JP3176646B2 - Manufacturing method of non-oriented electrical steel sheet for high frequency - Google Patents

Manufacturing method of non-oriented electrical steel sheet for high frequency

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Publication number
JP3176646B2
JP3176646B2 JP09562791A JP9562791A JP3176646B2 JP 3176646 B2 JP3176646 B2 JP 3176646B2 JP 09562791 A JP09562791 A JP 09562791A JP 9562791 A JP9562791 A JP 9562791A JP 3176646 B2 JP3176646 B2 JP 3176646B2
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JP
Japan
Prior art keywords
steel sheet
temperature
oriented electrical
electrical steel
high frequency
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
JP09562791A
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Japanese (ja)
Other versions
JPH05140646A (en
Inventor
守雄 塩崎
高英 島津
洋介 黒崎
孝司 棟田
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Nippon Steel Corp
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Nippon Steel Corp
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Publication of JPH05140646A publication Critical patent/JPH05140646A/en
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Publication of JP3176646B2 publication Critical patent/JP3176646B2/en
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Description

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

【0001】[0001]

【産業状の利用分野】本発明は、モータ及び小型トラン
ス用として一般に用いられる電気製品の素材であるが、
特に周波数が高い領域、即ち400Hz以上での使用に有
効な無方向性電磁鋼板である。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a material for electric products generally used for motors and small transformers.
In particular, it is a non-oriented electrical steel sheet that is effective for use in a high frequency region, that is, 400 Hz or higher.

【0002】この分野では例えば、掃除機用モータ、イ
ンバータ型エアコンや冷蔵庫用モータ、インテリジェン
トビル用の蛍光灯などの小型トランス、各種モータ、飛
行機機内用のモータや照明機器、ロボット制御用モー
タ、更には医療用の血液遠心分離器用モータなどがあ
る。
In this field, for example, motors for vacuum cleaners, motors for inverter type air conditioners and refrigerators, small transformers such as fluorescent lamps for intelligent buildings, various motors, motors and lighting devices for airplanes, motors for robot control, and more. Are motors for medical blood centrifuges.

【0003】[0003]

【従来の技術】上記利用分野は、最近急速に注目され始
めた分野であって、電気機器のエネルギー効率向上や精
密モータの厳密な位置制御などに有効なものであるが、
周波数としては400Hz以上が必要となってきた。この
ため、従来の電磁鋼板に使用される所謂、商用周波数5
0〜60Hzと違い、400Hz以上の例えば700Hzに着
目して研究しなければならないが、未だこの領域に最適
な鋼板は製造、販売されていない。例えば、無方向性電
磁鋼板の最高級品としては、Si:3%、Al:1%程
度で板厚が0.35mm、結晶粒径が150μm程度のも
のが市販されている。これは50Hzで優れた磁気特性を
有するが、高周波では満足すべき特性が得られていな
い。
2. Description of the Related Art The above-mentioned field of use is a field that has recently started attracting attention, and is effective for improving the energy efficiency of electric equipment and for strict position control of precision motors.
A frequency of 400 Hz or more has been required. For this reason, the so-called commercial frequency 5 used for the conventional electromagnetic steel sheet is used.
Unlike 0 to 60 Hz, research must be focused on 400 Hz or more, for example, 700 Hz, but a steel sheet optimal for this region has not yet been manufactured and sold. For example, as the highest grade non-oriented electrical steel sheet, those having a sheet thickness of about 0.35 mm and a crystal grain size of about 150 μm are commercially available as Si: about 3% and Al: about 1%. It has excellent magnetic properties at 50 Hz, but does not have satisfactory properties at high frequencies.

【0004】従来の考え方として、周波数が高くなれ
ば、トータル鉄損の内でうず電流損の比率が増大するこ
とが知られている。このうず電流損を小さくするために
従来、板厚を薄くし、固有抵抗を大きくすることが有効
であることが一般に知られていた。
[0004] As a conventional idea, it is known that as the frequency increases, the ratio of the eddy current loss in the total iron loss increases. Conventionally, it has been generally known that it is effective to reduce the plate thickness and increase the specific resistance in order to reduce the eddy current loss.

