JPH0419295B2 - - Google Patents
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- Publication number
- JPH0419295B2 JPH0419295B2 JP59188547A JP18854784A JPH0419295B2 JP H0419295 B2 JPH0419295 B2 JP H0419295B2 JP 59188547 A JP59188547 A JP 59188547A JP 18854784 A JP18854784 A JP 18854784A JP H0419295 B2 JPH0419295 B2 JP H0419295B2
- Authority
- JP
- Japan
- Prior art keywords
- iron loss
- flux density
- magnetic flux
- rolled
- less
- 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 - Lifetime
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- Soft Magnetic Materials (AREA)
Description
(産業上の利用分野)
本発明は鉄損が低くかつ磁束密度の優れた無方
向性電磁鋼板に関するものである。
(従来の技術)
無方向性電磁鋼板はモーター及び中小型変圧器
等に広く使用されているが、近年省エネルギータ
イプの電気機器の強い要請から、比較的安価な中
小型電気機器に至る迄高効率化を図るため高い磁
束密度を保ち乍ら鉄損の低い電磁鋼板の要請が益
益強まつて来ている。
かかる要望にこたえるため、鉄鋼各社でもその
開発に鋭意努力が重ねられており本発明者等もさ
きに特開昭58−151453号公報等に開示されている
如く鉄損がW15/505/50で4.5w/Kg以下で磁束密度
がB50で1.71T以上の製品の開発を行い提案して
いる。
第1図に従来成分系における鉄損値と磁束密度
の関係を示している。即ち無方向性電磁鋼板はSi
約3%の高級グレードS9から殆どSiを含まない
S60迄、グレートは多岐に亘り、Siの高い高級
品程鉄損値は低い。然し反面Si含有量が増す程磁
束密度は低下する。第1図1〜1′の曲線で示さ
れるのが従来品の製品特性範囲で折線2はJIS規
格C−2550におけるS09〜S23の限界値をむ
すぶ直線である。第1図の破線3の範囲が特開昭
58−151453号公報で提案したW15/504.5w/Kg以
下、B501.71T以上の領域であるが、Snなどの特
殊成分が添加されている。
(発明が解決しようとする問題点)
従来の無方向性電磁鋼板は低鉄損値を得るため
に磁束密度を犠性にするか、または優れた磁気特
性を得るためには高価な特殊成分を添加していた
が、本発明はSnなどの成分を添加せずに、しか
も低鉄損、高磁束密度が得られる無方向性電磁鋼
板を提供することを目的とする。
(問題点を解決するための手段)
以下本発明を具体的に説明する。
本発明はMnを高めた成分系にCuを添加するこ
とにより磁気的性質に望ましい〔100〕および
〔110〕集合組織を発達させかつ磁気特性に望まし
くない〔111〕集合組織を制御せしめて、高磁束
密度、低鉄損の電磁鋼板を提供しようとするもの
であり、特に本発明ではCuのかかる集合組織制
御効果が顕著であることを究明した点に特長があ
る。
本発明の鋼成分の限定理由について説明する。
鋼成分〔C〕は鉄損を悪化する有害な成分で、
結晶粒成長を阻害するため0.010%(成分は全て
重量%である)以下とする。
Siは周知のように鉄損値を下げる効果のある成
分で0.3%以上含有させると鉄損は向上するが一
方その含有量が増えると前述のように磁束密度を
低下させるため1.5%以下とする。
Alは脱酸剤として有効な合金であるが脱酸以
外の目的に使用する場合は固有抵抗を高めて鉄損
値を下げるため0.1%以上使用する。0.1%未満で
はAlNの生成により磁性が悪くなり、0.3%を超
えるとSi同様磁束密度を下げる。Alを脱酸のみ
の目的で使用する場合は0.1%以下とするがかか
るAl量ではAlN生成で磁性に有害なためBを添
加しBNを生成せしめAlNの生成を抑制させる必
要がある。そのためにはB/Nの比が0.5〜1.5の
範囲が最も有効であり規制した。即ちNの量に応
じてBを添加する。尚Bの量もあまり増加する
と、鋼片の割れのおそれがあるため0.005%以下
とする。
Mnは前述のように集合組織の制御に効果があ
り磁気特性を向上せしめるが0.7%未満ではその
効果が少く又、1.5%以上と高くなるとα−γ−
変態温度が低下し熱延板以降の焼鈍工程で安定し
た結晶粒成長焼鈍が行いにくい。
Cuは本発明では重要な成分であり、0.1〜1.0%
の範囲で磁気特性の向上に顕著な効果を発揮す
る。CuもMnと同様に集合組織制御に有効である
が0.1%未満では効果が少く1.0%以上では脆くな
り作業性、加工性等で問題が生じる。
上述の成分以外は鉄及び不可避的不純物であ
る。
次に本発明の特徴とするCu添加効果第2及び
第3図に基づき説明する。上記図は夫々第1表の
低Si素材へのCu添加による磁性向上を示したも
ので、第2図のAは該成分の鋼のスラブを熱間圧
延後、800℃の温度で40分保持した熱延板自己焼
鈍を行い、次いで0.50mm厚みに冷間圧延した後、
900℃の温度で40秒保持の連続仕上焼鈍を施した
製品、いわゆるフルプロセス材の磁性を表示した
ものである。同図のBは同様の自己焼鈍材を1回
の冷延工程にて0.50mm厚みにした後750℃の温度
で2時間保持の需要家焼鈍を施しした製品(いわ
ゆるセミプロセス材)の磁性を表示したものであ
る。
また、第3図のCは第2図と同様の熱延自己焼
鈍材を冷間圧延後、中間焼鈍を施し、更に4%の
スキンパスを行つた後、第2図のBと同様の需要
家焼鈍を施したセミプロセス材に係るものであ
り、同図のDは10%のスキンパス圧延を行つたセ
ミプロセス材(他の処理は第3図のCと同様)に
係るものである。
この様に製造工程が異なつたとしてもCu添加
と共に鉄損値(W15/50)は低下し、特に0.1%を境
に急激な低下を示している。
然し乍ら磁束密度(B50)については殆んど変
化なく、いづれも1.71T以上の良好な値を示して
いる。
