JPS60103121A - Production of grain oriented silicon steel sheet having high magnetic flux density and low iron loss - Google Patents
Production of grain oriented silicon steel sheet having high magnetic flux density and low iron lossInfo
- Publication number
- JPS60103121A JPS60103121A JP20983583A JP20983583A JPS60103121A JP S60103121 A JPS60103121 A JP S60103121A JP 20983583 A JP20983583 A JP 20983583A JP 20983583 A JP20983583 A JP 20983583A JP S60103121 A JPS60103121 A JP S60103121A
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- Prior art keywords
- rolling
- annealing
- steel sheet
- diameter
- hot
- Prior art date
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Classifications
-
- C—CHEMISTRY; METALLURGY
- C21—METALLURGY OF IRON
- C21D—MODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
- C21D8/00—Modifying the physical properties by deformation combined with, or followed by, heat treatment
- C21D8/12—Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties
- C21D8/1216—Modifying the physical properties by deformation combined with, or followed by, heat treatment during manufacturing of articles with special electromagnetic properties the working step(s) being of interest
- C21D8/1222—Hot rolling
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- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Crystallography & Structural Chemistry (AREA)
- Thermal Sciences (AREA)
- Manufacturing & Machinery (AREA)
- Electromagnetism (AREA)
- Mechanical Engineering (AREA)
- Materials Engineering (AREA)
- Metallurgy (AREA)
- Organic Chemistry (AREA)
- Metal Rolling (AREA)
- Manufacturing Of Steel Electrode Plates (AREA)
Abstract
Description
【発明の詳細な説明】
(技術の概要)
本発明は、高磁束密度、低鉄損の方向性けい素鋼板の製
造方法Gこ関し、特に(110)面強度が最大値を示す
細粒の2次再結晶粒の発生する位置を板厚中心寄りに移
動させることにより、磁束密度が極めて高く鉄損の低い
方向性けい素鋼板を有利に製造する方法について提案す
る。Detailed Description of the Invention (Summary of the Technology) The present invention relates to a method for producing grain-oriented silicon steel sheets with high magnetic flux density and low core loss, and particularly relates to a method for producing grain-oriented silicon steel sheets with high magnetic flux density and low core loss. We propose a method for advantageously manufacturing grain-oriented silicon steel sheets with extremely high magnetic flux density and low iron loss by moving the position where secondary recrystallized grains are generated closer to the center of the sheet thickness.
(従来技術)
一方向性けい素鋼板は、主として変圧器その他の電気機
器の鉄芯として用いられているが、その性質としては磁
化特性が優れていること、すなわち磁束密度(B工。値
で代表される)が高くがっ鉄損が低いことが要求される
。(Prior art) Unidirectional silicon steel sheets are mainly used as iron cores for transformers and other electrical equipment, and their properties include excellent magnetization properties, that is, magnetic flux density (B). (typically) is required to have high iron loss and low iron loss.
一般に、一方向性けい素鋼板の磁気特性を向上させる第
1に有効な方法としては、鋼板中の2次再結晶粒の<
00−1 >軸を圧延方向に高度に揃えることであり、
第二には最終成品中に残存する不純物や析出物をできる
だけ減少させることが挙げられる。こうした既知の手法
の採用により最近では一方向性けい素鋼板の製造につい
て種々の改善がなされて、その磁気特性も年を追って改
善され今日ではBlo値が1.8.9T以上の高磁束密
度で、W17150値が1.05 W/に9の低鉄損が
得られるようになっている。In general, the first effective method for improving the magnetic properties of unidirectional silicon steel sheets is to
00-1 > The axis is highly aligned in the rolling direction,
The second is to reduce as much as possible the impurities and precipitates remaining in the final product. By adopting these known methods, various improvements have recently been made in the production of unidirectional silicon steel sheets, and their magnetic properties have improved over the years, and today they have a high magnetic flux density with a Blo value of 1.8.9T or more. , the W17150 value is 1.05 W/9, so that a low iron loss can be obtained.
このように一方向性けい素鋼板の性能は、数年前のエネ
ルギー危機を境にして電力損失の一層の低減が望まれる
ようになったことを契機として、とりわけ鉄芯材料の分
野では、さらに低鉄損の高級一方向性けい素鋼板への指
向が高まってきた。In this way, the performance of grain-oriented silicon steel sheets has improved, particularly in the field of iron core materials, as the energy crisis a few years ago led to the desire to further reduce power loss. There has been an increasing trend toward high-grade unidirectional silicon steel sheets with low iron loss.