【0005】しかしながら、板厚を薄くするにも冷延能
力の限界があり、また固有抵抗を上昇するにもSiやA
l量には脆性の面から自ずと限界があるなど、生産上の
問題があり、またコスト的にも不利となっている。この
ため、従来、高周波用として比較的安いコストで、大量
生産する技術が市場から望まれている。
[0005] However, there is a limit to the cold rolling ability in reducing the sheet thickness, and Si or A is not effective in increasing the specific resistance.
There is a problem in production, for example, there is a limit to the amount of l from the viewpoint of brittleness, and it is disadvantageous in terms of cost. For this reason, conventionally, a technique for mass production at relatively low cost for high frequency has been desired from the market.

【0006】成分や板厚以外に結晶粒径の効果として公
知の例えば、The Physics of Meta
ls and Metallography vol.
35(1973),No.4,168〜172頁に100
〜500μmの粗大な結晶粒が鉄損を最小にすることが
知られていた。しかし、高周波領域では、このような結
晶粒径では逆に鉄損が著しく劣化する。
[0006] In addition to the composition and the plate thickness, known as the effect of the crystal grain size, for example, The Physics of Meta
ls and Metallography vol.
35 (1973), No. 100 on pages 4,168-172
It was known that coarse grains of ~ 500 [mu] m minimize iron loss. However, in the high-frequency region, the iron loss remarkably deteriorates with such a crystal grain size.

【0007】[0007]

【発明が解決しようとする課題】上記の点に鑑み、特願
平2−15755号公報で開示しているように、高周波
領域での磁気特性が優れている無方向性電磁鋼板の製品
を提供した。この内容は以下の通りである。即ち、Si
とAlの合計量が2.0〜4.0%、C≦0.005%
を含有する無方向性電磁鋼板であって、板厚0.10〜
0.25mmで、該鋼板の平均結晶粒径が5〜60μmで
ある鉄損W5/700 が12W/kg以下、磁束密度B5/700
1.0T以上の優れた磁気特性を有する周波数400Hz
以上で使用される高周波用無方向性電磁鋼板である。こ
の発明の思想は特に結晶粒径にある。結晶粒径の効果
は、従来の古典的うず電流損の計算式からは予測されな
い新規な知見であるが、400Hz以上の磁気特性には非
常に重要な意味を持つ。即ち、高周波での磁気特性を改
善させようとすれば、従来の粗大粒では駄目で細粒にし
なければならないことを示した。
In view of the above, there is provided a product of a non-oriented electrical steel sheet having excellent magnetic properties in a high frequency region as disclosed in Japanese Patent Application No. 2-15755. did. The contents are as follows. That is, Si
And Al total 2.0-4.0%, C ≦ 0.005%
A non-oriented electrical steel sheet containing
0.25 mm, the average crystal grain size of the steel sheet is 5 to 60 μm, the iron loss W 5/700 is 12 W / kg or less, and the magnetic flux density B 5/700 is 1.0 T or more.
The high-frequency non-oriented electrical steel sheet used above. The idea of the present invention lies particularly in the crystal grain size. Although the effect of the crystal grain size is a new finding that cannot be predicted from the conventional classical eddy current loss calculation formula, it has a very important meaning for the magnetic characteristics of 400 Hz or more. In other words, it has been shown that in order to improve the magnetic characteristics at high frequencies, conventional coarse grains must be used and fine grains must be used.

【0008】更に、上記の特願平2−15755号公報
記載の発明では実施例に示す製造方法を開示している。
即ち、SiとAlの合計量が2.0〜4.0%、C:
0.002%、Mn:0.30%、S:0.006%、
N:0.005%とした溶鋼を連続鋳造してスラブとな
し、熱延により2.5mm厚の熱延板とし、これを冷延
し、次いで連続焼鈍を温度650〜950℃とした後、
絶縁皮膜を塗布・焼付して製造する方法である。この製
造プロセスでは鋼板としての高周波磁気特性に優れたも
のがあるが、しかし製品鋼板にリジングと称される畳し
わ状の形状不良が発生する問題点があった。リジングが
ある場合、モータコアにこの鋼板を積層すると占積率が
著しく劣化するため商品価値がなくなる。このため、生
産側として歩留が落ちる重大な問題があった。
Further, the invention described in Japanese Patent Application No. 2-15755 discloses the manufacturing method shown in the embodiment.
That is, the total amount of Si and Al is 2.0 to 4.0%, and C:
0.002%, Mn: 0.30%, S: 0.006%,
N: Continuously cast molten steel of 0.005% to form a slab, hot-rolled into a hot-rolled sheet having a thickness of 2.5 mm, cold-rolled, and then subjected to continuous annealing at a temperature of 650 to 950 ° C.
This is a method of manufacturing by applying and baking an insulating film. In this manufacturing process, there is a steel sheet having excellent high-frequency magnetic characteristics, but there is a problem that a fold-like shape defect called ridging occurs in a product steel sheet. If there is ridging, laminating this steel sheet on the motor core will significantly reduce the space factor, and will lose commercial value. For this reason, there has been a serious problem that the yield drops as a production side.