(Industrial Application Field) The present invention relates to a non-oriented electrical steel sheet with low iron loss and excellent magnetic flux density. (Prior technology) Non-oriented electrical steel sheets are widely used in motors and small and medium-sized transformers, etc., but in recent years, due to the strong demand for energy-saving electrical equipment, high efficiency has been developed for relatively inexpensive small and medium-sized electrical equipment. Demand for electrical steel sheets with low iron loss while maintaining high magnetic flux density is increasing in order to achieve this goal. In order to meet such demands, various steel companies are making earnest efforts to develop them, and the present inventors have previously discovered that the iron loss is W 15/505 / 50 , as disclosed in Japanese Patent Application Laid-Open No. 151453/1983. We are developing and proposing a product with a magnetic flux density of B 50 and 1.71T or more at 4.5w/Kg or less. FIG. 1 shows the relationship between iron loss value and magnetic flux density in a conventional component system. In other words, non-oriented electrical steel sheet is Si
There is a wide variety of grades, from high grade S9 with about 3% to S60 which contains almost no Si, and the higher the Si content, the lower the iron loss value. However, as the Si content increases, the magnetic flux density decreases. The curves 1 to 1' in FIG. 1 show the product characteristic range of the conventional product, and the broken line 2 is a straight line connecting the limit values of S09 to S23 in JIS standard C-2550. The range of dashed line 3 in Figure 1 is JP-A-Sho.
Although it is in the range of W 15/50 4.5w/Kg or less and B 50 1.71T or more as proposed in Publication No. 58-151453, special components such as Sn are added. (Problems to be Solved by the Invention) Conventional non-oriented electrical steel sheets either sacrifice magnetic flux density in order to obtain low iron loss values, or require expensive special components to obtain excellent magnetic properties. However, an object of the present invention is to provide a non-oriented electrical steel sheet that can obtain low iron loss and high magnetic flux density without adding components such as Sn. (Means for solving the problems) The present invention will be specifically explained below. The present invention develops [100] and [110] textures that are desirable for magnetic properties and controls [111] textures that are undesirable for magnetic properties by adding Cu to a component system with increased Mn content. The present invention aims to provide an electrical steel sheet with low magnetic flux density and low iron loss, and the present invention is particularly characterized by the fact that it has been found that the texture control effect of Cu is remarkable. The reasons for limiting the steel components of the present invention will be explained. Steel component [C] is a harmful component that worsens iron loss.