(発明への動機)
ところで、本発明者等は、以前から一方向性けい素鋼板
の2次再結晶粒発達に関する基礎研究を進めて来たが、
より高い磁束密度でしかもより低い鉄損値を示す一方向
性けい素鋼板を得るには、従来からのX、li1回折に
よる調査、検討だけでは現象論的な考察しかできず不充
分であることが判った。そこで、本発明者らは、特開昭
55−83660号、あるいは実開昭55−88884
9号として提案したような走査電子像を用いた透過コツ
セル装置の開発を進め、この装置により一方向性けい素
鋼板の途中工程から採取した熱延板、中間焼鈍板、脱炭
・1次再結晶板さらには初期2次再結晶板等を詳細に調
査した結果状に列記するような新規な知見を得た。(Motivation for the Invention) By the way, the present inventors have been conducting basic research on the development of secondary recrystallized grains in unidirectional silicon steel sheets.
In order to obtain grain-oriented silicon steel sheets that exhibit higher magnetic flux density and lower core loss values, conventional investigations and studies using X, li1 diffraction alone are insufficient, as only phenomenological considerations can be made. It turns out. Therefore, the inventors of the present invention have proposed the method described in Japanese Unexamined Patent Publication No. 55-83660 or Utility Model Application No. 55-88884.
We are proceeding with the development of a transmission thin cell device using a scanning electron image, as proposed in No. As a result of detailed investigation of crystal plates, initial secondary recrystallization plates, etc., we have obtained new findings as listed below.
(1) (110) (o O1)方位の2次再結晶粒
の発生源となる結晶核が集積する位置は、熱延板表面か
ら約皆。深さに存在する(110)(001)方位伸長
粒(2次再結晶粒発生源)中の歪みの存在しない領域か
ら起こる。(1) (110) (o O1) The locations where crystal nuclei, which are the sources of secondary recrystallized grains, accumulate are approximately all from the surface of the hot-rolled sheet. This occurs from a strain-free region in (110) (001) oriented elongated grains (secondary recrystallized grain generation source) that exist at depth.
(2) (110) (o 01 )方位の2次再結晶
核発生は、熱延からのストラフチャ・メモリーにより、
1次冷延→中間焼鈍→2次冷延→脱炭・1次再結晶力Z
鈍エイJI!へと受け継がれ表面から30〜50μ深さ
において優先的に起こる。(2) Secondary recrystallization nucleation in the (110) (o 01 ) orientation occurs due to struture memory from hot rolling.
1st cold rolling → intermediate annealing → 2nd cold rolling → decarburization/1st recrystallization power Z
Dull stingray JI! and occurs preferentially at a depth of 30-50μ from the surface.
(3) 脱炭・1次再結晶焼鈍後の2次再結晶核は、数
個の< 11 (+ ) (o O1)方位の結晶粒が
合体(5ub(<rain coalescence
) L/てできた大きな結晶粒でマトリックス粒の2〜
6倍である。(3) Secondary recrystallization nuclei after decarburization and primary recrystallization annealing are composed of several <11 (+) (o O1) oriented crystal grains that coalesce (5ub (<rain coalescence
) L/ large crystal grains made of matrix grains 2~
It is 6 times more.
(4) 2次再結晶焼鈍初期において、(110)<0
01>方位の大きな結晶粒が優先成長する。(4) At the initial stage of secondary recrystallization annealing, (110)<0
Large crystal grains with 01> orientation grow preferentially.
以上のような知見に基づいて本発明者等は、良好な(1
10)(001)方位の2次再結晶核発スラブ加熱時に
は、本発明者らによって特願昭57−154887号と
して既に提案したように、スラブ上面と下面との加熱温
度を均一にすることとした。これによって、熱延中の表
面近傍に形成される(110 )(001)方位の2次
再結晶粒発生核の生成割合を上下両面で均等かつ高濃度
モ二集積でき、磁気特性の改善が達成された。Based on the above findings, the present inventors have determined that a good (1
10) When heating the slab for secondary recrystallization nucleation in the (001) orientation, as already proposed by the present inventors in Japanese Patent Application No. 57-154887, it is necessary to make the heating temperature uniform on the upper and lower surfaces of the slab. did. As a result, the generation rate of secondary recrystallized grain generation nuclei in the (110) (001) orientation that is formed near the surface during hot rolling can be uniformly and highly concentrated on both the upper and lower surfaces, and the magnetic properties are improved. It was done.
