JPH02182829A - Production of non-oriented magnetic steel plate excellent in surface property and magnetic characteristic - Google Patents

Production of non-oriented magnetic steel plate excellent in surface property and magnetic characteristic

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Publication number
JPH02182829A
JPH02182829A JP64000393A JP39389A JPH02182829A JP H02182829 A JPH02182829 A JP H02182829A JP 64000393 A JP64000393 A JP 64000393A JP 39389 A JP39389 A JP 39389A JP H02182829 A JPH02182829 A JP H02182829A
Authority
JP
Japan
Prior art keywords
rolling
slab
temperature
finish rolling
seconds
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
JP64000393A
Other languages
Japanese (ja)
Other versions
JPH0733544B2 (en
Inventor
Kazutaka Tone
和隆 東根
Masakatsu Sumimoto
住本 正勝
Yosuke Kurosaki
洋介 黒崎
Shirou Yonezono
米園 史郎
Sakae Sonoyama
園山 栄
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
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Publication date
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Priority to JP64000393A priority Critical patent/JPH0733544B2/en
Publication of JPH02182829A publication Critical patent/JPH02182829A/en
Publication of JPH0733544B2 publication Critical patent/JPH0733544B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Soft Magnetic Materials (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、電磁鋼板成品板のりジンクを消失せしめ、且
つ磁束密度の高い無方向性電磁鋼板の製造方法に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a method for manufacturing a non-oriented electrical steel sheet that eliminates glue zinc from a finished electrical steel sheet and has a high magnetic flux density.

(従来の技術) 電磁鋼板は、その用途として電動機、変圧器等の鉄芯と
して積層されることが多く、優れた電磁特性を有する事
は勿論、その他占積率、層間抵抗等が大きく影響する表
面性状も優れていることが要求される。
(Conventional technology) Electrical steel sheets are often used as a laminated iron core for electric motors, transformers, etc., and not only do they have excellent electromagnetic properties, but other factors such as space factor and interlayer resistance have a large effect on their properties. Excellent surface properties are also required.

無方向性電磁鋼板の製造にあたっては、優れた磁気特性
を得、しかも成品収率が向上する方法として、近年連続
鋳造法が多く採用されている。この連続鋳造法を利用す
ると、C,St等の偏析が少なく、均質な鋳片を製造す
る上で優れた製法である。又、従来の造塊法に比べ極め
て歩留が向上することは、周知の事実として知られてい
る。
In recent years, continuous casting has been widely adopted in the production of non-oriented electrical steel sheets as a method for obtaining excellent magnetic properties and improving product yield. When this continuous casting method is used, segregation of C, St, etc. is reduced, and it is an excellent method for producing homogeneous slabs. Furthermore, it is a well-known fact that the yield is significantly improved compared to the conventional agglomeration method.

ところがSlを1.0%以上含有する高珪素鋼板では、
最終成品にリジングとよばれる波状欠陥が発生し、これ
らは単に外観を悪くするだけでなく、積層した場合め占
積率を低下させ、実質的に成品から造られるモーターや
変圧器の特性を悪くする為、問題となっている。
However, in high-silicon steel sheets containing 1.0% or more of Sl,
A wave-like defect called ridging occurs in the final product, and these not only deteriorate the appearance, but also reduce the space factor when laminated, and essentially impair the characteristics of motors and transformers made from the product. This is a problem because of this.

このリジング発生機構については、組成の異なる相がバ
ンドを形成し、これに起因して起こる説、圧延に伴う集
合組織が関係しているという説等色々考えられていたが
、近年リジングの現出は集合組織以外の因子、すなわち
連続鋳造によって得られた鋳片の粗大柱状晶に起因して
いるという考え方が正当化されているようである。
Various theories have been proposed regarding the mechanism of this ridging, including a theory that phases with different compositions form bands, and a theory that it is caused by the texture caused by rolling, but in recent years, the appearance of ridging has been The idea that this is caused by a factor other than the texture, that is, the coarse columnar crystals of the slab obtained by continuous casting, seems to be justified.

この点については、本発明者等の長年にわたる研究から
も明らかにされており、鋳片の粗大柱状晶が熱延板に延
伸粒として多く残存すると、最終成品におけるリジング
は大きいという結果を得ている。
This point has been clarified through many years of research by the present inventors, and it has been found that if large amounts of coarse columnar crystals in the slab remain as drawn grains in the hot-rolled sheet, the ridging in the final product will be large. There is.

リジングを防止する方法として、これまでいろいろ考え
られているが、その基本的考え方は、(1)鋳片の柱状
晶率を減少させる(結晶粒微細化元素Nb等の添加、低
温鋳造、電磁攪拌中での鋳造等)こと。(2)発生した
粗大柱状晶を微細に再結晶させる(γ〜α変態の有効利
用、分塊圧延等)こと。(3)製造工程の中に焼鈍工程
を追加し、延伸粒組織を微細粒に再結晶させることであ
り、具体的方法を示すならば、特許第1102479号
に示される方法である。
Various methods have been considered to prevent ridging, but the basic idea is to (1) reduce the columnar crystallinity of the slab (addition of grain refining elements such as Nb, low-temperature casting, electromagnetic stirring, etc.). (casting inside, etc.). (2) Finely recrystallizing the generated coarse columnar crystals (effective use of γ-α transformation, blooming, etc.). (3) Adding an annealing step to the manufacturing process to recrystallize the stretched grain structure into fine grains; a specific method is the method shown in Japanese Patent No. 1102479.