【0009】上記問題点を解決すべく本発明者等は、製
造プロセス全体を原点に帰って見直した結果、鋼成分を
高純度化して熱延中の再結晶を促進させることにより、
熱延コイルの焼鈍を省略した場合のリジング発生を完全
に防止し、なおかつ上記、結晶粒径効果を応用させて更
に高周波磁気特性の一段と優れた無方向性電磁鋼板を開
発した。つまり本発明は、高周波特性の優れた無方向性
電磁鋼板を高位安定した歩留で生産する技術を提供する
ことを目的とする。
In order to solve the above problems, the present inventors have reviewed the entire manufacturing process from the origin, and as a result, by purifying steel components and promoting recrystallization during hot rolling,
We have developed a non-oriented electrical steel sheet that completely prevents the occurrence of ridging when the annealing of the hot-rolled coil is omitted, and further applies the above-mentioned grain size effect to further improve high frequency magnetic properties. That is, an object of the present invention is to provide a technique for producing a non-oriented electrical steel sheet having excellent high frequency characteristics at a high and stable yield.

【0010】[0010]

【課題を解決するための手段】上記目的を達成するた
め、本発明が要旨とするところは、重量比で、C≦0.
005%、Si:2.0〜4.0%、Mn:0.1〜
1.5%、P≦0.1%、S≦0.005%、Sol.
Al:0.1〜1.5%、N≦0.003%を含有する
鋼スラブを熱間圧延するに際し、仕上温度を930℃〜
1050℃とし、次いで酸洗後、冷間圧延を行い0.1
5〜0.30mmの板厚とし、続いて650〜900℃の
温度で連続焼鈍することを特徴とする高周波用無方向性
電磁鋼板の製造方法である。
In order to achieve the above object, the gist of the present invention is that the weight ratio of C ≦ 0.
005%, Si: 2.0 to 4.0%, Mn: 0.1 to
1.5%, P ≦ 0.1%, S ≦ 0.005%, Sol.
When hot rolling a steel slab containing Al: 0.1-1.5% and N ≦ 0.003%, the finishing temperature is 930 ° C.-
The temperature was adjusted to 1050 ° C., and then cold-rolled after pickling,
A method for producing a high-frequency non-oriented electrical steel sheet, characterized by a sheet thickness of 5 to 0.30 mm, followed by continuous annealing at a temperature of 650 to 900 ° C.

【0011】以下、本発明の限定理由について詳しく説
明する。 C:0.005%を越えると磁気時効の問題があるた
め、0.005%以下とする。 Si:固有抵抗を増加させるのに有効な元素があるが、
2.0%未満では固有抵抗が不十分で、4.0%を越え
ると脆性の危険性があるので2.0〜4.0%とする。 Mn:硫化物の形態を制御する。0.1%未満ではMn
Sが析出し、磁壁の移動に有害となるのが、添加量を増
やすとコスト面で不利となるので上限を1.5%とす
る。 P:これも固有抵抗を増加するが、多すぎると脆くなる
ので上限を0.1%とする。 S:有害元素である。磁壁の移動を妨げ高周波磁気特性
を劣化させると同時にリジングを発生させる為、上限を
0.005%とする。このリジングは、後述の熱延仕上
圧延完了後の再結晶をS不純物が抑制するために起きる
ものである。 Sol.Al:固有抵抗を増加させるのに有効な元素で
あるが、0.1%未満ではこの効果が不十分であり、多
すぎると添加コストの問題があるため上限を1.5%と
する。 N:これも有害元素である。磁壁の移動を妨げ高周波磁
気特性を劣化させると同時にリジングを発生させるた
め、上限を0.003%とする。このリジングは、後述
の熱延仕上圧延完了後の再結晶をN不純物が抑制するた
めに起きるものである。 その他の元素はとくに限定するものでないが、例えば
B,Sn,Sbなどを集合組織改善目的で添加すること
ができるが、添加コストの問題があるので本発明では採
用しない。
Hereinafter, the reasons for limitation of the present invention will be described in detail. C: If it exceeds 0.005%, there is a problem of magnetic aging, so the content is made 0.005% or less. Si: There is an element effective for increasing the specific resistance,
If it is less than 2.0%, the specific resistance is insufficient, and if it exceeds 4.0%, there is a risk of brittleness. Therefore, the content is set to 2.0 to 4.0%. Mn: Controls the form of sulfide. If less than 0.1%, Mn
The upper limit is set to 1.5%, since increasing the amount of S precipitates and is harmful to the movement of the domain wall. P: This also increases the specific resistance, but if too large, it becomes brittle, so the upper limit is made 0.1%. S: It is a harmful element. The upper limit is set to 0.005% in order to prevent the movement of the domain wall and deteriorate the high-frequency magnetic characteristics and at the same time generate ridging. This ridging occurs because S impurities suppress recrystallization after completion of hot-rolling finish rolling described below. Sol. Al: an element effective for increasing the specific resistance, if less than 0.1%, this effect is insufficient, and if too large, there is a problem of addition cost, so the upper limit is made 1.5%. N: This is also a harmful element. The upper limit is set to 0.003% in order to hinder the movement of the domain wall, degrade the high-frequency magnetic characteristics and simultaneously generate ridging. This ridging occurs because N impurities suppress recrystallization after the completion of hot-rolling finish rolling described below. Although other elements are not particularly limited, for example, B, Sn, Sb, etc. can be added for the purpose of improving the texture, but are not adopted in the present invention because of the problem of addition cost.

