JPH06248348A - Method for heat-treating high silicon steel sheet in magnetic field - Google Patents

Method for heat-treating high silicon steel sheet in magnetic field

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Publication number
JPH06248348A
JPH06248348A JP5063142A JP6314293A JPH06248348A JP H06248348 A JPH06248348 A JP H06248348A JP 5063142 A JP5063142 A JP 5063142A JP 6314293 A JP6314293 A JP 6314293A JP H06248348 A JPH06248348 A JP H06248348A
Authority
JP
Japan
Prior art keywords
magnetic field
less
steel sheet
silicon steel
high silicon
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.)
Granted
Application number
JP5063142A
Other languages
Japanese (ja)
Other versions
JP3019656B2 (en
Inventor
Yasushi Tanaka
靖 田中
Shiyaofuan Bii
シャオファン ビー
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
NKK Corp
Nippon Kokan Ltd
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 NKK Corp, Nippon Kokan Ltd filed Critical NKK Corp
Priority to JP5063142A priority Critical patent/JP3019656B2/en
Publication of JPH06248348A publication Critical patent/JPH06248348A/en
Application granted granted Critical
Publication of JP3019656B2 publication Critical patent/JP3019656B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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

Abstract

PURPOSE:To produce a high silicon steel sheet high in magnetic permeability and low in iron loss by heat treatment in a magnetic field. CONSTITUTION:As for a silicon steel sheet having a compsn. contg. 4 to 10wt.% Si or 4 to 10wt.% Si+Al and, in which preferably, the content of C, Mn, P, S, N, O or the like is regulated to prescribed one and having <=0.5mm sheet thickness and 20mum to 2.0mm average crystal grain size, the impression of a magnetic field of 1.6 to 640A/m effective magnetic field is started in the temp. range of 350 to <650 deg.C, and successively, cooling is executed to <=300 deg.C in the same magnetic field.

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、モータやトランスの鉄
心材料等に使用される高珪素鋼板の磁界中熱処理方法に
関し、透磁率が高く鉄損が低い高珪素鋼板を製造しよう
とするものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic field heat treatment method for high silicon steel sheets used as iron core materials for motors and transformers, and is intended to produce high silicon steel sheets having high magnetic permeability and low iron loss. is there.

【0002】[0002]

【従来の技術】モータやトランスの鉄心材料として広く
用いられている電磁鋼板には、通常、珪素が添加されて
いる。このように珪素が添加される理由は、珪素添加に
より電気抵抗が向上すること、磁気異方性が低下するこ
と、添加元素として安価であり、冶金学的にも安定した
相を形成すること等が挙げられる。従来、珪素は冷間圧
延が可能な3.5wt%程度を限度に鋼板に添加され、
板厚0.5〜0.1mm程度に圧延され、鉄心材料とし
て使用されてきた。一方、最近さらに多くの珪素を添加
することで磁気特性を向上させた高珪素鋼板の製造方法
が種々提案され、融体急冷法(例えば、特公昭60−3
2705号)、温間圧延法(例えば、特公平3−808
46号)、浸珪法(例えば、特公平2−60041号)
等が工業的技術として確立されている。
2. Description of the Related Art Silicon is usually added to magnetic steel sheets that are widely used as iron core materials for motors and transformers. The reason why silicon is added in this way is that the addition of silicon improves electrical resistance, decreases magnetic anisotropy, is inexpensive as an additional element, and forms a stable phase metallurgically. Is mentioned. Conventionally, silicon has been added to steel plates up to the limit of about 3.5 wt% that allows cold rolling,
It has been rolled to a plate thickness of about 0.5 to 0.1 mm and used as an iron core material. On the other hand, recently, various methods for producing a high-silicon steel sheet having improved magnetic properties by adding more silicon have been proposed, including a melt quenching method (see, for example, Japanese Examined Patent Publication No. 60-3).
2705), a warm rolling method (for example, Japanese Patent Publication No. 3-808).
46), a siliconizing method (for example, Japanese Patent Publication No. 2-60041)
Etc. are established as industrial technology.

【0003】ところで、Siが3wt%以上含まれる高
珪素鋼板の磁界中冷却効果については従来からよく知ら
れており、以下のような具体的な提案もなされている。
GoertzはSiを3〜11wt%含む鉄合金をリン
グ状に鋳込み、10Oe(800A/m)の磁界中で7
00℃から冷却することにより透磁率の改善を図ること
ができるとしている〔J. Appl. Phys.,22,(7),964,(195
1)〕。特開昭57−79120号では、超急冷薄帯を高
温で熱処理して{100}〈0kl〉あるいは{10
0}〈001〉を発達させ、特定の温度域を磁界中で熱
処理することにより磁界中焼鈍時の冷却速度を500℃
/分以上に速めても長手方向の軟磁気特性を向上させる
ことができる方法を提案している。
By the way, the effect of cooling a high silicon steel sheet containing Si in an amount of 3 wt% or more in a magnetic field has been well known, and the following concrete proposals have been made.
Goertz casts an iron alloy containing Si in an amount of 3 to 11 wt% into a ring shape and conducts it in a magnetic field of 10 Oe (800 A / m).
It is said that the magnetic permeability can be improved by cooling from 00 ° C [J. Appl. Phys., 22, (7), 964, (195
1)]. In Japanese Patent Application Laid-Open No. 57-79120, a super-quenched ribbon is heat treated at high temperature to produce {100} <0kl> or {10}.
0} <001> is developed and heat treatment is performed in a magnetic field in a specific temperature range to reduce the cooling rate during annealing in a magnetic field to 500 ° C.
It proposes a method capable of improving the soft magnetic characteristics in the longitudinal direction even if the speed is increased to more than 1 minute.