その内容は連続鋳造された鋳片を1000℃−1200
℃に加熱した後、粗圧延仕上圧延を行って熱延板とする
場合に、粗最終パスを900℃以上で、且つ、50%以
上の強圧下圧延で終了し、続く仕・上圧延を850℃〜
720℃の低温領域で終えることによって、板厚方向に
均一な歪エネルギーを熱延板に蓄積し、その後の熱延板
焼鈍、又は中間焼鈍といった最終焼鈍以前の焼鈍におい
て、この歪エネルギーを再結晶駆動力として利用しよう
とするものである。
The contents are continuously cast slabs at 1000℃-1200℃.
After heating to ℃, when performing rough rolling and finish rolling to obtain a hot rolled sheet, the rough final pass is completed at 900 ℃ or higher and strong reduction rolling of 50% or higher, and the subsequent finish and top rolling is performed at 850 ℃ or higher. ℃~
By finishing in the low temperature region of 720°C, uniform strain energy is accumulated in the hot rolled sheet in the thickness direction, and this strain energy is recrystallized during subsequent hot rolled sheet annealing or intermediate annealing before final annealing. The idea is to use it as a driving force.

一般的に、Slが1.0%〜3.0%のMid−5tグ
レードの無方向性電磁鋼板は、要求鉄損レベルが厳しく
、又磁束密度の多価い材料が要求されており、このため
最終焼鈍以前に1回〜2回の焼鈍工程を付加し、鋼板の
再結晶化処理を強制的に行わせ、最終成品でのりジンク
のない、且つ高い磁束密度の無方向性電磁鋼板が造り出
されている。
In general, Mid-5t grade non-oriented electrical steel sheets with a Sl content of 1.0% to 3.0% have a strict core loss level and require a material with a high magnetic flux density. Therefore, an annealing process is added once or twice before the final annealing to force the steel sheet to undergo recrystallization treatment, resulting in a non-oriented electrical steel sheet with no glue or zinc and a high magnetic flux density. It's being served.

(発明が解決しようとする課題) しかし、最近の周辺技術の向上に従い、最終焼鈍以前に
行う焼鈍工程のみにたよらず、低鉄損で且つ高磁束密度
の磁気特性を引き出す方法の検討が始まっている。
(Problem to be solved by the invention) However, with recent improvements in peripheral technology, studies have begun on methods to bring out the magnetic properties of low iron loss and high magnetic flux density, in addition to relying only on the annealing process performed before final annealing. There is.

こういった背景の中、低コスト化への要求も厳しく、こ
の焼鈍工程を省略した製造工程が、今後の主流となる事
はまちがいのない状況となってきている。
Against this background, there is a strong demand for lower costs, and there is no doubt that manufacturing processes that omit this annealing step will become mainstream in the future.

ところが、この焼鈍工程を省略すると鋼板中の組織の再
結晶化が寸分得られず、成品でのりジンクの多発、磁束
密度の低下等の問題が起こってきているのが現状である
However, if this annealing step is omitted, the recrystallization of the structure in the steel sheet cannot be achieved to a certain extent, and problems such as frequent occurrence of adhesive zinc and a decrease in magnetic flux density have occurred in the finished product.

本発明は、上記、最終焼鈍工程以前の焼鈍工程のない製
造工程のなかで、最終成品のりジンクの発生を消滅せし
め、且つ、良好な磁束密度を得ることを可能とした製造
技術を提供するものである。
The present invention provides a manufacturing technology that eliminates the occurrence of glue zinc in the final product and makes it possible to obtain a good magnetic flux density in the manufacturing process that does not include an annealing process before the final annealing process. It is.

(課題を解決するための手段) 本発明は重量比でC: 0.02%以下、S I:1.
0〜3.0%、Mn: 0.1〜1.0%、A、Q :
1.0%以下及び残部をFeとその他の不可避不純物よ
りなる溶鋼から、得られた連続鋳造鋳片を、1000〜
1250℃の温度に加熱した後、粗圧延、仕上圧延を行
って熱延板とし、以降常法に従って一回の冷延と最終焼
鈍を行う無方向性電磁鋼板の製造法において、上記、粗
圧延開始から仕上圧延開始までの処理時間を、(1)式
X秒以上とし続く仕上圧延を750℃〜900℃の高温
領域で終えることを特徴とする表面性状に優れ、且つ磁
気特性の良好な無方向性電磁鋼板を製造する方法である
(Means for Solving the Problems) The present invention has a weight ratio of C: 0.02% or less, SI: 1.
0-3.0%, Mn: 0.1-1.0%, A, Q:
Continuously cast slabs obtained from molten steel consisting of 1.0% or less and the balance consisting of Fe and other unavoidable impurities,
In the method for producing a non-oriented electrical steel sheet in which the sheet is heated to a temperature of 1250°C, rough rolling and finish rolling are performed to obtain a hot rolled sheet, and thereafter cold rolling and final annealing are performed once according to a conventional method. The process time from the start to the start of finish rolling is longer than (1) X seconds, and the finish rolling is finished in a high temperature range of 750 to 900 °C. This is a method for manufacturing grain-oriented electrical steel sheets.