そこで、今回発明者らは、ざらに熱延条件その他につい
て詳細な研究を行った。Therefore, the inventors conducted a detailed study on the hot rolling conditions and other aspects.
その結果、一連の一方向性けい素鋼板の製造に当っては
、熱延鋼板の表面近傍に生成する(110)<001>
方位の2次再結晶粒発生源となる結晶核の集積部を、従
来よりも板厚中心寄りに生成させれば、細粒の2次再結
晶粒を発達させることができ、B が1.91 T以上
、W、775o: 0.99W/ic90
という優れた磁気特性を示すことを知見した。As a result, when manufacturing a series of unidirectional silicon steel sheets, (110) <001> is generated near the surface of the hot rolled steel sheet.
If the accumulation of crystal nuclei, which is the source of secondary recrystallized grains in orientation, is generated closer to the center of the plate thickness than in the past, fine secondary recrystallized grains can be developed, and B is 1. 91 T or higher, W, 775o: It was found that it exhibits excellent magnetic properties of 0.99 W/ic90.
しかも、上記の知見は熱間仕上圧延に際して、圧延ロー
ル径を上流側から下流側に向けて好ましくは順次小さく
する熱間圧延によって果せば高い信頼性のもとて所期の
効果が達せられることも判ったのである。Furthermore, the above knowledge can be achieved with high reliability by hot rolling in which the roll diameter is preferably gradually reduced from the upstream side to the downstream side during hot finish rolling. I also found out that.
(発明の目的)
本発明の目的は、(110)<001>方位の2次再結
晶粒の発生源となる結晶核集積部を板厚板を安定して得
ることにある。(Objective of the Invention) An object of the present invention is to stably obtain a thick plate with a crystal nucleus accumulation portion that becomes a source of secondary recrystallized grains with (110) <001> orientation.
(発明の構成)
上記の目的を達成する本発明熱延条件の好ましい例は以
下の如くである。素材の成分組成は、重ffi%で、S
i 8.35%、00.048%、seo、oxs%、
S’t) 0.025%、No 0.015%、残部不
可避不純物と1reよりなるもので、そのけい素鋼スラ
ブを1820°Cで均熱加熱後、粗圧延および連続熱間
圧延を行なって2.7 as厚の熱延板とした。(Structure of the Invention) Preferred examples of the hot rolling conditions of the present invention that achieve the above object are as follows. The composition of the material is heavy ffi%, S
i 8.35%, 00.048%, seo, oxs%,
S't) 0.025%, No. 0.015%, the remainder being unavoidable impurities and 1re. After soaking and heating the silicon steel slab at 1820°C, rough rolling and continuous hot rolling were performed. A hot rolled sheet with a thickness of 2.7 as was used.
なお、連続熱間仕上圧延は、第1図の(イ)。The continuous hot finish rolling is shown in (a) in Figure 1.
(ロ)および(ハ)の仕上圧延ロールを使って行なった
。すなわち、(イ)に示す圧延条件は、従来から採用さ
れている連続圧延条件で、A1スタンドからA6スタン
ドまでの圧延ロール径(第1図の斜線で示すワークロー
ル)がD□の同一であり、(ロ)に示す圧延条件は、&
1スタンドからA8スタンドまでの圧延ロール径は(イ
)と同じDoであるが、A4スタンドからA6スタンド
までの圧延ロール径D2 、Da * D4はDoのも
のより小さく、シかも下流側に向って順次小さなロール
径となるようにしてあり、また(ハ)に示す圧延条件は
、&1スタンドから煮6スタンドへと順次圧延ロール径
を小さくしたものである。The finishing rolls (b) and (c) were used. In other words, the rolling conditions shown in (a) are conventional continuous rolling conditions, and the diameter of the rolling rolls from the A1 stand to the A6 stand (the work rolls indicated by diagonal lines in Fig. 1) are the same as D□. , The rolling conditions shown in (b) are &
The rolling roll diameter from the 1st stand to the A8 stand is Do, which is the same as in (a), but the rolling roll diameters D2 and Da*D4 from the A4 stand to the A6 stand are smaller than those of Do, and the rolling roll diameters from the A4 stand to the A6 stand are smaller than those of Do, and the rolling roll diameters from the A4 stand to the A6 stand are smaller than Do. The diameter of the rolls is gradually decreased, and the rolling conditions shown in (c) are such that the diameter of the rolling rolls is gradually decreased from the &1 stand to the 6 stand.