【0004】特開昭62−56527号では、100〜
200Oeの磁界を鋼板打ち抜き後に印加し、鋼板中の
析出物の状態をコントロールすることにより磁気特性を
向上させることを提案している。特開昭62−2270
79号および特開昭63−26326号においては、浸
珪法における磁界中冷却方法を提案している。これらは
連続ラインにおいて磁界を印加する方法および複数回磁
界を印加する方法を開示しており、経済的に軟磁性材料
が得られることが述べられている。特開平1−3099
22号では、方向性珪素鋼板に金属粉を含む皮膜を塗布
した後、磁界中で冷却することにより、これら金属粉の
析出物を析出させ、磁気特性を向上させる方法を提案し
ている。
In JP-A-62-56527, 100-
It has been proposed to apply a magnetic field of 200 Oe after punching a steel sheet and control the state of precipitates in the steel sheet to improve the magnetic properties. Japanese Patent Laid-Open No. 62-2270
No. 79 and Japanese Patent Laid-Open No. 63-26326 propose a cooling method in a magnetic field in a siliconizing method. These disclose a method of applying a magnetic field in a continuous line and a method of applying a magnetic field multiple times, and it is stated that a soft magnetic material can be economically obtained. Japanese Patent Laid-Open No. 1-3099
No. 22 proposes a method of applying a coating containing metal powder to a grain-oriented silicon steel sheet and then cooling it in a magnetic field to deposit precipitates of the metal powder and improve the magnetic properties.

【0005】[0005]

【発明が解決しようとする課題】しかし、これらの提案
にはそれぞれ以下のような問題がある。まず、Goer
tzによる古典的な方法は、700℃から磁界中で冷却
するものであるため、鋼帯を高温状態に加熱保持する必
要があるとともに、印加磁界も10Oe(800A/
m)と大きく、この磁界を高珪素鋼帯に印加させるため
には長大な磁場印加コイルを設備するか、或いは印加電
流値を大きく取る必要があり、このため経済性に問題が
ある。特開昭57−79120号は超急冷法によって製
造される薄帯に対する磁場中冷却方法を開示している
が、超急冷法によって製造される薄帯は先に述べたよう
な特殊な集合組織を有しており、また、超急冷法では板
幅の広い薄帯を得ることが困難で、しかも板厚精度、表
面粗度の点でも問題があり、経済的に軟磁気特性の優れ
た鋼板を得ることができない欠点がある。
However, each of these proposals has the following problems. First, Goer
Since the classical method by tz is to cool from 700 ° C. in a magnetic field, it is necessary to heat and hold the steel strip in a high temperature state, and the applied magnetic field is also 10 Oe (800 A / 800 A /
m), and in order to apply this magnetic field to the high silicon steel strip, it is necessary to install a long magnetic field applying coil or take a large applied current value, which is a problem in terms of economy. Japanese Patent Application Laid-Open No. 57-79120 discloses a magnetic field cooling method for a ribbon manufactured by the ultra-quenching method. The ribbon manufactured by the ultra-quenching method has a special texture as described above. In addition, it is difficult to obtain a thin strip with a wide sheet width by the ultra-quenching method, and there are problems in terms of sheet thickness accuracy and surface roughness. There are drawbacks that cannot be obtained.

【0006】特開昭62−56527号の方法は、析出
物の析出状態をコントロールするため、析出物を含まな
い高級電磁鋼板には適用できないという欠点がある。ま
た、印加磁界も大きく、しかも打ち抜き後の磁界印加で
あるため経済的ではない。また、特開昭62−2270
79号等の方法は、印加磁界が大きいため設備的な面で
経済性に欠けるという問題がある。特開平1−3099
22号は、析出物の析出状態をコントロールするもので
あり、これも析出物を含まない鋼板には適用できないと
いう問題があり、また、印加磁界も10Oe以上と大き
い欠点がある。本発明はこのような従来技術の問題に鑑
みなされたもので、安価で且つ安定した磁気特性を有す
る温間圧延法やSi浸透処理法(浸珪法)によって製造
された高珪素鋼板を前提とし、大きな設備的負担を伴う
ことなく経済的に高珪素鋼板の磁気特性を向上させるこ
とができる磁界中熱処理方法を提供しようとするもので
ある。
The method of Japanese Patent Laid-Open No. 62-56527 has a drawback that it cannot be applied to high-grade electrical steel sheets containing no precipitate because it controls the precipitation state of the precipitate. In addition, the applied magnetic field is large, and since the magnetic field is applied after punching, it is not economical. Also, JP-A-62-1270
The method of No. 79 and the like has a problem in that the applied magnetic field is large and the economy is poor in terms of equipment. Japanese Patent Laid-Open No. 1-3099
No. 22 controls the precipitation state of precipitates, which also has a problem that it cannot be applied to a steel sheet containing no precipitates, and the applied magnetic field has a large defect of 10 Oe or more. The present invention has been made in view of the problems of the prior art as described above, and is premised on a high silicon steel sheet manufactured by a warm rolling method or a Si infiltration treatment method (siliconizing method) that is inexpensive and has stable magnetic properties. An object of the present invention is to provide a magnetic field heat treatment method capable of economically improving the magnetic properties of a high-silicon steel sheet without a large facility burden.

【0007】[0007]

【課題を解決するための手段】高珪素鋼板の磁界中熱処
理に関しては、先に述べたように種々の方法が提案され
ている。しかしながら、効率的に磁界中熱処理の効果を
引き出すための重要な要件である磁界の強さに関して
は、特開昭62−56527号、特開昭62−2270
79号および特開昭63−26326号において10O
e(800A/m)以上の磁界を印加する方法が開示さ
れているだけである。
Various methods have been proposed for the heat treatment of a high silicon steel sheet in a magnetic field, as described above. However, regarding the strength of the magnetic field, which is an important requirement for efficiently obtaining the effect of the heat treatment in the magnetic field, JP-A-62-56527 and JP-A-62-1270.
79 and Japanese Patent Laid-Open No. 63-26326, 10O
Only the method of applying a magnetic field of e (800 A / m) or more is disclosed.

【0008】本発明者らは温間圧延法またはSi浸透処
理法により製造される高珪素鋼板について、最適な磁界
中熱処理条件、特に適正な印加磁界の強さを見出すべく
試験研究を行った。その結果、高珪素鋼板の磁気特性は
従来考えられているよりも印加磁界の弱い領域において
極めて強い印加磁界依存性を有し、しかもこの印加磁界
の弱い領域において、従来得られてきた効果よりも格段
に優れた磁気特性が得られることを見出した。また、こ
の効果は温間圧延法、Si浸透処理法という高珪素鋼板
の製造法に関わりなく得られる一般的な現象であること
が確認できた。
The inventors of the present invention conducted a test study on a high silicon steel sheet produced by a warm rolling method or a Si infiltration treatment method in order to find out the optimum heat treatment conditions in a magnetic field, particularly an appropriate applied magnetic field strength. As a result, the magnetic properties of the high silicon steel sheet have an extremely strong applied magnetic field dependency in a region where the applied magnetic field is weaker than conventionally thought, and moreover, in the region where the applied magnetic field is weaker than the effect obtained conventionally. It has been found that remarkably excellent magnetic properties can be obtained. It was also confirmed that this effect is a general phenomenon that can be obtained regardless of the method of manufacturing a high silicon steel sheet, such as the warm rolling method and the Si infiltration treatment method.