X(秒)−[130−鋳片等軸晶率(%)〕……(1)
式更に本発明はC: 0.02%以下、Sl:1.0〜
3.0%、Mn: 0.1−1.0%、Afl:1.0
%以下を含み、且ツB : 0.0003〜0.005
0%を含有し残部をFeとその他の不可避不純物よりな
る溶鋼から得られた連続鋳造鋳片を用いる表面性状に優
れ、且つ磁気特性の良好な無方向性電磁鋼板を製造する
方法である。
X (seconds) - [130 - Equiaxed crystallinity of slab (%)]... (1)
Furthermore, the present invention has C: 0.02% or less, Sl: 1.0~
3.0%, Mn: 0.1-1.0%, Afl: 1.0
% or less, and B: 0.0003 to 0.005
This method uses continuously cast slabs obtained from molten steel containing 0% Fe and the balance consisting of Fe and other unavoidable impurities to produce non-oriented electrical steel sheets with excellent surface properties and good magnetic properties.

以下本発明の詳細な説明する。The present invention will be explained in detail below.

第1図は鋳片等軸晶率の算出方法を示したものである。FIG. 1 shows a method for calculating the equiaxed crystallinity of a slab.

第2図写真A、Bは粗圧延を終了した仕上圧延前バーの
金相写真(L断面)を示したもので、鋳片等軸晶率30
%のものを出発素材とし、粗圧延開始から仕上圧延開始
までの時間は、写真Aが80秒、写真Bが105秒の場
合である。
Photos A and B in Figure 2 show metal phase photos (L cross section) of the bar before finish rolling after rough rolling.
% is used as the starting material, and the time from the start of rough rolling to the start of finish rolling is 80 seconds in Photo A and 105 seconds in Photo B.

この写真Aにみられるとおり、粗圧延開始から仕上圧延
開始までの時間が80秒と短いものは、バー厚の中心付
近に微細に結晶化した組織が板厚の約40%程度の領域
に存在し、残りの部分の大半には鋳片組織でみられた柱
状晶組織が、そのまま圧延中に延ばされて残ったと考え
られる延伸粒が観察される。
As seen in photo A, when the time from the start of rough rolling to the start of finish rolling is as short as 80 seconds, there is a finely crystallized structure near the center of the bar thickness in an area of about 40% of the plate thickness. However, in most of the remaining parts, elongated grains are observed, which are thought to have remained after the columnar crystal structure seen in the slab structure was stretched as it was during rolling.

この延伸粒が、成品まで残るとりジンクとなることは、
すでに多くの文献で説明されており、公知の事実である
The fact that these drawn grains become the zinc that remains until the finished product is
This has already been explained in many documents and is a well-known fact.

これに対して写真Bに示した如く、粗圧延開始から仕上
圧延開始までの時間を105秒としたものは、バー厚の
ほぼ全厚にわたって、微細に結晶化した組織が広がって
いることがわかる。
On the other hand, as shown in Photo B, when the time from the start of rough rolling to the start of finish rolling was 105 seconds, it can be seen that a finely crystallized structure spreads over almost the entire thickness of the bar. .

このような一定の等軸晶率に対して、粗圧延開始から仕
上圧延開始までの時間を増減することに゛よって、延伸
粒の残存比率を制御できることを見い出したわけである
It has been discovered that the remaining ratio of drawn grains can be controlled by increasing or decreasing the time from the start of rough rolling to the start of finish rolling with respect to such a constant equiaxed crystal ratio.

この現象は、次のようなメタラジ−で起こると考えられ
る。
This phenomenon is thought to occur in the following metallurgy.

Slを1.0%から3.0%含有する極低炭素鋼は、9
00℃付近に変態点を持っている。そしてこれらの材料
は、磁気特性の重要な要素である磁束密度を高めるため
に、仕上圧延温度を750℃〜900℃の間で行わせる
必要があり、このためには、粗圧延温度を900℃〜1
100℃の温度領域で行わせる必要がある。
Ultra-low carbon steel containing 1.0% to 3.0% Sl is 9
It has a transformation point around 00℃. In order to increase the magnetic flux density, which is an important element of magnetic properties, these materials need to be finished rolled at a temperature between 750°C and 900°C. ~1
It is necessary to carry out the process in a temperature range of 100°C.

つまりこの粗圧延温度領域は、変態域に突入していく領
域にあり、微細に結晶化し易い領域と言うことが出来よ
う。しかしこの温度領域に制御するだけでは、バー厚全
厚から、延伸粒を消滅させることは不可能であった。又
これ以上の低温側に粗圧延温度を低下すると、仕上温度
が750℃から900℃に確保出来ない問題もある。
In other words, this rough rolling temperature region is a region entering the transformation region, and can be said to be a region where fine crystallization is likely to occur. However, by simply controlling the temperature within this range, it was impossible to eliminate the stretched grains from the entire bar thickness. Further, if the rough rolling temperature is lowered to a lower temperature than this, there is a problem that the finishing temperature cannot be maintained from 750°C to 900°C.

すなわち、900℃から1100℃の温度領域で鋳片か
らバー厚までの大圧下量をかけ、数回におよぶバス圧延
の間に、粗圧延での圧下による歪エネルギーを核として
起こる延伸粒の破砕現象を、バス間毎の時間を成る値よ
りも大きく持つことによって積極的に行わせ、これによ
り仕上圧延前のバー厚状態で、全厚にわたって延伸粒を
消滅させることが可能となるわけである。
In other words, a large amount of reduction is applied from the slab to the bar thickness in the temperature range of 900°C to 1100°C, and during several times of bus rolling, the fracture of the drawn grains occurs due to the strain energy caused by the reduction during rough rolling. This phenomenon can be actively caused by making the time between each bath longer than the value, and this makes it possible to eliminate stretched grains over the entire thickness of the bar before finish rolling. .