【0012】これら元素を含有するべく製鋼で成分調整
し、連続鋳造しスラブを造る。ついで熱間圧延を行う。
スラブ加熱温度は通常の950〜1280℃で実施し、
粗圧延、仕上圧延してコイルを巻き取る。この時、仕上
圧延終了温度(以下、仕上温度とする)が重要で930
℃〜1050℃が必要である。なぜなら、930℃未満
の温度では、熱延板中心厚みの部分に〈110〉±θ//
RDの繊維集合組織が発達し、熱延コイル焼鈍を省略し
た場合に最終製品でリジングと称される畳表面の縞模様
の如き形状不良が出るためである。また、仕上温度が高
すぎると最終製品で結晶粒径が大きくなりやすく、目的
の60μm以下の結晶粒が得難くなるため、1050℃
以下、好ましくは1000℃以下が必要である。巻取温
度についても特に規制しないが770℃を越えて所謂、
自己焼鈍の領域に入ると酸化層が厚くなり、次の酸洗ラ
インでの生産性が悪くなるので、770℃以下が好まし
い。熱延コイルの板厚は1.6〜2.5mm程度が冷延率
と製品集合組織の面から望ましい。
[0012] In order to contain these elements, the components are adjusted by steel making and continuously cast to produce a slab. Next, hot rolling is performed.
Slab heating temperature is carried out at the usual 950-1280 ° C,
The coil is wound by rough rolling and finish rolling. At this time, the finish rolling end temperature (hereinafter, referred to as finish temperature) is important and is 930.
C. to 1050 C. are required. Because, at a temperature lower than 930 ° C., <110> ± θ //
This is because when the fiber texture of the RD develops and the hot-rolled coil annealing is omitted, a shape defect such as a stripe pattern on the tatami mat surface called ridging appears in the final product. On the other hand, if the finishing temperature is too high, the crystal grain size tends to be large in the final product, and it is difficult to obtain the desired crystal grain of 60 μm or less.
Or lower, preferably 1000 ° C. or lower. There is no particular restriction on the winding temperature, but the temperature exceeds 770 ° C.
The temperature is preferably 770 ° C. or lower, because the oxide layer becomes thicker in the self-annealing region and the productivity in the next pickling line deteriorates. The thickness of the hot-rolled coil is desirably about 1.6 to 2.5 mm from the viewpoint of the cold-rolling rate and the product texture.