これらの熱延板は、900℃で8分間の均一化焼鈍を施
したあと、圧下率約70%の1次冷延を行ない、950
℃で3分間の中間焼鈍を行なった後、圧下率約65%の
2次冷延を施して0.8闘厚の最終冷延板とした。その
後820℃で湿水素中で1次再結晶を兼ねる脱炭焼鈍を
施した後、MgOを主成分とする焼鈍分離剤を塗布し、
次いで850°Cで50時間の2次再結晶焼鈍を行い、
1180°Cで5時間H2ガス中で純化焼鈍を施した。These hot-rolled sheets were uniformly annealed at 900°C for 8 minutes and then subjected to primary cold rolling at a rolling reduction of approximately 70%.
After performing intermediate annealing at ℃ for 3 minutes, secondary cold rolling was performed at a rolling reduction of about 65% to obtain a final cold rolled sheet with a rolling thickness of 0.8. After that, decarburization annealing that also serves as primary recrystallization in wet hydrogen at 820°C is applied, and then an annealing separator containing MgO as the main component is applied.
Next, secondary recrystallization annealing was performed at 850°C for 50 hours.
Purification annealing was performed at 1180°C for 5 hours in H2 gas.
そのときの製品の磁気特性を第2図および第8図に、ま
た熱延板の板厚方向の(110)面強度変化(X線イン
バース強度)を第4図に示した。The magnetic properties of the product at that time are shown in FIGS. 2 and 8, and the change in (110) plane strength (X-ray inverse strength) in the thickness direction of the hot rolled sheet is shown in FIG.
鎗 ^ Rオ J慢 ′I+ シー aシ n 舊オ
Δζ 融「 口 n\ Y内 −イ ルヒ J/I−7
7% u−よh よ、ら明らかなように、等径ロール圧
延(A)の従来法での連続仕上圧延条件では、Bo。が
1.90 T 。Spear ^ R o J arrogance 'I+ C a shi n 舊オ
Δζ Yuru' mouth n\ Y inside - Iruhi J/I-7
As is clear, under the continuous finish rolling conditions of the conventional method of equal diameter roll rolling (A), Bo. is 1.90 T.
W17/60が1.04 W/に9程度であるのに対し
、本発明に従う上流側等径下流側異径ロールの本発明例
(B)および順次小径ロールとするものの本発明例(0
)では、Bo。が1.916〜1.918 T 、、W
17150が0.98〜0.97 W/に9と磁束密度
、鉄損共に極端に向上しているのが注目される。また本
発明の熱延条件の例を示す(B)と((3)の条件比較
では、次第に小径化させていくものの例(0)の条件の
が若干特性が良い。W17/60 is about 9 to 1.04 W/, whereas the present invention example (B) of the upstream side equal diameter downstream side different diameter roll according to the present invention and the present invention example (0
) So, Bo. is 1.916 to 1.918 T,,W
It is noteworthy that 17150 has an extremely improved magnetic flux density and iron loss of 0.98 to 0.97 W/9. Further, in a comparison of conditions (B) and (3), which are examples of the hot rolling conditions of the present invention, the conditions of example (0), which gradually reduce the diameter, have slightly better characteristics.