第3図は、鋳片等軸晶率が30%の鋳片に対して、粗圧
延開始から仕上圧延開始までの時間を広範囲にとり、そ
の時間と成品リジング評点との関係を示したものである
Figure 3 shows the relationship between the time and the finished product ridging score over a wide range of times from the start of rough rolling to the start of finish rolling for a slab with an equiaxed grain ratio of 30%. .

このリジング評点とは最終成品のC断面の表面の凹凸の
ギャップ量をμ単位で読み取ったもので、A:く4μ、
B :4.0〜5,4μ、C:5.5〜6.9μ、D=
>6.9μと判定したものであり、需要家との長年の経
験から、Bまでを出荷可能としている。
This ridging rating is the gap amount of the unevenness on the surface of the C section of the final product read in μ units, A: 4μ,
B: 4.0~5.4μ, C: 5.5~6.9μ, D=
>6.9μ, and based on many years of experience with customers, it is possible to ship products up to B.

本例において合格評点A、Bを得ようとすれば、粗圧延
開始から仕上圧延開始までの時間を100秒必要とする
ことがわかる。
It can be seen that in order to obtain passing grades A and B in this example, a time of 100 seconds is required from the start of rough rolling to the start of finish rolling.

次にこの粗圧延開始から仕上圧延開始までの時間による
延伸粒の破砕効果が鋳片の等軸晶率にどう影響されるか
を第4図に示す。
Next, FIG. 4 shows how the effect of crushing the drawn grains depending on the time from the start of rough rolling to the start of finish rolling is influenced by the equiaxed crystallinity of the slab.

第4図にみられるとおり、鋳片の等軸晶率の高いものは
短い時間で、そして低いものは長い時間を必要としてく
る事がわかる。これは成品リジングを発生させる延伸粒
が、鋳片段階での柱状晶の度合いに比例しており、この
部分が少なければ、それだけ粗圧延開始から仕上圧延開
始までの時間による延伸粒の破砕効果が少なくてすむこ
とを意味しているわけである。
As seen in Figure 4, it can be seen that a slab with a high equiaxed crystallinity requires a short time, and a slab with a low equiaxed crystallinity requires a long time. This is because the drawn grains that cause product ridging are proportional to the degree of columnar crystals in the slab stage, and the smaller this portion is, the more the effect of crushing the drawn grains due to the time from the start of rough rolling to the start of finish rolling will be reduced. This means that less is required.

本発明者らは、この鋳片等軸晶率と、粗圧延開始時間か
ら仕上圧延開始までの時間と成品リジングとの間に、あ
る関係があることを見出したわけである。そしてこの関
係を実験結果をもとに数式にしたものが(1)式である
The present inventors have discovered that there is a certain relationship between the equiaxed crystallinity of the slab, the time from the start of rough rolling to the start of finish rolling, and the ridging of the finished product. Equation (1) is a mathematical expression of this relationship based on experimental results.

X(秒)−(130−鋳片等軸晶率(%)〕……(1)
式つまり、鋳片の等軸晶率が0%の時は、この粗圧延開
始から仕上圧延開始までの時間を130秒以上にするこ
とで、成品のりジンク評点をB以下の良好なものにする
ことが可能であり、又、鋳片の等軸品率が70%の時は
、この粗圧延開始から仕上圧延開始までの時間を60秒
以上にすることで、成品のりジンク評点をB以下の良好
なものにすることが可能である。
X (seconds) - (130 - Equiaxed crystallinity of slab (%))... (1)
In other words, when the equiaxed crystallinity of the slab is 0%, by setting the time from the start of rough rolling to the start of finish rolling to 130 seconds or more, the finished product has a good zinc rating of B or below. In addition, when the equiaxed product ratio of the slab is 70%, by setting the time from the start of rough rolling to the start of finish rolling to be 60 seconds or more, the zinc rating of the finished product can be lower than B. It is possible to make it good.

このように、 (1)式を満足するX秒以上の粗圧延開
始から仕上圧延開始までの時間を確保することで、成品
のりジンクの発生を防止できるわけである。
In this way, by ensuring the time from the start of rough rolling to the start of finish rolling of X seconds or more that satisfies formula (1), it is possible to prevent the occurrence of glue zinc in the finished product.

実際に得られる鋳片の等軸品率は、電磁攪拌装置の普及
および鋳造温度制御技術の向上によって、現在O%から
100%まで可能であるが、鋳造の安定性、設備コスト
の関係から、実際には0%から70%までの範囲で製造
されている。
Due to the widespread use of electromagnetic stirrers and improvements in casting temperature control technology, the equiaxed product ratio of slabs actually obtained is currently possible from 0% to 100%, but due to the stability of casting and equipment costs, In reality, it is produced in a range of 0% to 70%.

次に、仕上温度と磁束密度との関係を第5図に示す。Next, FIG. 5 shows the relationship between finishing temperature and magnetic flux density.