【0013】熱延コイルは通常の酸洗工程で鋼板表面ス
ケールを除去された後、熱延コイルの焼鈍を行わないで
冷延を実施する。従来、古くから無方向性電磁鋼板の高
級品に対しては、熱延コイルの焼鈍が実施されていた。
この理由は、熱延板の結晶が粒成長して結晶粒界が少な
くなり、冷延後の一次再結晶の核発生時に旧粒界から出
る〈111〉方位(磁化困難軸)粒を減らすことによる
磁気特性の向上であった。しかし、本発明の特徴である
製品結晶粒径を小さくしようとする場合、熱延コイルの
焼鈍を施すと冷延後の再結晶核が少なくなることによっ
て、製品の結晶粒径が粗大化する傾向になり発明の目的
を遂げることができない。このため熱延コイルの焼鈍は
省略すべきである。
The hot rolled coil is subjected to cold rolling without annealing the hot rolled coil after the surface scale of the steel sheet is removed in a usual pickling process. Conventionally, for a high-grade non-oriented electrical steel sheet, annealing of a hot-rolled coil has been performed for a long time.
The reason for this is that the grains of the hot-rolled sheet grow to reduce the number of crystal grain boundaries, and the number of <111> -oriented (hard-magnetization) grains coming out of the old grain boundaries during primary recrystallization after cold rolling is reduced. The magnetic properties were improved by the method. However, when trying to reduce the product crystal grain size, which is a feature of the present invention, when the hot-rolled coil is annealed, recrystallization nuclei after cold rolling are reduced, and the crystal grain size of the product tends to increase. And the purpose of the invention cannot be achieved. Therefore, annealing of the hot-rolled coil should be omitted.

【0014】冷延での仕上厚は0.15〜0.30mmで
ある。高周波特性は、製品板厚が薄ければ薄い程良くな
るが、過度に薄いと冷延破断が起きやすく、次工程の連
続焼鈍でも破断し易いため0.15mm以上とする。ま
た、0.30mmを越えると高周波特性が不満足である。
The finish thickness in cold rolling is 0.15 to 0.30 mm. The high-frequency characteristics are improved as the product thickness becomes thinner. However, if the product thickness is excessively thin, cold rolling breakage is apt to occur, and it is easy to break even in continuous annealing in the next step. If it exceeds 0.30 mm, the high frequency characteristics are unsatisfactory.

【0015】続く連続焼鈍の温度は重要で、従来の如く
高級無方向性電磁鋼板とされる焼鈍温度900〜115
0℃を採用してはならない。結晶粒径の平均は5〜60
μmが適当で、この粒径を狙って温度設定するが、その
温度は650〜900℃である。この理由は650℃未
満では再結晶が完了しないので圧延組織が鋼板中に残存
し、この内部応力が磁壁の移動の障害となり磁気特性を
劣化させる。また900℃を越えると結晶粒径が60μ
mよりも大きくなり目的を達成できない。なお、焼鈍の
均熱時間については特に規制するものではないが、5分
以内が生産性の面から適当である。以下に、本発明の実
施例について具体的に説明する。
The temperature of the subsequent continuous annealing is important, and the annealing temperature is 900 to 115, which is a conventional high-grade non-oriented electrical steel sheet.
Do not use 0 ° C. The average crystal grain size is 5-60
μm is appropriate, and the temperature is set in view of this particle size, and the temperature is 650 to 900 ° C. The reason is that recrystallization is not completed below 650 ° C., so that the rolled structure remains in the steel sheet, and this internal stress hinders the movement of the domain wall and deteriorates the magnetic properties. When the temperature exceeds 900 ° C., the crystal grain size becomes 60 μm.
m and the object cannot be achieved. The soaking time for annealing is not particularly limited, but within 5 minutes is appropriate from the viewpoint of productivity. Hereinafter, examples of the present invention will be specifically described.

【0016】[0016]

【実施例】【Example】

[実施例−1]溶鋼の成分を各種変更して、連続鋳造し
てスラブを製造した。このスラブを1120℃で加熱
し、仕上温度を940℃とした後、水冷し700℃で巻
き取った。この熱延コイル2.5mm厚を、酸洗して0.
15mm厚まで冷延した。これに680℃×90秒の連続
焼鈍をH2 +N2 混合雰囲気中で実施し絶縁皮膜を塗布
・焼付して製品となした。製品はリング状の試料片に打
抜き捲線を施した後、磁気特性を測定した。なお、磁束
密度の値は700Hzにおいて磁化力を最大値で500A
/mとした場合の最大磁束密度である。この実験内容と
結果を表1に示す。
[Example-1] A slab was manufactured by continuous casting while changing various components of molten steel. The slab was heated at 1120 ° C., the finishing temperature was set at 940 ° C., and then cooled with water and wound at 700 ° C. The hot-rolled coil of 2.5 mm thickness is pickled to a thickness of 0.1 mm.
It was cold rolled to a thickness of 15 mm. This was subjected to continuous annealing at 680 ° C. for 90 seconds in a mixed atmosphere of H 2 + N 2 , and an insulating film was applied and baked to obtain a product. The product was subjected to punching and winding on a ring-shaped specimen, and then the magnetic properties were measured. The maximum value of the magnetic flux density at 700 Hz was 500 A.
/ M is the maximum magnetic flux density. Table 1 shows the details of the experiment and the results.