【0009】印加磁界の弱い領域で上述のような効果が
得られるということは、優れた磁気特性を有する高珪素
鋼板を製造できるというだけでなく、磁界印加のための
磁化コイルを簡略化できることを意味し、製造コスト上
も極めて有利である。このように本発明者らは、磁界中
熱処理の条件のうちで印加磁界の強弱が磁気特性に極め
て強い影響を及ぼし、従来考えられてきたよりも弱い印
加磁界において従来よりも優れた磁気特性を有する高珪
素鋼板の製造が可能になることを見出したものである。
本発明はかかる知見に基づきなされたもので、以下のよ
うな構成を有する。
The fact that the above-mentioned effects are obtained in a region where the applied magnetic field is weak means not only that a high silicon steel sheet having excellent magnetic characteristics can be manufactured, but also that the magnetizing coil for applying a magnetic field can be simplified. This means that it is extremely advantageous in terms of manufacturing cost. As described above, the inventors of the present invention have an extremely strong influence on the magnetic characteristics depending on the strength of the applied magnetic field under the conditions of the heat treatment in the magnetic field, and have the magnetic characteristics superior to the conventional one in the weaker applied magnetic field than conventionally considered. The inventors have found that it becomes possible to manufacture high silicon steel sheets.
The present invention has been made on the basis of such findings and has the following configurations.

【0010】(1) Si:4〜10wt%を含有する
高珪素鋼板を、350℃以上650℃未満の温度域にお
いて有効磁界1.6〜640A/mの磁界を印加開始
し、引き続き該磁界中で300℃以下まで冷却すること
を特徴とする高珪素鋼板の磁界中熱処理方法。 (2) Si:4〜10wt%、C:0.01wt%以
下、Mn:0.5wt%以下、P:0.01wt%以
下、S:0.01wt%以下、Sol.Al:0.20
wt%以下、N:0.01wt%以下、O:0.02w
t%以下、残部Feおよび不可避不純物からなり、板厚
0.5mm以下、平均結晶粒径20μm〜2.0mmの
高珪素鋼板を、350℃以上650℃未満の温度域にお
いて有効磁界1.6〜640A/mの磁界を印加開始
し、引き続き該磁界中で300℃以下まで冷却すること
を特徴とする高珪素鋼板の磁界中熱処理方法。 (3) Si+Al:4〜10wt%を含有する高珪素
鋼板を、350℃以上650℃未満の温度域において有
効磁界1.6〜640A/mの磁界を印加開始し、引き
続き該磁界中で300℃以下まで冷却することを特徴と
する高珪素鋼板の磁界中熱処理方法。 (4) Si+Al:4〜10wt%、C:0.01w
t%以下、Mn:0.5wt%以下、P:0.01wt
%以下、S:0.01wt%以下、Sol.Al:0.
20wt%以下、N:0.01wt%以下、O:0.0
2wt%以下、残部Feおよび不可避不純物からなり、
板厚0.5mm以下、平均結晶粒径20μm〜2.0m
mの高珪素鋼板を、350℃以上650℃未満の温度域
において有効磁界1.6〜640A/mの磁界を印加開
始し、引き続き該磁界中で300℃以下まで冷却するこ
とを特徴とする高珪素鋼板の磁界中熱処理方法。
(1) A high silicon steel sheet containing Si: 4 to 10 wt% is applied with an effective magnetic field of 1.6 to 640 A / m in a temperature range of 350 ° C. or higher and lower than 650 ° C. A method of heat treating a high silicon steel sheet in a magnetic field, characterized by cooling to 300 ° C. or less at room temperature. (2) Si: 4 to 10 wt%, C: 0.01 wt% or less, Mn: 0.5 wt% or less, P: 0.01 wt% or less, S: 0.01 wt% or less, Sol. Al: 0.20
wt% or less, N: 0.01 wt% or less, O: 0.02w
t% or less, the balance Fe and unavoidable impurities, and a high silicon steel plate having a plate thickness of 0.5 mm or less and an average crystal grain size of 20 μm to 2.0 mm in an effective magnetic field of 1.6 to A method for heat treating a high silicon steel sheet in a magnetic field, which comprises starting to apply a magnetic field of 640 A / m and subsequently cooling to 300 ° C. or less in the magnetic field. (3) A high silicon steel sheet containing Si + Al: 4 to 10 wt% is applied with a magnetic field of an effective magnetic field of 1.6 to 640 A / m in a temperature range of 350 ° C. or higher and lower than 650 ° C., and subsequently 300 ° C. in the magnetic field. A method for heat treating a high silicon steel sheet in a magnetic field, characterized by cooling to the following. (4) Si + Al: 4-10 wt%, C: 0.01w
t% or less, Mn: 0.5 wt% or less, P: 0.01 wt
% Or less, S: 0.01 wt% or less, Sol. Al: 0.
20 wt% or less, N: 0.01 wt% or less, O: 0.0
2 wt% or less, consisting of balance Fe and unavoidable impurities,
Plate thickness 0.5 mm or less, average crystal grain size 20 μm to 2.0 m
A high silicon steel sheet of m having a high temperature characterized by starting to apply a magnetic field of an effective magnetic field of 1.6 to 640 A / m in a temperature range of 350 ° C. or higher and lower than 650 ° C. and subsequently cooling it to 300 ° C. or lower in the magnetic field. Method for heat treatment of silicon steel sheet in magnetic field.