In order to inhibit crystal grain growth, the content should be 0.010% or less (all components are by weight). As is well known, Si is a component that has the effect of lowering the iron loss value, and if it is contained at 0.3% or more, the iron loss will improve, but on the other hand, as its content increases, the magnetic flux density will decrease as mentioned above, so it should be kept at 1.5% or less. . Al is an effective alloy as a deoxidizing agent, but when used for purposes other than deoxidizing, use 0.1% or more to increase specific resistance and lower iron loss. If it is less than 0.1%, magnetism deteriorates due to the formation of AlN, and if it exceeds 0.3%, the magnetic flux density decreases like Si. When Al is used only for the purpose of deoxidizing, it should be 0.1% or less, but since such an amount of Al causes AlN formation, which is harmful to magnetism, it is necessary to add B to generate BN and suppress the formation of AlN. For this purpose, a B/N ratio in the range of 0.5 to 1.5 is most effective and has been regulated. That is, B is added depending on the amount of N. Furthermore, if the amount of B increases too much, there is a risk of cracking of the steel billet, so it should be kept at 0.005% or less. As mentioned above, Mn is effective in controlling texture and improves magnetic properties, but if it is less than 0.7%, the effect is small, and if it is higher than 1.5%,
The transformation temperature decreases, making it difficult to perform stable grain growth annealing in the annealing process after hot-rolled sheets. Cu is an important component in the present invention, 0.1~1.0%
It exhibits a remarkable effect on improving magnetic properties within the range of . Like Mn, Cu is effective in controlling texture, but if it is less than 0.1%, the effect is small, and if it is more than 1.0%, it becomes brittle, causing problems in workability, processability, etc. Components other than those mentioned above are iron and unavoidable impurities. Next, the effect of adding Cu, which is a feature of the present invention, will be explained based on FIGS. 2 and 3. The above figures show the improvement in magnetism due to the addition of Cu to the low-Si materials in Table 1, and A in Figure 2 shows a slab of steel with the same composition, which is held at a temperature of 800℃ for 40 minutes after hot rolling. After self-annealing the hot-rolled sheet and then cold-rolling it to a thickness of 0.50mm,
This shows the magnetism of a so-called full process material, which is a product that has been subjected to continuous finish annealing at a temperature of 900°C for 40 seconds. B in the same figure shows the magnetism of a product (so-called semi-processed material) made by applying a similar self-annealed material to a thickness of 0.50 mm in one cold rolling process and then annealing it at a temperature of 750℃ for 2 hours. This is what is displayed. In addition, C in Fig. 3 is a hot-rolled self-annealed material similar to that in Fig. 2, which is cold-rolled, intermediate annealed, and then subjected to a 4% skin pass. This relates to a semi-processed material that has been annealed, and D in the figure relates to a semi-processed material that has been subjected to 10% skin pass rolling (other treatments are the same as C in FIG. 3). Even though the manufacturing process is different in this way, the iron loss value (W 15/50 ) decreases with the addition of Cu, and shows a particularly rapid decrease after 0.1%. However, there is almost no change in magnetic flux density (B 50 ), and all of them show good values of 1.71 T or more.
【表】
以上よりCuは0.1%以上の添加により磁気特性
の向上が認められるが、作業性、加工性等の点か
ら1.0%以下が適当な範囲である。
(作 用)
次に本発明の製造条件について説明する。