【0017】[0017]

【表1】 [Table 1]

【0018】以上の如く、SiおよびSol.Alが本
発明範囲未満のそれぞれとは高周波鉄損が不満足で
ある。また、Mn,S,Nが本発明範囲を外れるそれぞ
れ,とは微小析出物が多いため高周波磁気特性が
劣化する。不純物の多い,のコイルでは一部にリジ
ングが発生して歩留を落とした。結局、本発明範囲を満
足する,との試料で高周波の700Hzで優れた鉄
損と励磁特性を示した。
As described above, Si and Sol. When the Al is less than the range of the present invention, the high frequency iron loss is unsatisfactory. Further, each of Mn, S, and N outside the range of the present invention has a large amount of fine precipitates, so that high-frequency magnetic characteristics deteriorate. In coils with many impurities, ridging occurred in part and the yield was reduced. As a result, the samples satisfying the scope of the present invention exhibited excellent iron loss and excitation characteristics at a high frequency of 700 Hz.

【0019】[実施例−2]表2の化学成分を含むスラ
ブを鋳造した。このスラブを1210℃×20分均熱で
加熱し仕上温度を変える実験を行い、巻取温度を740
℃とした。熱延コイルは全て1.9mmの厚みとし、酸洗
して0.20mm厚まで冷延した。これを、780℃×1
5秒の連続焼鈍をH2 +N2 混合雰囲気中で実施し絶縁
皮膜を塗布・焼付して製品となした。製品はリング状の
試料片に打抜き捲線を施した後、実施例−1と同様に磁
気特性を測定した。この実験内容と結果を表3に示す。
Example 2 A slab containing the chemical components shown in Table 2 was cast. An experiment was conducted in which this slab was heated at 1210 ° C. × 20 minutes soak to change the finishing temperature.
° C. All hot rolled coils were 1.9 mm thick, pickled and cold rolled to 0.20 mm thick. 780 ° C x 1
A continuous annealing for 5 seconds was performed in a H 2 + N 2 mixed atmosphere, and an insulating film was applied and baked to obtain a product. The product was subjected to punching winding on a ring-shaped sample piece, and the magnetic properties were measured in the same manner as in Example-1. Table 3 shows the details of the experiment and the results.

【0020】[0020]

【表2】 [Table 2]

【0021】[0021]

【表3】 [Table 3]

【0022】表3に示す如く、仕上温度が930℃未満
ではリジングが発生する。また、1050℃を越える
と、製品の結晶粒が大きくなって磁気特性が劣化する。
As shown in Table 3, when the finishing temperature is lower than 930 ° C., ridging occurs. On the other hand, if the temperature exceeds 1050 ° C., the crystal grains of the product become large and the magnetic properties deteriorate.

【0023】[実施例−3]表4の化学成分を含むスラ
ブを鋳造した。このスラブを1050℃×20分均熱で
加熱し仕上温度を990℃、巻取温度を700℃とし
た。熱延コイルは全て1.8mmの厚みとし、酸洗して
0.20mm厚まで冷延した。これを、連続焼鈍の温度×
均熱時間で、雰囲気を40%H2 +60%N2 のドライ
混合の条件で実施し、絶縁皮膜を塗布・焼付して製品と
なした。製品はリング状の試料片に打抜き捲線を施した
後、磁気特性を測定した。この実験内容と結果を表5に
示す。
Example 3 A slab containing the chemical components shown in Table 4 was cast. The slab was heated at 1050 ° C. for 20 minutes soaking so that the finishing temperature was 990 ° C. and the winding temperature was 700 ° C. All hot rolled coils were 1.8 mm thick, pickled and cold rolled to 0.20 mm thick. This is the temperature of continuous annealing ×
During the soaking time, the atmosphere was dry mixed with 40% H 2 + 60% N 2 , and an insulating film was applied and baked to obtain a product. The product was subjected to punching and winding on a ring-shaped specimen, and then the magnetic properties were measured. Table 5 shows the details of the experiment and the results.