【0011】[0011]

【作用】以下、本発明の詳細をその限定理由とともに説
明する。まず、磁界中熱処理に供される高珪素鋼板の成
分組成等について説明する。この高珪素鋼板は、Siを
4〜10wt%またはSi+Alを4〜10wt%を含
有している。Siは、その添加量が略6.5wt%で磁
歪が零となり最も優れた軟磁性を示す。Siが4wt%
未満では高珪素鋼板としての所望の磁気特性が得られな
い。一方、Siが10wt%を超えると飽和磁束密度が
著しく減少する。このため、Siは4〜10wt%とす
る。
The details of the present invention will be described below together with the reasons for limitation. First, the component composition and the like of the high silicon steel sheet subjected to the heat treatment in the magnetic field will be described. This high silicon steel sheet contains 4 to 10 wt% of Si or 4 to 10 wt% of Si + Al. When Si is added in an amount of about 6.5 wt%, the magnetostriction is zero and Si exhibits the best soft magnetism. Si is 4 wt%
If it is less than the above, the desired magnetic properties as a high silicon steel sheet cannot be obtained. On the other hand, when Si exceeds 10 wt%, the saturation magnetic flux density is remarkably reduced. Therefore, Si is 4 to 10 wt%.

【0012】また、Siはその一部をAlで置換するこ
とも可能であり、この場合にはSi+Al量を規定する
必要がある。Si+Alが4wt%未満では本発明が目
的とする磁気特性が得られない。一方、Si+Alが1
0wt%を超えると飽和磁束密度が著しく減少する。こ
のため、Siの一部をAlで置換する場合には、Si+
Al:4〜10wt%とする。
Further, it is possible to replace a part of Si with Al, and in this case, it is necessary to regulate the amount of Si + Al. If Si + Al is less than 4 wt%, the magnetic characteristics aimed at by the present invention cannot be obtained. On the other hand, Si + Al is 1
When it exceeds 0 wt%, the saturation magnetic flux density is significantly reduced. Therefore, when a part of Si is replaced with Al, Si +
Al: 4-10 wt%.

【0013】次に、他の元素の好ましい含有量について
説明する。Cは軟磁性に有害な元素であり、その含有量
はできるだけ低いほうが望ましい。また、Cが0.01
wt%超えると経時的に軟磁性が劣化する所謂時効劣化
現象が生じる。このためCは0.01wt%以下とする
ことが好ましい。MnはSと結合してMnSとなり、ス
ラブ段階での熱間加工性を改善する作用がある。しか
し、Mnが0.5wt%を超えると飽和磁束密度の減少
が大きくなるため適当でない。このためMnは0.5w
t%以下とすることが好ましい。Pは軟磁気特性を劣化
させる元素であり、その含有量はできるだけ低いほうが
好ましい。経済性およびPが0.01wt%以下であれ
ば実質的にその悪影響は無視できることから、Pは0.
01wt%以下とすることが好ましい。
Next, the preferable contents of other elements will be described. C is an element harmful to soft magnetism, and its content is preferably as low as possible. Also, C is 0.01
When the content exceeds wt%, a so-called aging deterioration phenomenon occurs in which soft magnetism deteriorates with time. Therefore, C is preferably 0.01 wt% or less. Mn combines with S to become MnS, which has the effect of improving hot workability in the slab stage. However, when Mn exceeds 0.5 wt%, the saturation magnetic flux density is greatly reduced, which is not suitable. Therefore, Mn is 0.5w
It is preferably t% or less. P is an element that deteriorates soft magnetic properties, and its content is preferably as low as possible. The economic efficiency and the adverse effect can be practically neglected if P is 0.01 wt% or less, so P is 0.
It is preferable to set it to 01 wt% or less.

【0014】Sは熱間圧延時の脆性を増大させる元素で
あるとともに、軟磁気特性も劣化させるため、その含有
量はできるだけ低いほうが好ましい。この硫黄量は経済
性およびSが0.01wt%以下であれば実質的にその
悪影響は無視できることから、Sは0.01wt%以下
とすることが好ましい。Alは脱酸により鋼を清浄化す
る作用を有するとともに、磁気特性上も電気抵抗を高め
る作用を有する。Siを4〜10wt%添加する鋼で
は、Siにより磁気特性の改善を図り、Alは鋼の脱酸
作用のみを果たせばよいことから、Sol.Alは0.
20wt%以下とすることが好ましい。一方、Siの一
部をAlで置換する場合には、上述したようにSi+A
lを4〜10wt%とする。
Since S is an element that increases brittleness during hot rolling and also deteriorates soft magnetic characteristics, its content is preferably as low as possible. It is preferable that the sulfur content be 0.01 wt% or less because the sulfur content is economical and the adverse effect can be substantially ignored if the S content is 0.01 wt% or less. Al has a function of cleaning steel by deoxidation, and also has a function of increasing electric resistance in terms of magnetic characteristics. In steel containing 4 to 10 wt% of Si, Si improves the magnetic properties, and Al only has to perform the deoxidizing action of steel. Al is 0.
It is preferably 20 wt% or less. On the other hand, when replacing a part of Si with Al, as described above, Si + A
1 is 4 to 10 wt%.

【0015】Nは軟磁気特性を劣化させる元素であり、
時効による磁気特性の経時的変化も引き起こすため、そ
の含有量はできるだけ低いほうが好ましい。経済性およ
びNが0.01wt%以下であれば実質的にその悪影響
は無視できることから、Nは0.01wt%以下とする
ことが好ましい。Oは軟磁気特性を劣化させる元素であ
り、その含有量はできるだけ低いほうが好ましい。経済
性および鋼板中のO量が0.02wt%以下であれば実
質的にその悪影響は無視できることから、Oは0.02
wt%以下とすることが好ましい。以上の成分以外に、
鋼中の不可避不純物としてCr、Ni、Cu、Sn、M
o等が含まれる場合があり、これらがそれぞれ0.05
wt%程度を限度に含まれても本発明の効果は損なわれ
ない。
N is an element that deteriorates the soft magnetic characteristics,
The content thereof is preferably as low as possible because it also causes a change in the magnetic properties over time due to aging. It is preferable to set N to 0.01 wt% or less because the economical efficiency and the adverse effect thereof can be substantially ignored if N is 0.01 wt% or less. O is an element that deteriorates soft magnetic properties, and the content thereof is preferably as low as possible. If 0.02 wt% or less of O is economical and the adverse effect is practically negligible, O is 0.02%.
It is preferable to set it to wt% or less. In addition to the above ingredients,
Cr, Ni, Cu, Sn, M as unavoidable impurities in steel
o may be included, each of which is 0.05
The effect of the present invention is not impaired even if it is contained within the limit of about wt%.