前述の成分を有するスラブを通常の手段で熱間
圧延した後、700℃以上の温度で巻取り、10分〜
40分保持する自己焼鈍を施す、或は熱間圧延後
750℃以上、α−γ変態点温度以下の温度で熱延
板焼鈍を行う。そのあと通常行われる圧下率によ
り冷間圧延し製品板厚となし、変態温度以下で粒
成長のための連続焼鈍が施される所謂フルプロセ
ス材に利用される。又更にスキンパス圧延等も含
め、その後に需要家焼鈍を施すセミプロセス材に
ついても前述の様に利用し、良好な磁気特性を附
加する事が出来る。
(実施例)
(1) 第1表に示した組成にCuを0.5%添加したス
ラブを熱間圧延し830℃の温度で40分保持の自
己焼鈍を施し、圧下率78%の冷間圧延により
0.50mm厚の冷延板にし、900℃40秒で連続焼鈍
を行つたあと750℃×2時間の需要家焼鈍を行
い鉄損W15/50:3.34w/Kg磁束密度B50:1.76T
を得た。
(2) 実施例(1)と同様の熱延済鋼板を中間板厚0.52
mmまで冷間圧延し775℃×60secで中間焼鈍後、
圧下率4%のスキンパス圧延を行い0.50mmの製
品板を製造し、その後750℃×2時間の需要家
焼鈍を行い次の磁気特性を得た。
W15/50:3.24w/Kg
B50 :1.75T
(3) 実施例(1)と同じ熱延済鋼板を中間板厚0.56mm
に圧延し、その後900℃、40秒で中間焼鈍を行
い、そのあと圧下率10%のスキンパス圧延を施
し0.50mmの製品板厚とした。その後750℃×2
時間の需要家焼鈍後の磁気特性は次の通りであ
つた。
W15/50:3.05w/Kg
B50 :1.72T
(4) 第2表に示した組成の鋼スラブを熱間圧延
し、820℃の温度で60分保持の自己焼鈍を施し、
圧下率81%の冷間圧延により0.50mm厚の冷延板
にし、850℃で60秒間の連続焼鈍を行つたあと、
750℃×2時間の需要家焼鈍を行い、鉄損
W15/50:3.30w/Kg、磁束密度B50:1.78Tを得
た。
(5) 実施例(4)と同じ自己焼鈍済熱延鋼板を中間板
厚0.56mmに冷間圧延し、その後、850℃で60秒
間の中間焼鈍を行い、そのあと圧下率10%のス
キンパス圧延を施し、0.50mm厚の製品板とし
た。その後、750℃×2時間の需要家焼鈍後の
磁気特性は次の通りであつた。
W15/50:2.98W/Kg B50:1.74T[Table] From the above, it is recognized that magnetic properties are improved by adding 0.1% or more of Cu, but from the viewpoint of workability, processability, etc., 1.0% or less is an appropriate range. (Function) Next, the manufacturing conditions of the present invention will be explained. After hot-rolling the slab with the above-mentioned components by conventional means, it is rolled up at a temperature of 700°C or higher for 10 minutes or more.
Self-annealed for 40 minutes or after hot rolling
The hot rolled sheet is annealed at a temperature of 750°C or higher and lower than the α-γ transformation temperature. The material is then cold-rolled at a normal rolling reduction rate to achieve a product thickness, and is used in so-called full-process materials, which are subjected to continuous annealing for grain growth below the transformation temperature. Furthermore, semi-processed materials, including those subjected to skin pass rolling, etc., which are subsequently subjected to customer annealing, can also be used as described above, and good magnetic properties can be added to them. (Example) (1) A slab with the composition shown in Table 1 added with 0.5% Cu was hot-rolled, self-annealed at a temperature of 830°C for 40 minutes, and then cold-rolled at a reduction rate of 78%.
A cold-rolled plate with a thickness of 0.50 mm was made, and was continuously annealed at 900℃ for 40 seconds, followed by customer annealing at 750℃ for 2 hours. Iron loss W 15/50 : 3.34w/Kg Magnetic flux density B 50 : 1.76T
I got it. (2) The same hot-rolled steel plate as in Example (1) was prepared with an intermediate plate thickness of 0.52.
After cold rolling to mm and intermediate annealing at 775℃×60sec,
A product sheet of 0.50 mm was produced by skin pass rolling with a rolling reduction of 4%, and then annealed at 750°C for 2 hours to obtain the following magnetic properties. W 15/50 : 3.24w/Kg B 50 : 1.75T (3) The same hot-rolled steel plate as in Example (1) with an intermediate thickness of 0.56mm.
After that, intermediate annealing was performed at 900°C for 40 seconds, followed by skin pass rolling with a rolling reduction of 10% to give a product thickness of 0.50 mm. Then 750℃×2
The magnetic properties after customer annealing for several hours were as follows. W 15/50 : 3.05w/Kg B 50 : 1.72T (4) A steel slab with the composition shown in Table 2 was hot rolled, self-annealed at a temperature of 820℃ for 60 minutes,
After cold-rolling with a reduction rate of 81% to form a cold-rolled sheet with a thickness of 0.50 mm and continuous annealing at 850°C for 60 seconds,
Customer annealing was performed at 750°C for 2 hours to reduce iron loss.