【0024】[0024]

【表4】 [Table 4]

【0025】[0025]

【表5】 [Table 5]

【0026】連続焼鈍温度が、650℃未満では圧延組
織が鋼板に残り磁性が良くない。また、900℃を越え
ると粗大粒成長して磁気特性が劣化する。連続焼鈍温度
が本発明範囲の実験No.〜は、700Hzで優れた磁
気特性を示した。これらいずれの鋼板にもリジングは認
められなかった。なお、50Hzでの鉄損はの試料で良
好であったが、その他の試料では不良であった。
If the continuous annealing temperature is lower than 650 ° C., the rolled structure remains on the steel sheet and the magnetism is poor. On the other hand, when the temperature exceeds 900 ° C., coarse grains grow and the magnetic properties deteriorate. Experiment No. in which the continuous annealing temperature is within the range of the present invention. Shows excellent magnetic properties at 700 Hz. No ridging was observed in any of these steel sheets. The iron loss at 50 Hz was good for the sample, but poor for the other samples.

【0027】[0027]

【発明の効果】以上の如く本発明によれば、400Hz以
上の高周波で優れた磁気特性を有する無方向性電磁鋼板
を高位安定した歩留で製造する技術を提供するものであ
る。
As described above, according to the present invention, there is provided a technique for producing a non-oriented electrical steel sheet having excellent magnetic properties at a high frequency of 400 Hz or more at a high and stable yield.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 棟田 孝司 兵庫県姫路市広畑区富士町1番地 新日 本製鐵株式会社 広畑製鐵所内 (58)調査した分野(Int.Cl.7,DB名) C21D 8/12 C22C 38/00 303 ──────────────────────────────────────────────────の Continuing from the front page (72) Inventor Takashi Muneda 1 Fujimachi, Hirohata-ku, Himeji-shi, Hyogo Nippon Steel Corporation Hirohata Works (58) Field surveyed (Int. Cl. 7 , DB name) ) C21D 8/12 C22C 38/00 303

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 重量比で、C≦0.005%、Si:
2.0〜4.0%、Mn:0.1〜1.5%、P≦0.
1%、S≦0.005%、Sol.Al:0.1〜1.
5%、N≦0.003%を含有する鋼スラブを熱間圧延
するに際し、仕上温度を930℃〜1050℃とし、次
いで酸洗後、冷間圧延を行い0.15〜0.30mmの板
厚とし、続いて650〜900℃の温度で連続焼鈍する
ことを特徴とする高周波用無方向性電磁鋼板の製造方
法。
1. A method according to claim 1, wherein C ≦ 0.005% by weight, Si:
2.0-4.0%, Mn: 0.1-1.5%, P ≦ 0.
1%, S ≦ 0.005%, Sol. Al: 0.1-1.
When hot rolling a steel slab containing 5% and N ≦ 0.003%, the finishing temperature is set to 930 ° C. to 1050 ° C., then, after pickling, cold rolling is performed to obtain a 0.15 to 0.30 mm plate. A method for producing a high-frequency non-oriented electrical steel sheet, comprising: performing annealing at a temperature of 650 to 900 ° C.
JP09562791A 1991-04-25 1991-04-25 Manufacturing method of non-oriented electrical steel sheet for high frequency Expired - Fee Related JP3176646B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP09562791A JP3176646B2 (en) 1991-04-25 1991-04-25 Manufacturing method of non-oriented electrical steel sheet for high frequency

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP09562791A JP3176646B2 (en) 1991-04-25 1991-04-25 Manufacturing method of non-oriented electrical steel sheet for high frequency

Publications (2)

Publication Number Publication Date
JPH05140646A JPH05140646A (en) 1993-06-08
JP3176646B2 true JP3176646B2 (en) 2001-06-18

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Country Link
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005113185A (en) * 2003-10-06 2005-04-28 Nippon Steel Corp High strength silicon steel sheet excellent in magnetic property, and its production method

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005113185A (en) * 2003-10-06 2005-04-28 Nippon Steel Corp High strength silicon steel sheet excellent in magnetic property, and its production method
JP4546713B2 (en) * 2003-10-06 2010-09-15 新日本製鐵株式会社 Final product of high-strength electrical steel sheet with excellent magnetic properties, its use and manufacturing method

Also Published As

Publication number Publication date
JPH05140646A (en) 1993-06-08

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