【0016】これらの成分を有する高珪素鋼板は温間圧
延法、Si浸透処理法等いずれの方法で製造されるもの
でもよい。また、これらの鋼板は、板厚が0.5mm以
下、平均結晶粒径が20μm以上2.0mm以下のもの
が好ましい。板厚が0.5mmを超ると鋼板の渦電流損
失が極めて大きくなる。また、平均結晶粒径の平均結晶
粒径が20μm未満ではヒステリシス損失が増大するた
め、鉄損が大きくなり実用に適さなくなる。一方、平均
結晶粒径が2.0mmを超えると、打ち抜き性、曲げ性
等の鋼板の加工性が劣化する。
The high silicon steel sheet having these components may be manufactured by any method such as a warm rolling method and a Si infiltration treatment method. Further, these steel plates preferably have a plate thickness of 0.5 mm or less and an average crystal grain size of 20 μm or more and 2.0 mm or less. If the plate thickness exceeds 0.5 mm, the eddy current loss of the steel plate becomes extremely large. If the average crystal grain size of the average crystal grain size is less than 20 μm, the hysteresis loss increases, so that the iron loss becomes large and it becomes unsuitable for practical use. On the other hand, if the average crystal grain size exceeds 2.0 mm, the workability of the steel sheet such as punchability and bendability deteriorates.

【0017】本発明の磁界中熱処理は、上記の高珪素鋼
板の再結晶焼鈍時またはSi浸透拡散処理時、若しくは
鋼板にコーティング、スリッティング等を実施する際の
鋼板の加熱−冷却時に行うことができ、また、それ自体
独立の工程として実施してもよい。ここで、鋼板に所定
の磁界を印加開始する温度、すなわち磁界中熱処理開始
温度は350℃以上650℃未満とする。磁界中熱処理
開始温度が350℃未満であると磁界印加の効果が得ら
れず、一方、650℃以上では磁界印加により磁気特性
は向上するものの、650℃未満から磁界中熱処理を開
始した場合に較べるとその効果は劣る。このため、磁界
中熱処理開始温度は350℃以上650℃未満とする。
但し、好ましくは400〜550℃の温度域で磁界中熱
処理を開始するとその効果は一層顕著である。
The heat treatment in the magnetic field of the present invention may be carried out during recrystallization annealing of the above-mentioned high silicon steel sheet or during Si permeation diffusion treatment, or during heating / cooling of the steel sheet when coating or slitting the steel sheet. Alternatively, it may be carried out as an independent process. Here, the temperature at which a predetermined magnetic field is started to be applied to the steel sheet, that is, the heat treatment start temperature in the magnetic field is 350 ° C. or higher and lower than 650 ° C. When the heat treatment start temperature in the magnetic field is lower than 350 ° C, the effect of applying the magnetic field cannot be obtained. On the other hand, when the heat treatment temperature is 650 ° C or higher, the magnetic properties are improved by the magnetic field application, but compared with the case where the heat treatment in the magnetic field is started from lower than 650 ° C. And its effect is inferior. Therefore, the heat treatment start temperature in the magnetic field is set to 350 ° C or higher and lower than 650 ° C.
However, the effect is more remarkable when the heat treatment in the magnetic field is started preferably in the temperature range of 400 to 550 ° C.

【0018】印加磁界の大きさは、反磁界を補正した有
効磁界として1.6A/m以上、640A/m以下であ
ることが必要である。地球磁場は南北方向に通常40A
/m程度であるが、地球磁場の効果は試料の形状、向き
によって異なる。この地球磁場も勘案した有効磁界とし
て、磁界の大きさが1.6A/m未満では磁界印加の効
果は得られない。一方、640A/m超では磁界を全く
印加しない場合よりは磁気特性は向上するものの、その
磁気特性は640A/m以下の場合よりも劣り、また、
磁化コイルの長大化、印加電流の増大を招くため好まし
くない。このため、印加磁界の大きさは1.6A/m以
上、640A/m以下とする。但し、好ましくは印加磁
界を40A/m以上、320A/m以下とすればその効
果は一層顕著となる。
The magnitude of the applied magnetic field must be 1.6 A / m or more and 640 A / m or less as an effective magnetic field in which the diamagnetic field is corrected. The earth's magnetic field is normally 40A in the north-south direction.
However, the effect of the earth's magnetic field depends on the shape and orientation of the sample. If the magnitude of the magnetic field is less than 1.6 A / m, the effect of applying the magnetic field cannot be obtained as an effective magnetic field in consideration of the earth's magnetic field. On the other hand, if it exceeds 640 A / m, the magnetic characteristics are improved as compared with the case where no magnetic field is applied at all, but the magnetic characteristics are inferior to the case where it is 640 A / m or less.
This is not preferable because it causes the magnetizing coil to become longer and the applied current to increase. Therefore, the magnitude of the applied magnetic field is 1.6 A / m or more and 640 A / m or less. However, if the applied magnetic field is preferably 40 A / m or more and 320 A / m or less, the effect becomes more remarkable.

【0019】以上のようにして磁界を印加された鋼板
は、当該磁界中において300℃以下まで冷却される。
300℃を超えた温度域で磁界印加を終了すると、磁界
中熱処理による磁気特性向上効果を100%引き出すこ
とができない。磁界印加の終了温度が300℃以下であ
れば所望の磁気特性が得られる。以上述べた磁界中熱処
理の雰囲気については、非酸化性雰囲気であれば特に制
約はないが、鋼板に既にコーティングが施されており、
その焼付を兼ねた熱処理において本発明法を実施する場
合には、厳密に非酸化性である必要はなく、多少酸素濃
度が高い雰囲気であっても構わない。
The steel sheet to which the magnetic field is applied as described above is cooled to 300 ° C. or less in the magnetic field.
If the magnetic field application is terminated in the temperature range exceeding 300 ° C., the effect of improving the magnetic characteristics by the heat treatment in the magnetic field cannot be fully obtained. If the end temperature of the magnetic field application is 300 ° C. or lower, desired magnetic characteristics can be obtained. The atmosphere of the heat treatment in the magnetic field described above is not particularly limited as long as it is a non-oxidizing atmosphere, but the steel sheet has already been coated,
When the method of the present invention is carried out in the heat treatment that also serves as the baking, it is not necessary to be strictly non-oxidizing, and an atmosphere having a slightly high oxygen concentration may be used.