第4図に示ず熱延板板厚方向の(110)面強度変化の
グラフから明らかなように、等径ロールを用いる従来法
(A)では、熱延板表面から板厚方向へ向って約号。程
度の深さの位置において、(110)面強度が最大とな
り、それより深い位置では急激に弱くなる。これに対し
て、圧延方向で小径化している本発明例(B)および(
0)の場合は、(110)面強度の最大値を示す領域(
幅)は従来例(A)よりも拡大され、しかも(110)
(001)方位の2次再結晶核発生源の位置、すなわち
(110)面強度の最大値を示す位置が板厚の中心方向
に移動していることが注目される。本発明法の(B)l
C)Gこあっては、最大の(110)面強度の位置が、
熱延板表面力ら板厚中心方向へ約曇〜嵐程度の深さであ
り、この位置のとき、第2,3図に示すように優れた磁
気特性を示しているのである。As is clear from the graph of the (110) plane strength change in the thickness direction of the hot-rolled sheet (not shown in Figure 4), in the conventional method (A) using rolls of equal diameter, from the surface of the hot-rolled sheet in the thickness direction About issue. The strength of the (110) plane reaches its maximum at a depth of about 100 mL, and rapidly weakens at deeper positions. On the other hand, inventive examples (B) and (
0), the area showing the maximum value of the (110) surface strength (
Width) is larger than the conventional example (A), and (110)
It is noteworthy that the position of the secondary recrystallization nucleus generation source in the (001) orientation, that is, the position showing the maximum value of the (110) plane strength, has moved toward the center of the plate thickness. (B)l of the method of the present invention
C) In G, the position of maximum (110) plane strength is
The depth of the hot-rolled sheet toward the center of its thickness is approximately cloudy to stormy, and at this position, it exhibits excellent magnetic properties as shown in FIGS. 2 and 3.
このように、(110)(001)方位の2次再結晶核
発生源の位置を、板厚中心方向へ移動させることによる
特性向上の理由は、完全に解明されたわけではないが、
第2図および第8図に示す両者の比較から明らかなよう
に(110)(001)方位の2次再結晶核の発生頻度
が多くなるとともに、その位置が板厚方向へ移動するこ
とが影響しているのは事実であり、これは熱延時の変形
挙動の相違に起因して起り、そのために圧延ロール径を
下流側に向けて順次小さくすれば、押し込み効果となっ
て上述のような現象を生むのである。Although the reason for the improvement in properties by moving the position of the secondary recrystallization nucleus generation source in the (110)(001) direction toward the center of the plate thickness has not been completely elucidated,
As is clear from the comparison shown in Figures 2 and 8, the frequency of occurrence of secondary recrystallized nuclei in the (110) (001) orientation increases and the position of the secondary recrystallization nuclei moves in the thickness direction. It is true that this phenomenon occurs due to differences in deformation behavior during hot rolling. Therefore, if the diameter of the rolling rolls is gradually decreased toward the downstream side, the indentation effect will occur and the phenomenon described above will occur. It gives birth to
以上説明したように、細粒の(110) (OO1,)
・・方位に強く集積した2次再結晶粒を発達させるため
の熱延条件としては、既に知られているような熱延板表
面近傍の(110)(001)方位の結晶粒を敢多く存
在させることの他に、上述したように該(lto )(
Ool)方位の結晶粒の発生位置が表面近傍より板厚中
心方向に移動した状況で存在すること、またこのような
状況を作り出すことによって本来冷延安定方位である(
100)< o ]、 1 >方位の結晶粒をできる限
り少なくすることが可能となるのである。こうした条件
が満足される結果、本発明にあっては磁束密度が高く鉄
損の低い一方向性けい素鋼板の製待が可能となったと考
えられる。As explained above, fine grain (110) (OO1,)
...The hot rolling conditions for developing secondary recrystallized grains that are strongly concentrated in the orientation are as follows: the presence of many (110)(001) oriented crystal grains near the surface of the hot rolled sheet, as is already known. In addition to making the (lto)(
The generation position of crystal grains with the Ool) orientation is shifted from near the surface toward the center of the plate thickness, and by creating such a situation, the orientation of the crystal grains is originally a stable cold rolling orientation.
100) <o], 1> orientation crystal grains can be reduced as much as possible. It is believed that as a result of satisfying these conditions, the present invention is able to manufacture unidirectional silicon steel sheets with high magnetic flux density and low iron loss.
これに対し、これまでも熱延中の集合組織を変える幾つ
かの試みが提案されており、代表的なものとしては特公
昭58−5970号として提案されたものは、上下に非
対称フローを発生させるという異周速圧延の方法がある
。しかしながら、この既知の異周速圧延法は板厚方向に
上下面Qこ非対称な塑性フローを導くことにより集合組
織を変化させることには有効であっても、本発明のよう
な(110)(001)方位の結晶粒の発生位置をより
板厚中心部に近づけることは不可能である。In response to this, several attempts have been proposed to change the texture during hot rolling, and the representative one proposed in Japanese Patent Publication No. 58-5970 generates an asymmetric flow in the vertical direction. There is a method of rolling at different circumferential speeds. However, although this known variable circumferential speed rolling method is effective in changing the texture by introducing an asymmetrical plastic flow on the upper and lower surfaces in the thickness direction, it is difficult to change the texture (110) as in the present invention. It is impossible to bring the generation position of crystal grains with the 001) orientation closer to the center of the plate thickness.