第5図にみられるとおり、熱延板焼鈍を組み込んでいる
工程においては、仕上温度による磁束密度への影響はみ
られないが、熱延板焼鈍、又は最終焼鈍以前に焼鈍を行
わない場合は、この仕上温度と磁束密度との間には相関
関係が見られ、仕上温度が低下する程、磁束密度は劣化
する。
As shown in Figure 5, in processes that incorporate hot-rolled plate annealing, there is no effect on magnetic flux density due to finishing temperature, but in cases where hot-rolled plate annealing or no annealing is performed before final annealing, There is a correlation between the finishing temperature and the magnetic flux density, and the lower the finishing temperature, the worse the magnetic flux density becomes.

この材料は、900℃前後に変態点をもっており、90
0℃を境に低温域ではα相となっている。このα相の内
では、極力高温で保持される時間を長く保つことによっ
て、磁束密度を向上させる方位が鋼板中に増加していく
This material has a transformation point around 900℃,
In the low temperature range below 0°C, it is in the α phase. Within this α phase, by keeping the temperature as high as possible for as long as possible, orientations that improve the magnetic flux density increase in the steel sheet.

すなわち、仕上温度を750℃から900℃の高温域で
処理することによって、熱延板の方位をつかさどる集合
組織を改善し、熱延板焼鈍の省略を可能とせしめたわけ
である。
That is, by processing the hot-rolled sheet at a high finishing temperature of 750° C. to 900° C., the texture that controls the orientation of the hot-rolled sheet is improved, making it possible to omit hot-rolled sheet annealing.

ここで、仕上温度の上限を900℃に限定したが、この
範囲内で極力高い温度が磁束密度に対して良いことは言
うまでもない。
Here, the upper limit of the finishing temperature was limited to 900° C., but it goes without saying that a temperature as high as possible within this range is good for magnetic flux density.

次に本発明における構成要件の限定理由についてのべる
Next, the reasons for limiting the constituent elements of the present invention will be described.

珪素鋼中のC量が0602%を超えると、成品でのCi
lを低減させるために長時間の脱炭焼鈍工程が必要とな
り、著しく生産性を悪化させるばかりでなく、磁気特性
を悪化させる為、本発明においては鋼中Cilを0.0
2%に限定した。
When the amount of C in silicon steel exceeds 0.602%, the amount of Ci in the finished product is
In order to reduce Cil, a long decarburization annealing process is required, which not only significantly deteriorates productivity but also deteriorates magnetic properties. Therefore, in the present invention, Cil in steel is set to 0.0.
It was limited to 2%.

5ljtについては、所要の鉄損であるW15150で
<4.8W/kgを目標としており、Slの下限値を、
1.0%以上とした。一方、上限値については、通板性
を考慮し、3.0%とした。
For 5ljt, the target is <4.8W/kg at W15150, which is the required iron loss, and the lower limit of Sl is
The content was set to 1.0% or more. On the other hand, the upper limit was set at 3.0% in consideration of threadability.

Mnについては、鋼板の硬度を増加させ、打抜き性を改
善する5ため添加するが、上限値の1.0%は経済的理
由によるものである。又、下限値については、その効力
が少なくなる0、1%とした。
Mn is added to increase the hardness of the steel sheet and improve punchability, but the upper limit of 1.0% is for economic reasons. Furthermore, the lower limit value was set at 0.1%, which would reduce its effectiveness.

Alについても、珪素鋼の固有抵抗増加による鉄損向上
のために添加する元素であるが、添加しすぎると板の冷
延性を阻害することと、経済的理由によるもので、上限
値を1.0%とした。
Al is also an element added to improve iron loss by increasing the specific resistance of silicon steel, but if added too much, it will impede the cold rollability of the plate, and for economic reasons, the upper limit has been set at 1. It was set to 0%.

また、むしろ析出分散相として、粒成長を阻害するAg
Nの析出を防止し、鉄損を改善させる材料の場合は、A
lをT「にして製造しており、どちらのケースにも応用
可能な技術である為0、範囲を1.0%以下とした。
In addition, Ag, which inhibits grain growth, acts as a precipitated dispersed phase.
For materials that prevent N precipitation and improve iron loss, A
Since the technology is applicable to both cases, the range is set to 0 and the range is 1.0% or less.

鉄損を出す為には、焼鈍工程での1次粒成長を利用して
成品の結晶粒径を20〜100μまでに大きくして、所
定の鉄損を出すわけであるが、加熱温度が高いとMnS
、AffN等の析出分散相が溶体化し、熱延工程で析出
し、上記焼鈍工程での1次粒成長を阻害して、磁性不良
となる。
In order to produce iron loss, the primary grain growth in the annealing process is used to increase the crystal grain size of the finished product to 20 to 100μ to produce the specified iron loss, but the heating temperature is high. and MnS
, AffN, and the like become a solution, precipitate during the hot rolling process, inhibit primary grain growth during the annealing process, and result in poor magnetic properties.

そこで加熱炉温度は上限値を1250℃に限定した。Therefore, the upper limit of the heating furnace temperature was limited to 1250°C.

下限値については、圧延荷重の能力から1000℃とし
た。
The lower limit was set at 1000° C. based on the rolling load capacity.