【0020】[0020]

【実施例】【Example】

〔実施例1〕表1に示す化学組成を有する板厚0.35
mmの高珪素鋼板を圧延法にて製造した後、リング形状
に打ち抜き、該リングに磁界印加用コイルを形成した
後、N2雰囲気中で1200℃×1時間焼鈍を行ない、
その冷却時に直流磁界を印加した。磁界が印加されてい
る温度領域での冷却速度は略100℃/分であり、ま
た、磁界中では200℃まで冷却を行った。その後、コ
イルを取り外して直流BHループを測定し、最大透磁率
を求めた。図1に磁界中熱処理時の印加磁界の大きさを
80A/m(1Oe)と800A/m(10Oe)とし
た場合について、磁界印加開始温度を900℃から20
0℃まで変化させた時の最大透磁率の変化を示す。これ
によれば、印加磁界が800A/mの場合には、400
℃から900℃までの範囲では最大透磁率に及ぼす磁界
印加開始温度の影響は小さいが、印加磁界が80A/m
と小さい場合には磁界印加開始温度の影響が強く表れ、
350℃以上650℃未満の領域において磁界印加を開
始することにより、最大透磁率の改善が図られることが
判る。また、特に磁界印加開始温度を400〜550℃
の温度域とすることにより、より一層顕著な改善効果が
得られることが判る。
[Example 1] Plate thickness 0.35 having the chemical composition shown in Table 1
After manufacturing a high-mm steel plate of mm by a rolling method, punching it into a ring shape, forming a coil for applying a magnetic field on the ring, and then annealing it at 1200 ° C. for 1 hour in an N 2 atmosphere,
A DC magnetic field was applied during the cooling. The cooling rate in the temperature range where the magnetic field was applied was about 100 ° C./min, and the cooling was performed up to 200 ° C. in the magnetic field. Then, the coil was removed and the DC BH loop was measured to determine the maximum magnetic permeability. FIG. 1 shows the case where the applied magnetic field during the heat treatment in the magnetic field was 80 A / m (1 Oe) and 800 A / m (10 Oe), the magnetic field application start temperature was from 900 ° C. to 20 ° C.
The change of the maximum magnetic permeability when changing to 0 degreeC is shown. According to this, when the applied magnetic field is 800 A / m, 400
In the range of ℃ to 900 ℃, the influence of the magnetic field application start temperature on the maximum permeability is small, but the applied magnetic field is 80 A / m
When the value is small, the effect of the magnetic field application start temperature appears strongly,
It is understood that the maximum magnetic permeability can be improved by starting the magnetic field application in the region of 350 ° C. or higher and lower than 650 ° C. In addition, especially the magnetic field application start temperature is 400 to 550 ° C.
It can be seen that a more remarkable improvement effect can be obtained by setting the temperature range to.

【0021】〔実施例2〕実施例1で用いたものと同様
の試料を用い、1200℃からの冷却時に500℃で磁
界印加を開始し、この際、印加磁界の大きさを0〜80
0A/mの範囲で変化させた。磁界を印加した例では、
磁界中で200℃まで冷却を行った。これらの試料につ
いて、実施例1と同様の方法で最大透磁率を測定した。
その結果を図2に示す。これによれば、印加磁界が小さ
いほど最大透磁率は高く、100A/m付近で最大とな
っている。同図によれば印加磁界が1.6A/m〜64
0A/mの範囲において最大透磁率が効果的に改善さ
れ、特に40A/m〜320A/mの範囲において改善
効果が顕著である。
Example 2 Using a sample similar to that used in Example 1, magnetic field application was started at 500 ° C. when cooling from 1200 ° C., and the magnitude of the applied magnetic field was 0-80.
It was changed in the range of 0 A / m. In the example of applying a magnetic field,
It cooled to 200 degreeC in the magnetic field. The maximum magnetic permeability of these samples was measured by the same method as in Example 1.
The result is shown in FIG. According to this, the smaller the applied magnetic field is, the higher the maximum magnetic permeability is, and the maximum is around 100 A / m. According to the figure, the applied magnetic field is 1.6 A / m to 64
The maximum magnetic permeability is effectively improved in the range of 0 A / m, and the improving effect is particularly remarkable in the range of 40 A / m to 320 A / m.

【0022】〔実施例3〕実施例1で用いたものと同様
の試料を用い、1200℃からの冷却時に500℃で磁
界印加(印加磁界:80A/m)を開始し、この際、冷
却速度を2000℃/分〜20℃/分の領域で変化さ
せ、磁界中で200℃まで冷却を行った。これらの試料
について、実施例1と同様の方法で最大透磁率を測定し
た。その結果を図3に示す。これによれば冷却速度は本
発明の効果に影響を及ぼさないことが判る。
Example 3 Using a sample similar to that used in Example 1, application of a magnetic field (applied magnetic field: 80 A / m) was started at 500 ° C. when cooling from 1200 ° C. Was varied in the range of 2000 ° C./min to 20 ° C./min, and cooling was performed to 200 ° C. in a magnetic field. The maximum magnetic permeability of these samples was measured by the same method as in Example 1. The result is shown in FIG. This shows that the cooling rate does not affect the effect of the present invention.

【0023】〔実施例4〕実施例1で用いたものと同様
の試料を用い、1200℃からの冷却時に500℃で磁
界印加(印加磁界:80A/m)を開始し、1分間保持
した後、引き続き磁界中で300℃まで冷却し、しかる
後300℃以下を無磁界中にて冷却した。この試料の最
大透磁率を実施例1と同様の方法で測定した結果、実施
例2で得られた最大透磁率の値と同様の値が得られた。
このことから、印加磁界中において温度を一定時間保持
しても得られる特性に変りはないこと、また、300℃
以下においては磁界印加の必要がないことが確認でき
た。
Example 4 Using a sample similar to that used in Example 1, magnetic field application (applied magnetic field: 80 A / m) was started at 500 ° C. when cooling from 1200 ° C., and after holding for 1 minute. Then, it was cooled to 300 ° C. in a magnetic field, and then cooled to 300 ° C. or less in a non-magnetic field. As a result of measuring the maximum magnetic permeability of this sample in the same manner as in Example 1, the same value as the maximum magnetic permeability value obtained in Example 2 was obtained.
From this, it can be seen that even if the temperature is maintained for a certain period of time in the applied magnetic field, the characteristics obtained do not change,
In the following, it was confirmed that it was not necessary to apply a magnetic field.