以上本発明を従来技術と対比して説明したところから明
らかなように、好適実施態様としC示した連続仕上圧延
機の圧延ロール径を次第に小さくして(110)<00
1>方位の2次再結晶核の発生源を板厚中心に移行させ
る連続熱間圧延法は、先行する諸公知技術と発想の基本
を異にするものであって、それによって発揮される効果
もはるかにすぐれたものである。As is clear from the above explanation of the present invention in comparison with the prior art, the rolling roll diameter of the continuous finishing mill shown in C as a preferred embodiment is gradually reduced to (110)<00.
The continuous hot rolling method in which the source of secondary recrystallization nuclei in the 1> orientation is shifted to the center of the plate thickness is fundamentally different from previous known techniques, and the effects achieved by it are is also far superior.
次に本発明における製造工程についてその具体的内容を
圧延ロール径を上流側と下流側とで変える好a例にもと
づいて以下に述べる。Next, the specific details of the manufacturing process in the present invention will be described below based on a preferred example in which the rolling roll diameter is changed between the upstream side and the downstream side.
本発明法で用いる出発素材は、公知の製鋼方法ζ例えば
転炉見気炉などによって製鋼し、さらに造塊又は連続鋳
造などによってスラブとしたものを用いるが、近年では
工業的利点の多い連続鋳造法による方法が好適に用いら
れる。The starting material used in the method of the present invention is a steel made by a known steelmaking method such as a converter furnace and then made into a slab by ingot making or continuous casting. A method according to the method is preferably used.
該出発表材の虎分鉗蔭、は、従来の公知の一フf1m性
けい素鋼板と同じく、例えば■Si 2.0−4.0%
、MO0,005P−0,05%、sb o、o O5
〜0.25%、Sあるいは880.005〜0.05%
を含有する組成、■si 2.0〜4.0%、I O,
01〜0.05%、S O,005〜0.05%、N
O,001〜0.01%を含有する組成、又は■Si
2.0〜4゜0%、S O,005〜0.05%、B
O,0008〜0.0040%、N O,001〜o、
o 1%を含有する組成の如き諷ものが好適Gこ採用さ
れる。The released material, like the conventional well-known silicon steel sheet, has Si 2.0-4.0%, for example.
, MO0,005P-0,05%, sb o, o O5
~0.25%, S or 880.005~0.05%
A composition containing ■si 2.0 to 4.0%, IO,
01-0.05%, SO, 005-0.05%, N
Composition containing O,001 to 0.01%, or ■Si
2.0~4゜0%, SO, 005~0.05%, B
O,0008~0.0040%, NO,001~o,
Compositions such as those containing 1% o are preferably employed.
次に、連続鋳造もしくは造塊−分塊法によって得られた
けい素鋼スラブは、素材中に含有されているMnSある
いはMnSe等を解離固溶させるために、1250°C
〜14oo′Cの高温加熱を施す必要がある。この高温
加熱は、次の熱間圧延工程中に形成させる表面近傍の(
110)(001)方位の強い結晶粒を得るために均熱
加熱を行う必要がある。Next, the silicon steel slab obtained by continuous casting or ingot-blooming method is heated to 1250°C in order to dissociate and dissolve MnS or MnSe contained in the material
It is necessary to perform high temperature heating of ~14oo'C. This high-temperature heating is applied to the (
In order to obtain crystal grains with a strong 110) (001) orientation, it is necessary to perform soaking heating.