本発明は、熱延板となった以降、最終焼鈍工程以前に焼
鈍工程を含まない製造工程のものに限定したが、このよ
うな焼鈍工程を一部省略した方法では、所定の磁束密度
が出にくいため、磁束密度が出やすい温度領域を限定し
た。
Although the present invention is limited to manufacturing processes that do not include an annealing process after the hot-rolled sheet is produced and before the final annealing process, a method that partially omits such an annealing process will not produce a predetermined magnetic flux density. Therefore, we limited the temperature range where magnetic flux density is likely to occur.

750℃未満では十分な磁束密が得られない。また90
0℃超では、仕上圧延機内でa域とγ域との2層域圧延
となり、極めて圧延性が悪化すること、及び磁束密が飽
和してしまうことにより、上限温度を900℃とした。
If the temperature is lower than 750°C, sufficient magnetic flux density cannot be obtained. 90 again
If it exceeds 0°C, rolling will occur in the two-layer region of a region and γ region in the finishing rolling mill, resulting in extremely poor rolling properties and saturated magnetic flux density, so the upper limit temperature was set at 900°C.

析出分散相であるAINは、成品の粒成長を著しく阻害
することは周知の事実であるが、これを防ぐためにはN
と親和力の強いBを添加し、鋼中にBNを生成させ、i
と反応するNを取り除く。
It is a well-known fact that AIN, which is a precipitated dispersed phase, significantly inhibits the grain growth of finished products, but in order to prevent this, N
By adding B, which has a strong affinity with
Remove N that reacts with

本発明は、これらB添加の効果を発揮させるため、Bの
範囲を0.0003%から0.0050%とした。下限
の0.0003%未満となると、上記B添加の効果が発
揮されなくなり、又、上限の0.0050%については
経済的理由によるものである。
In the present invention, in order to exhibit the effects of B addition, the range of B is 0.0003% to 0.0050%. If it is less than the lower limit of 0.0003%, the effect of B addition will not be exhibited, and the upper limit of 0.0050% is due to economic reasons.

(実施例1) 重量比でC: 0.0025%、S i:1.5%、M
n:0.25%、P : 0.02%、s :o、oo
a%、5o11.Afl : 0.33%で、残部を鉄
及び不可避不純物よりなる溶鋼を、湾曲型連続鋳造機に
て鋳造し、250m+*厚の鋳片を鋳造した。この鋳片
を出発素材に、1100℃の温度に加熱した後、粗圧延
開始から仕上圧延開始までの時間を第1表に示すように
変更した。
(Example 1) Weight ratio: C: 0.0025%, Si: 1.5%, M
n: 0.25%, P: 0.02%, s: o, oo
a%, 5o11. Molten steel with Afl: 0.33% and the balance consisting of iron and unavoidable impurities was cast using a curved continuous casting machine to cast a slab with a thickness of 250 m+*. After heating this slab as a starting material to a temperature of 1100° C., the time from the start of rough rolling to the start of finish rolling was changed as shown in Table 1.

特に、鋳片については、電磁攪拌装置を使用し、鋳片内
部の等軸品比率を変化させ、熱延条件との相関関係を評
価してみた(10%以上は鋳片電磁攪拌装置を使用した
)。
In particular, for slabs, we used an electromagnetic stirrer to change the proportion of equiaxed parts inside the slab and evaluated the correlation with hot rolling conditions (for slabs of 10% or more, an electromagnetic stirrer was used). did).

鋳片の等軸晶率、熱延条件、熱延以降通板条件、成品の
りジンク、磁気特性結果、総合判定を同じく第1表に示
す。
Table 1 also shows the equiaxed crystallinity of the slab, hot rolling conditions, passing conditions after hot rolling, finished product paste zinc, magnetic property results, and overall evaluation.

比較例1は、鋳片等軸晶率を0から70%に変化させた
ものを出発材料として粗圧延開始から仕上圧延開始まで
の時間を第1表に示すように、(1)式より算出される
値よりも少なくしたものの結果であるが、みられるとお
りいずれの等軸品のものも、成品で問題となる評点C以
上のりジンクが発生している。
In Comparative Example 1, the time from the start of rough rolling to the start of finish rolling was calculated using equation (1) as shown in Table 1 using a slab whose equiaxed crystallinity was changed from 0 to 70% as a starting material. As can be seen, all of the equiaxed products had adhesive zinc with a rating of C or higher, which is a problem in finished products.

尚、磁束密度については、本発明の温度範囲で仕上圧延
を実施しており良好な結果が得られた。
As for the magnetic flux density, finish rolling was performed within the temperature range of the present invention, and good results were obtained.

(実施例2) fifft比でC: 0.0025%、S 1:1.5
%、Mn:0.25%、P : 0.02%、S :0
.003%、sol、Afl : 0.03%、B :
 0.0020%で、残部を鉄及び不可避不純物よりな
る溶鋼を湾曲型連続鋳造機にて鋳造し、250mm厚の
鋳片を鋳造した。この鋳片を出発素材に、内部の等軸晶
比率を変化させ、熱延条件との相関関係を評価してみた
(10%以上は鋳片電磁攪拌装置を使用した)。
(Example 2) fift ratio: C: 0.0025%, S: 1:1.5
%, Mn: 0.25%, P: 0.02%, S: 0
.. 003%, sol, Afl: 0.03%, B:
Molten steel with a concentration of 0.0020% and the remainder consisting of iron and unavoidable impurities was cast using a curved continuous casting machine to cast a slab with a thickness of 250 mm. Using this slab as a starting material, the internal equiaxed crystal ratio was varied and the correlation with hot rolling conditions was evaluated (for 10% or more, a slab electromagnetic stirrer was used).

