.5 (T) are shown below.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図イ,ロ,ハは本発明の鋼板を説明するた
めの補助図で、代表的な結晶の磁化構造説明図、
第2図、第3図は夫々実施例における磁化回転力
曲線図及び逆極点図、第4図、第5図は実施例2
における磁化回転力曲線図及び逆極点図、第6図
は実施例3における磁化回転力曲線図、第7図は
比較例における磁化回転力曲線図、第8図は実施
例1における磁歪を磁束密度0.5(T)、1.5
(T)の場合について測定した結果を示す図であ
る。
Figures 1A, 1B, and 1C are auxiliary diagrams for explaining the steel plate of the present invention, including typical crystal magnetization structure explanatory diagrams,
Figures 2 and 3 are magnetization rotational force curve diagrams and inverse pole figures in Example, respectively, and Figures 4 and 5 are Example 2.
Fig. 6 is a magnetization rotational force curve diagram and inverse pole figure in Example 3, Fig. 7 is a magnetization rotational force curve diagram in a comparative example, and Fig. 8 is a magnetization rotational force curve diagram in Example 1 as a function of magnetic flux density. 0.5(T), 1.5
It is a figure which shows the result measured in case (T).

Claims (1)

【特許請求の範囲】 1 重量%で、C:0.001〜0.01%、Si:2.0〜3.5
%、Mn:0.1〜0.4%、Al:0.01〜0.70%、S:
0.02%以下、残部Feおよび不可避的不純物元素
からなり、体心立方格子結晶の三軸<100>の方
向の磁区のうち、圧延方向とのなす角(三次元空
間内での角度)の最も小さいものの磁区全体積に
占める比率が65〜95%である一次再結晶による電
磁鋼板。 2 圧延方向に最も磁化し易い結晶軸方向への磁
区が、他の二軸のそれぞれの軸方向への磁区に較
べて多く、磁区全体積の40%以上になつている特
許請求の範囲1の一次再結晶による電磁鋼板。
[Claims] 1% by weight, C: 0.001-0.01%, Si: 2.0-3.5
%, Mn: 0.1-0.4%, Al: 0.01-0.70%, S:
0.02% or less, the remainder consists of Fe and unavoidable impurity elements, and has the smallest angle (angle in three-dimensional space) with the rolling direction among the magnetic domains in the three-axis <100> direction of the body-centered cubic lattice crystal. An electrical steel sheet produced by primary recrystallization, in which the magnetic domain accounts for 65 to 95% of the total area. 2. The magnetic domain in the crystal axis direction that is most easily magnetized in the rolling direction is larger than the magnetic domains in the other two axis directions, and accounts for 40% or more of the total area of the magnetic domains. Electrical steel sheet produced by primary recrystallization.
JP2029978A 1978-02-23 1978-02-23 Electrical steel sheet by primary recrystallization Granted JPS54112317A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2029978A JPS54112317A (en) 1978-02-23 1978-02-23 Electrical steel sheet by primary recrystallization

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2029978A JPS54112317A (en) 1978-02-23 1978-02-23 Electrical steel sheet by primary recrystallization

Publications (2)

Publication Number Publication Date
JPS54112317A JPS54112317A (en) 1979-09-03
JPS6149380B2 true JPS6149380B2 (en) 1986-10-29

Family

ID=12023264

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2029978A Granted JPS54112317A (en) 1978-02-23 1978-02-23 Electrical steel sheet by primary recrystallization

Country Status (1)

Country Link
JP (1) JPS54112317A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06214230A (en) * 1993-01-14 1994-08-05 Koito Mfg Co Ltd Liquid crystal display device

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5012372A (en) * 1973-06-04 1975-02-07
JPS5112444A (en) * 1974-07-21 1976-01-31 Takahiro Tsubota

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5012372A (en) * 1973-06-04 1975-02-07
JPS5112444A (en) * 1974-07-21 1976-01-31 Takahiro Tsubota

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06214230A (en) * 1993-01-14 1994-08-05 Koito Mfg Co Ltd Liquid crystal display device

Also Published As

Publication number Publication date
JPS54112317A (en) 1979-09-03

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