【0024】〔実施例5〕表2に示す成分組成を有する
Si浸透処理法で製造された板厚0.1mmの高珪素鋼
帯を図4に示す磁化コイルを備えた連続ラインに装入
し、コーターで絶縁皮膜を塗布した後、図5に示した熱
サイクルにて焼付処理を施した。そして、この焼付処理
時の冷却過程において、160A/m(2Oe)および
1600A/m(20Oe)の外部磁界を550℃から
印加開始し、磁界中で300℃まで冷却した。このよう
にして得られた高珪素鋼板コイルおよび磁界印加を行わ
なかった高珪素鋼板コイルから磁界印加方向にエプスタ
イン試験片を採取し、交流磁化試験により鉄損測定を行
った。その結果を図6に示す。これによれば、鉄損値は
磁界中熱処理により低減するだけでなく、明らかに磁界
の強さの影響が表れている。また、本実施例の結果か
ら、実際の連続ラインにおいても本発明の効果が確認で
きた。
[Example 5] A high silicon steel strip having a plate thickness of 0.1 mm and manufactured by the Si infiltration treatment method having the composition shown in Table 2 was charged into a continuous line equipped with a magnetizing coil shown in Fig. 4. After applying the insulating film with a coater, baking treatment was performed in the heat cycle shown in FIG. Then, in the cooling process during the baking treatment, an external magnetic field of 160 A / m (2 Oe) and 1600 A / m (20 Oe) was started to be applied from 550 ° C. and cooled to 300 ° C. in the magnetic field. Epstein test pieces were sampled in the magnetic field application direction from the high silicon steel plate coil thus obtained and the high silicon steel plate coil to which the magnetic field was not applied, and the iron loss was measured by an AC magnetization test. The result is shown in FIG. According to this, not only is the iron loss value reduced by heat treatment in a magnetic field, but the effect of the magnetic field strength is clearly shown. From the results of this example, the effect of the present invention could be confirmed even in an actual continuous line.

【0025】〔実施例6〕表3に示す成分組成を有する
板厚0.50mmの珪素鋼板を圧延法により作製した。
これら鋼板の平均結晶粒径はいずれも略0.7mmであ
った。これらの鋼板から内径19mm、外径41mmの
リングを放電加工により切り出し、磁界特性として直流
の最大透磁率および飽和磁束密度を測定した。次いで、
上記各リングに耐熱コイルを巻いた後、500℃に加熱
し、500℃から300℃までの間を磁界80A/mを
印加しながら冷却した。そして、これら試料の磁気特性
として直流の最大透磁率および飽和磁束密度を測定し
た。その結果を表4に示す。これによれば、Si単独添
加の場合およびSi+Al複合添加の場合ともに、Si
またはSi+Alが4%未満では磁界中冷却の効果は得
られない。また、SiまたはSi+Alが10%超でも
磁界中冷却の効果がなく、また、飽和磁束密度の減少が
顕著となり好ましくない。
Example 6 A silicon steel sheet having a composition shown in Table 3 and a thickness of 0.50 mm was prepared by a rolling method.
The average crystal grain size of each of these steel sheets was about 0.7 mm. A ring having an inner diameter of 19 mm and an outer diameter of 41 mm was cut out from these steel plates by electric discharge machining, and the maximum magnetic permeability of DC and the saturation magnetic flux density were measured as magnetic field characteristics. Then
After the heat resistant coil was wound around each of the above rings, it was heated to 500 ° C. and cooled between 500 ° C. and 300 ° C. while applying a magnetic field of 80 A / m. Then, the maximum magnetic permeability of DC and the saturation magnetic flux density were measured as the magnetic characteristics of these samples. The results are shown in Table 4. According to this, in the case of adding Si alone and the case of adding Si + Al composite,
Alternatively, if Si + Al is less than 4%, the effect of cooling in a magnetic field cannot be obtained. Further, even if Si or Si + Al exceeds 10%, there is no cooling effect in the magnetic field, and the saturation magnetic flux density is significantly reduced, which is not preferable.

【0026】〔実施例7〕表5に示す化学成分を有する
高珪素鋼板を圧延法により作製し、表6に示す板厚、平
均結晶粒径に調整した。これらの鋼板を450℃から有
効磁界50A/mの磁界中にて冷却し、製品とした。こ
れらの製品について、磁気特性として400Hz、1T
の鉄損値を測定するとともに、加工性の試験として三点
曲げ試験を行った。この三点曲げ試験では、ポンチを
2.0mm/分の速度で押し込んだときに割れが生ずる
押し込み距離をその指標とした。これらの結果を表7に
示す。これによれば、板厚が0.5mm超および平均結
晶粒径が20μm未満では鉄損値が極めて大きくなるこ
と、また、平均結晶粒径が2.0mmを超えると加工性
が極端に劣化することが判る。
Example 7 A high silicon steel sheet having the chemical composition shown in Table 5 was produced by a rolling method and adjusted to have the sheet thickness and average crystal grain size shown in Table 6. These steel plates were cooled from 450 ° C. in a magnetic field with an effective magnetic field of 50 A / m to obtain products. The magnetic characteristics of these products are 400Hz, 1T
The iron loss value was measured, and a three-point bending test was performed as a workability test. In this three-point bending test, the push-in distance at which cracking occurs when the punch is pushed at a speed of 2.0 mm / min is used as an index. The results are shown in Table 7. According to this, when the plate thickness exceeds 0.5 mm and the average crystal grain size is less than 20 μm, the iron loss value becomes extremely large, and when the average crystal grain size exceeds 2.0 mm, the workability is extremely deteriorated. I understand.

【0027】[0027]

【表1】 [Table 1]

【0028】[0028]

【表2】 [Table 2]

【0029】[0029]

【表3】 [Table 3]

【0030】[0030]

【表4】 [Table 4]

【0031】[0031]

【表5】 [Table 5]

【0032】[0032]

【表6】 [Table 6]

【0033】[0033]

【表7】 [Table 7]

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

【図1】印加磁界が800A/m、80A/mの各場合
について、磁界中冷却開始温度が高珪素鋼板の最大透磁
率に及ぼす影響を示すグラフ
FIG. 1 is a graph showing the influence of the cooling start temperature in a magnetic field on the maximum magnetic permeability of a high silicon steel sheet when the applied magnetic field is 800 A / m and 80 A / m, respectively.