加熱後のスラブは、粗圧延及び熱間仕上圧延により、2
〜3關厚程度の熱延板とされる。本発明では、熱間仕上
圧延時の仕上圧延ロール径を圧延方向に向って次第に小
さくするという条件で行つ製品特性(鉄損)との関係を
示す。この図から判るように、この上流・下流側ロール
径\の比が1.1〜5倍、望ましくは1.2〜4.5倍
η羞となるようなロール径比において最も良好な特性が
得られることがわかる。このような連続仕上圧延機の圧
延ロール径の組合わせは、第1図−(ハ)の条件のよう
に、圧延方向に順次小さくする方が製品の磁気特性向上
に有利であるが、第1図−(ロ)の条件のようにA1か
らA8までの前半ロール径あるいは應1からA2までの
ロール径を同程度とし、その後のA4から屋6あるいは
A8から黒6までの後半リール径を順次小さくしても製
品の磁気特性の向上を図ることが可能である。また課簾
玉らへ関ズ次を招$大・小ロール間のロール径の差には
特に制限を加えないが、急激な変化は操業上のトルプル
を招きやすくなるためさける方が良い。さらに連続仕上
圧延機の下流側(後半)のロール径を小さくすることに
よる荷重付加の増加、クラウンあるいは形状の制御法等
の問題解決には異なった圧延ミルの併用(4Hi −ミ
ルと5.Hi −ミル併用あるいは4Hi−ミル(!:
6Hi−ミルとブラネクリミル併用)等従来公知のい
ずれの技術を用いても良く、これらの併用に制限を加え
ない。After heating, the slab is subjected to rough rolling and hot finish rolling.
It is said to be a hot-rolled sheet with a thickness of ~3 mm. In the present invention, the relationship with product characteristics (iron loss) is shown under the condition that the finishing roll diameter during hot finishing rolling is gradually decreased in the rolling direction. As can be seen from this figure, the best characteristics are obtained when the ratio of the upstream and downstream roll diameters is 1.1 to 5 times, preferably 1.2 to 4.5 times. You can see what you can get. Regarding the combination of rolling roll diameters of such a continuous finishing mill, it is advantageous to gradually reduce the diameters of the product in the rolling direction as shown in the condition shown in Fig. 1-(c). As shown in Figure-(B), the diameter of the first half roll from A1 to A8 or the diameter of the roll from A1 to A2 should be the same, and then the diameter of the second half reel from A4 to A6 or from A8 to BLACK 6 should be the same. Even if it is made smaller, it is possible to improve the magnetic properties of the product. In addition, there is no particular restriction on the difference in roll diameter between the large and small rolls, but it is better to avoid sudden changes as they tend to cause operational problems. Furthermore, in order to solve problems such as the increase in load applied by reducing the roll diameter on the downstream side (second half) of the continuous finishing mill, and how to control the crown or shape, different rolling mills are used (4Hi-mill and 5.Hi-mill). -Mill combination or 4Hi-mil (!:
Any conventionally known technique such as the combination of 6Hi-mil and branecrimil may be used, and there are no restrictions on the combination of these techniques.
このような方法で熱延された熱延板は、8oO℃〜1】
00°Cでの均一化焼鈍を経て1回の冷間圧延で最終板
厚とする1回冷延法か、又は通常850℃から1050
°Cの中間焼鈍をはさんでさらに冷延する2回法にて最
初の圧下率は50%から80%程度、最終の川下率は5
0%から85%程度で0.2鴎からQ、3115g厚の
最終板厚程度とする2回冷延法で行うことができる。通
常仕上がり板1’Xは0.8略厚とされることが多い。The hot-rolled sheet hot-rolled by this method has a temperature of 8oO℃~1】
One-time cold rolling method in which the final plate thickness is obtained by one cold rolling after uniform annealing at 00°C, or usually from 850°C to 1050°C.
In the two-step method of intermediate annealing at °C and further cold rolling, the initial rolling reduction is about 50% to 80%, and the final downstream ratio is 5.
It can be carried out by a two-time cold rolling method in which the final sheet thickness is approximately 0.2 to 85% and 3115 g thick. Normally, the finished board 1'X is often approximately 0.8 mm thick.
最終冷延を終り、製品板厚に仕上げた鎖板は、表面脱脂
後、780°C〜850°Cの温度範囲で湿水素中で1
次再結晶焼鈍を兼ねる脱炭焼鈍を3分〜15分程度施す
。After finishing the final cold rolling and finishing the chain plate to the product thickness, the surface is degreased and then heated in wet hydrogen at a temperature range of 780°C to 850°C.
Decarburization annealing, which also serves as next recrystallization annealing, is performed for about 3 to 15 minutes.