鋳片の等軸晶率、熱延条件、熱延以降通板条件、成品の
りジンク、磁気特性結果、総合判定を同じく第2表に示
す。
Table 2 also shows the equiaxed crystallinity of the slab, hot rolling conditions, passing conditions after hot rolling, finished product paste zinc, magnetic property results, and overall evaluation.

を満足する時間に制御し、特に仕上圧延温度を700℃
から1000℃間で変化させた。
In particular, the finish rolling temperature is controlled at 700°C.
The temperature was varied between 1000°C and 1000°C.

鋳片については、電磁攪拌装置を使用し、鋳片比較例2
は、鋳片の等軸品率を0から50%に水準を振り、各々
の鋳片の等軸品率の値から、(1)式を満足する粗圧延
開始から仕上圧延開始までの時間を確保した上で、仕上
圧延温度を750℃以下のものと、900℃以上の領域
に水準を振り、実験を行った結果を示す。
For slabs, an electromagnetic stirring device was used, and slab comparison example 2 was prepared.
The equiaxed product ratio of the slab is scaled from 0 to 50%, and from the value of the equiaxed product ratio of each slab, the time from the start of rough rolling to the start of finish rolling that satisfies equation (1) is calculated. After ensuring this, the results of experiments were conducted with finishing rolling temperatures ranging from 750°C or lower to 900°C or higher.

第2表にみられるとおり750℃以下の場合は磁束密度
が著しく低下している。。また、900℃以上の場合に
は、磁束密度は良好材と同等レベルのものが得られるも
のの、仕上圧延の通板性が、二相域圧延となって不安定
となった。
As shown in Table 2, when the temperature is 750° C. or lower, the magnetic flux density decreases significantly. . Further, when the temperature was 900° C. or higher, although a magnetic flux density equivalent to that of the good material could be obtained, the passability in finish rolling became unstable due to rolling in a two-phase region.

尚、成品のりジンクは比較材も評点Aの良好なものが得
られた。
It should be noted that the comparison material of the finished glue zinc also had a good rating of A.

また、B添加によって5aj2. A (l値を低下さ
せてもA、QNの有害性を防止でき、実施例1よりも良
好な鉄損が得られている。
Moreover, by adding B, 5aj2. A (Even if the l value is lowered, the harmful effects of A and QN can be prevented, and a better iron loss than in Example 1 is obtained.

(発明の効果) 以上述べたようにこの発明によれば、熱延工程の粗圧延
開始から仕上圧延開始までの時間を、鋳片の等軸品比率
にみあって適切に制御することと、これに続く仕上圧延
温度を750℃から9(10℃の範囲に制御することに
よって、成品でのりジンクの発生のない、且つ磁束密度
の良好な無方向性電磁鋼板の製造を実現できる。
(Effects of the Invention) As described above, according to the present invention, the time from the start of rough rolling to the start of finish rolling in the hot rolling process can be appropriately controlled in accordance with the equiaxed product ratio of the slab; By controlling the subsequent finish rolling temperature within the range of 750° C. to 9° C. (10° C.), it is possible to produce a non-oriented electrical steel sheet that does not produce glue zinc and has a good magnetic flux density.

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

m1図は、鋳片C断面をパフ研磨し、その後マクロエッ
チしたものの鋳片内部組織を観察し、等軸晶と柱状晶の
厚み比率から等軸晶比率を算出する方法を示す模式図、
第2図は、鋳片等軸晶率が30%のものを出発材料とし
て、圧延開始までの時間を80秒(写真A)と105秒
(写真B)の2水準に振り、各々の仕上圧延前のバー厚
の状態でL断面のマクロエッチを行った顕微鏡写真、第
3図は、鋳片等軸晶率が30%のものを出発材料として
、粗圧延開始から仕上圧延開始までの時間を80秒から
115秒の間で水準を振った時の、最終成品でのりジン
ク評点付けしたものの散布図表、第4図は、製鋼で鋳片
等軸晶率を0%から70%までに水準を振り、熱延では
粗圧延開始から仕上圧延開始までの時間を50秒から1
35秒までの間で水準を振り各々の材料の最終成品での
りジンク評点付けしたものの散布図表、第5図は、仕上
圧延温度を700℃から960℃までの間で水準を振り
、得られた熱延板を熱延板焼鈍の有無に別けて最終成品
まで通板した時の磁束密度と仕上圧延温度との関係を示
した図表である。 第1図 第3図
Diagram m1 is a schematic diagram showing a method of observing the internal structure of a slab after puff-polishing the cross section of slab C and then macro-etching it, and calculating the equiaxed crystal ratio from the thickness ratio of equiaxed crystals and columnar crystals.
Figure 2 shows the finishing rolling of a slab with an equiaxed crystallinity of 30% as a starting material, varying the time to start rolling at two levels: 80 seconds (Photo A) and 105 seconds (Photo B). Figure 3 is a micrograph showing the macro-etching of the L cross section with the previous bar thickness, and shows the time from the start of rough rolling to the start of finish rolling using a cast slab with an equiaxed grain ratio of 30% as a starting material. Figure 4 is a scatter diagram of the glue zinc rating of the final product when the level was changed from 80 seconds to 115 seconds. In rolling and hot rolling, the time from the start of rough rolling to the start of finish rolling is 50 seconds to 1
Figure 5 is a scatter diagram of the adhesive and zinc ratings for the final product of each material, varying the level for up to 35 seconds. 2 is a chart showing the relationship between magnetic flux density and finish rolling temperature when hot-rolled sheets are passed through to final products with and without annealing. Figure 1 Figure 3