W 15/50 : 3.30w/Kg, magnetic flux density B 50 : 1.78T were obtained. (5) The same self-annealed hot rolled steel sheet as in Example (4) was cold rolled to an intermediate thickness of 0.56 mm, then intermediate annealed at 850°C for 60 seconds, and then skin pass rolled at a rolling reduction of 10%. was applied to produce a product plate with a thickness of 0.50mm. Thereafter, the magnetic properties after customer annealing at 750°C for 2 hours were as follows. W 15/50 : 2.98W/Kg B 50 : 1.74T
【表】
以上の各実施例の磁性第1図の4で示す範囲に
プロツトした。即ち実施例1,2,3,4,5
は、それぞれ、A1,A2,A3,A4,A5である。
この図の公知例(特開昭58−151453号公報)記
載の実施例B1,B2,B3(いずれも板厚0.50mmのセ
ミプロセス材)に比し本発明材の鉄損が低く而も
磁束密度はB50で1.71T以上であることがわかる。
(発明の効果)
本発明によればSn添加なしの組成鋼により鉄
損が低く磁束密度の高い電磁鋼板が得られ、安価
で高効率化電磁鋼板の強い要求に対し十分応える
ことが出来その工業的効果は非常に大きい。[Table] The magnetic properties of each of the above examples are plotted in the range shown by 4 in FIG. That is, Examples 1, 2, 3, 4, 5
are A 1 , A 2 , A 3 , A 4 , and A 5 , respectively. The iron loss of the material of the present invention is lower than that of Examples B 1 , B 2 , and B 3 (all semi-processed materials with a plate thickness of 0.50 mm) described in the known example (Japanese Patent Application Laid-Open No. 151453/1983) in this figure. Moreover, the magnetic flux density is found to be over 1.71T at B50 . (Effects of the Invention) According to the present invention, electrical steel sheets with low core loss and high magnetic flux density can be obtained using composition steel without Sn addition, and can fully meet the strong demand for inexpensive and high-efficiency electrical steel sheets. The effect is very large.
第1図は本発明鋼と従来鋼の磁気特性を表示し
た図、第2図及び第3図は本発明鋼のCu量と磁
気特性の関係を示した図である。
FIG. 1 is a diagram showing the magnetic properties of the steel of the present invention and conventional steel, and FIGS. 2 and 3 are diagrams showing the relationship between the amount of Cu and the magnetic properties of the steel of the present invention.
Claims (1)
Mn:0.7〜1.5%、Cu:0.1〜1.0%、酸可溶性Al:
0.1〜0.3%を含み、残部はFeおよび不可避的不純
物からなることを特徴とする鉄損が低く、かつ磁
束密度の優れた無方向性電磁鋼板。 2 重量で、C:0.010%以下、Si:0.3〜1.5%、
Mn:0.7〜1.5%、Cu:0.1〜1.0%、酸可溶性Al:
0.1%以下およびB:0.005%以下を含み、かつ
B/Nが0.5〜1.5であり、残部はFeおよび不可避
的不純物からなることを特徴とする鉄損が低く、
かつ磁束密度の優れた無方向性電磁鋼板。[Claims] 1. By weight, C: 0.010% or less, Si: 0.3 to 1.5%,
Mn: 0.7~1.5%, Cu: 0.1~1.0%, acid soluble Al:
A non-oriented electrical steel sheet with low iron loss and excellent magnetic flux density, characterized by containing 0.1 to 0.3% and the remainder consisting of Fe and unavoidable impurities. 2 By weight, C: 0.010% or less, Si: 0.3-1.5%,
Mn: 0.7~1.5%, Cu: 0.1~1.0%, acid soluble Al:
Contains 0.1% or less and B: 0.005% or less, and has a B/N of 0.5 to 1.5, with the remainder consisting of Fe and unavoidable impurities, and has low iron loss.
A non-oriented electrical steel sheet with excellent magnetic flux density.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59188547A JPS6167753A (en) | 1984-09-08 | 1984-09-08 | Non-oriented silicon steel sheet with low core loss and excellent magnetic flux density |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59188547A JPS6167753A (en) | 1984-09-08 | 1984-09-08 | Non-oriented silicon steel sheet with low core loss and excellent magnetic flux density |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6167753A JPS6167753A (en) | 1986-04-07 |
| JPH0419295B2 true JPH0419295B2 (en) | 1992-03-30 |
Family
ID=16225606
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59188547A Granted JPS6167753A (en) | 1984-09-08 | 1984-09-08 | Non-oriented silicon steel sheet with low core loss and excellent magnetic flux density |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6167753A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63317627A (en) * | 1987-06-18 | 1988-12-26 | Kawasaki Steel Corp | Semiprocessing non-oriented silicon steel sheet combining low iron loss with high magnetic permeability and its production |
| US5013372A (en) * | 1987-06-18 | 1991-05-07 | Kawasaki Steel Corporation | Semi-process non-oriented electromagnetic steel strip having low core loss and high magnetic permeability, and method of making |
| JPH068489B2 (en) * | 1988-12-28 | 1994-02-02 | 新日本製鐵株式会社 | Non-oriented electrical steel sheet with excellent weldability after magnetic annealing |
| JPH086135B2 (en) * | 1991-04-25 | 1996-01-24 | 新日本製鐵株式会社 | Manufacturing method of non-oriented electrical steel sheet with excellent magnetic properties |
-
1984
- 1984-09-08 JP JP59188547A patent/JPS6167753A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6167753A (en) | 1986-04-07 |
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