【図2】印加磁界の大きさが高珪素鋼板の最大透磁率に
及ぼす影響を示すグラフ
FIG. 2 is a graph showing the effect of the magnitude of the applied magnetic field on the maximum magnetic permeability of a high silicon steel sheet.

【図3】磁界中冷却時の冷却速度と高珪素鋼板の最大透
磁率との関係を示すグラフ
FIG. 3 is a graph showing the relationship between the cooling rate during cooling in a magnetic field and the maximum magnetic permeability of a high silicon steel sheet.

【図4】実施例5の実施に供された連続ラインを示す説
明図
FIG. 4 is an explanatory view showing a continuous line used for carrying out Example 5.

【図5】実施例5における焼付処理の熱サイクルを示す
図面
FIG. 5 is a drawing showing a thermal cycle of baking treatment in Example 5;

【図6】実施例5における各試料の鉄損値を示すグラフFIG. 6 is a graph showing the iron loss value of each sample in Example 5.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 Si:4〜10wt%を含有する高珪素
鋼板を、350℃以上650℃未満の温度域において有
効磁界1.6〜640A/mの磁界を印加開始し、引き
続き該磁界中で300℃以下まで冷却することを特徴と
する高珪素鋼板の磁界中熱処理方法。
1. A high silicon steel sheet containing Si: 4 to 10 wt% is applied with a magnetic field of an effective magnetic field of 1.6 to 640 A / m in a temperature range of 350 ° C. or higher and lower than 650 ° C., and subsequently in the magnetic field. A method of heat treating a high silicon steel sheet in a magnetic field, characterized by cooling to 300 ° C or less.
【請求項2】 Si:4〜10wt%、C:0.01w
t%以下、Mn:0.5wt%以下、P:0.01wt
%以下、S:0.01wt%以下、Sol.Al:0.
20wt%以下、N:0.01wt%以下、O:0.0
2wt%以下、残部Feおよび不可避不純物からなり、
板厚0.5mm以下、平均結晶粒径20μm〜2.0m
mの高珪素鋼板を、350℃以上650℃未満の温度域
において有効磁界1.6〜640A/mの磁界を印加開
始し、引き続き該磁界中で300℃以下まで冷却するこ
とを特徴とする高珪素鋼板の磁界中熱処理方法。
2. Si: 4 to 10 wt%, C: 0.01 w
t% or less, Mn: 0.5 wt% or less, P: 0.01 wt
% Or less, S: 0.01 wt% or less, Sol. Al: 0.
20 wt% or less, N: 0.01 wt% or less, O: 0.0
2 wt% or less, consisting of balance Fe and unavoidable impurities,
Plate thickness 0.5 mm or less, average crystal grain size 20 μm to 2.0 m
A high silicon steel sheet of m having a high temperature characterized by starting to apply a magnetic field of an effective magnetic field of 1.6 to 640 A / m in a temperature range of 350 ° C. or higher and lower than 650 ° C. and subsequently cooling it to 300 ° C. or lower in the magnetic field. Method for heat treatment of silicon steel sheet in magnetic field.
【請求項3】 Si+Al:4〜10wt%を含有する
高珪素鋼板を、350℃以上650℃未満の温度域にお
いて有効磁界1.6〜640A/mの磁界を印加開始
し、引き続き該磁界中で300℃以下まで冷却すること
を特徴とする高珪素鋼板の磁界中熱処理方法。
3. A high silicon steel sheet containing Si + Al: 4 to 10 wt% is applied with a magnetic field of an effective magnetic field of 1.6 to 640 A / m in a temperature range of 350 ° C. or higher and lower than 650 ° C., and subsequently in the magnetic field. A method of heat treating a high silicon steel sheet in a magnetic field, characterized by cooling to 300 ° C or less.
【請求項4】 Si+Al:4〜10wt%、C:0.
01wt%以下、Mn:0.5wt%以下、P:0.0
1wt%以下、S:0.01wt%以下、Sol.A
l:0.20wt%以下、N:0.01wt%以下、
O:0.02wt%以下、残部Feおよび不可避不純物
からなり、板厚0.5mm以下、平均結晶粒径20μm
〜2.0mmの高珪素鋼板を、350℃以上650℃未
満の温度域において有効磁界1.6〜640A/mの磁
界を印加開始し、引き続き該磁界中で300℃以下まで
冷却することを特徴とする高珪素鋼板の磁界中熱処理方
法。
4. Si + Al: 4-10 wt%, C: 0.
01 wt% or less, Mn: 0.5 wt% or less, P: 0.0
1 wt% or less, S: 0.01 wt% or less, Sol. A
l: 0.20 wt% or less, N: 0.01 wt% or less,
O: 0.02 wt% or less, balance Fe and unavoidable impurities, plate thickness 0.5 mm or less, average crystal grain size 20 μm
A high silicon steel sheet having a thickness of up to 2.0 mm is applied with a magnetic field having an effective magnetic field of 1.6 to 640 A / m in a temperature range of 350 ° C. or higher and lower than 650 ° C., and subsequently cooled to 300 ° C. or lower in the magnetic field. And a method of heat treating a high silicon steel sheet in a magnetic field.
JP5063142A 1993-02-26 1993-02-26 Heat treatment method of high silicon steel sheet in magnetic field Expired - Fee Related JP3019656B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
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Application Number Priority Date Filing Date Title
JP5063142A JP3019656B2 (en) 1993-02-26 1993-02-26 Heat treatment method of high silicon steel sheet in magnetic field

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JPH06248348A true JPH06248348A (en) 1994-09-06
JP3019656B2 JP3019656B2 (en) 2000-03-13

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Country Link
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009032753A (en) * 2007-07-24 2009-02-12 Isao Sato Manufacturing method for electromagnetic steel laminated core
WO2021199400A1 (en) * 2020-04-02 2021-10-07 日本製鉄株式会社 Non-oriented electromagnetic steel sheet and method for producing same

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009032753A (en) * 2007-07-24 2009-02-12 Isao Sato Manufacturing method for electromagnetic steel laminated core
WO2021199400A1 (en) * 2020-04-02 2021-10-07 日本製鉄株式会社 Non-oriented electromagnetic steel sheet and method for producing same

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