Claims (1)

【特許請求の範囲】 1、重量比で C:0.02%以下 Si:1.0〜3.0% Mn:0.1〜1.0% Al:1.0%以下 残部をFeとその他の不可避不純物よりなる溶鋼から得
られた連続鋳造鋳片を、1000〜1250℃の温度に
加熱した後、粗圧延、仕上圧延を行って熱延板とし、以
降常法に従って一回の冷延と最終焼鈍を行う無方向性電
磁鋼板の製造法において、上記粗圧延開始から仕上圧延
開始までの処理時間を、(1)式X秒以上とし、続く仕
上圧延を750℃〜900℃の高温領域で終えることを
特徴とする表面性状に優れ、且つ磁気特性の良好な無方
向性電磁鋼板を製造する方法。 X(秒)=〔130−鋳片等軸晶率(%)〕……(1)
式2、重量比で C:0.02%以下 Si:1.0〜3.0% Mn:0.1〜1.0% Al:1.0%以下 B:0.0003〜0.0050% 残部をFeとその他の不可避不純物よりなる溶鋼から得
られた連続鋳造鋳片を用いる請求項1記載の表面性状に
優れ、且つ磁気特性の良好な無方向性電磁鋼板を製造す
る方法。
[Claims] 1. C: 0.02% or less Si: 1.0 to 3.0% Mn: 0.1 to 1.0% Al: 1.0% or less The balance is Fe and others Continuously cast slabs obtained from molten steel containing unavoidable impurities are heated to a temperature of 1,000 to 1,250°C, then rough rolled and finish rolled to form hot rolled sheets, which are then cold rolled once according to conventional methods. In a method for manufacturing non-oriented electrical steel sheets that performs final annealing, the processing time from the start of rough rolling to the start of finish rolling is set to be at least X seconds according to formula (1), and the subsequent finish rolling is performed in a high temperature range of 750°C to 900°C. A method for producing a non-oriented electrical steel sheet having excellent surface properties and good magnetic properties. X (seconds) = [130 - Equiaxed crystallinity of slab (%)]...(1)
Formula 2, weight ratio: C: 0.02% or less Si: 1.0-3.0% Mn: 0.1-1.0% Al: 1.0% or less B: 0.0003-0.0050% 2. The method for producing a non-oriented electrical steel sheet with excellent surface texture and good magnetic properties according to claim 1, wherein a continuously cast slab obtained from molten steel with the balance being Fe and other unavoidable impurities is used.
JP64000393A 1989-01-06 1989-01-06 Method for producing non-oriented electrical steel sheet having excellent surface properties and good magnetic properties Expired - Lifetime JPH0733544B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP64000393A JPH0733544B2 (en) 1989-01-06 1989-01-06 Method for producing non-oriented electrical steel sheet having excellent surface properties and good magnetic properties

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP64000393A JPH0733544B2 (en) 1989-01-06 1989-01-06 Method for producing non-oriented electrical steel sheet having excellent surface properties and good magnetic properties

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Publication Number Publication Date
JPH02182829A true JPH02182829A (en) 1990-07-17
JPH0733544B2 JPH0733544B2 (en) 1995-04-12

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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
JP2007039754A (en) * 2005-08-04 2007-02-15 Sumitomo Metal Ind Ltd Method for producing Cu-containing non-oriented electrical steel sheet

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5174923A (en) * 1974-12-25 1976-06-29 Kawasaki Steel Co Atsumimuraganaku katsudenjitokuseino ryokona teikeisodenjikotaino seizohoho
JPS54163720A (en) * 1978-06-16 1979-12-26 Nippon Steel Corp Production of electric iron plate with excellent magnetic property
JPS5643091A (en) * 1979-09-14 1981-04-21 Tech Res & Dev Inst Of Japan Def Agency Underwater thermal clothing
JPS5752410A (en) * 1980-08-21 1982-03-27 Matsushita Electric Industrial Co Ltd Top plate molding method of cooking table
JPS5855210A (en) * 1981-09-28 1983-04-01 Nitto Electric Ind Co Ltd Kneading method of resin powder material and kneader used thereof

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5174923A (en) * 1974-12-25 1976-06-29 Kawasaki Steel Co Atsumimuraganaku katsudenjitokuseino ryokona teikeisodenjikotaino seizohoho
JPS54163720A (en) * 1978-06-16 1979-12-26 Nippon Steel Corp Production of electric iron plate with excellent magnetic property
JPS5643091A (en) * 1979-09-14 1981-04-21 Tech Res & Dev Inst Of Japan Def Agency Underwater thermal clothing
JPS5752410A (en) * 1980-08-21 1982-03-27 Matsushita Electric Industrial Co Ltd Top plate molding method of cooking table
JPS5855210A (en) * 1981-09-28 1983-04-01 Nitto Electric Ind Co Ltd Kneading method of resin powder material and kneader used thereof

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007039754A (en) * 2005-08-04 2007-02-15 Sumitomo Metal Ind Ltd Method for producing Cu-containing non-oriented electrical steel sheet

Also Published As

Publication number Publication date
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