最終焼鈍は、(110)(001)方位の2次再結晶粒
を充分発達させるため施されるもので、通常箱焼鈍によ
って直ちに1000″C以上に昇温しその温度に保持す
ることによって行なう。この最終焼鈍は、通常MgOを
主成分とする焼鈍分離剤を塗布し、箱焼鈍によって施さ
れるが、本発明において(110)(001)方位に高
度に揃った2次再結晶組織を発達させるためには、82
0″Cから900°Cの低温で保定焼鈍する方が有利で
あり、そのほか例えば0.5〜15°O/hの昇温速度
での除熱焼鈍でも良い。The final annealing is performed to sufficiently develop secondary recrystallized grains with the (110)(001) orientation, and is usually carried out by immediately raising the temperature to 1000''C or higher by box annealing and maintaining it at that temperature. This final annealing is usually performed by applying an annealing separator mainly composed of MgO and box annealing, but in the present invention, a secondary recrystallized structure highly aligned in the (110) (001) orientation is developed. In order, 82
It is more advantageous to carry out holding annealing at a low temperature of 0''C to 900°C, and alternatively, heat removal annealing at a temperature increase rate of 0.5 to 15°O/h may also be used.
(実 施 例)
実施例1
成分組成が重ffi%で、OO,048%、 Si 8
.85% 、 Se 0.018%、 MO0,015
%、Sb0.0251%を含有するけい素鋼スラブを1
350″Cで加熱後粗圧延−仕上圧延と経る連続熱間圧
延により2.7鰭厚の熱延板とした。なお連続熱間仕上
圧延の条件は、第1図の(ハ)に示すロール配列の条件
と同じ方法、すなわちA1のロール径り工:800闘φ
)から//l1tO(D、、:472闘φ)まで順次圧
延ロール径を小さくする(前のロール当り10%半径を
小さくする)方法で熱延した。これらの熱延板は、90
0°Cで3分間の均一化焼鈍を施した後、圧下率約70
%の1法令間圧延を行ない、950°Cで3分間の中間
焼鈍を行なった後、圧下率約、65%の2法令間圧延を
施して0.8關厚の最終冷延板とした。その後、820
℃で湿水素中で脱炭焼鈍を施した後、MgOを主成分と
する焼鈍分離剤を塗布し、850°Cで50時間の2次
再結晶焼鈍し、1180°Cで6時間H2ガス中で純化
焼鈍を施した。そのときの製品の磁気特性は次のようで
あった。(Example) Example 1 The component composition is heavy ffi%, OO, 048%, Si 8
.. 85%, Se 0.018%, MO0,015
%, silicon steel slab containing 0.0251% Sb.
After heating at 350"C, a hot rolled plate with a fin thickness of 2.7 was obtained by continuous hot rolling through rough rolling and finishing rolling.The conditions for the continuous hot rolling were as shown in (c) in Figure 1. The same method as the arrangement conditions, namely A1 roll diameter: 800 mm
) to //l1tO (D, ,: 472 mm φ) by successively decreasing the rolling roll diameter (reducing the radius by 10% for each previous roll). These hot rolled sheets are 90
After uniform annealing at 0°C for 3 minutes, the reduction rate was approximately 70.
%, and intermediate annealing at 950°C for 3 minutes, followed by double-law rolling at a reduction rate of approximately 65% to obtain a final cold-rolled sheet with a thickness of 0.8 mm. After that, 820
After decarburization annealing in wet hydrogen at ℃, an annealing separator mainly composed of MgO was applied, secondary recrystallization annealing was performed at 850℃ for 50 hours, and then at 1180℃ for 6 hours in H2 gas. Purification annealing was performed. The magnetic properties of the product at that time were as follows.
B :1.91T、 W1?15o:0.99W/kg
0
実施例2
成分組成が重態%で、OO,046%、 Si 3.1
3%、 At ff、025%、 In 0.072%
、NO,0068%を含有する連射けい素鋼スラブを1
400°Cで加熱後、粗圧延−仕上圧延と経る連続熱間
圧延により2.0酩厚の熱延板とした。この連続熱間仕
上、圧延条件は、第1図の(ハ)に示すロール配列の条
件と同等の方法すなわち711L1(AIのロール径は
D :850朋φ)からA6 (Da ’ 279聞φ
)まで順次圧延ロール径を小さくする(前のロール当り
20%半径を小さくする)方法で熱延した。B: 1.91T, W1?15o: 0.99W/kg
0 Example 2 Component composition is heavy weight %, OO, 046%, Si 3.1
3%, At ff, 025%, In 0.072%
, NO,0068%
After heating at 400°C, a hot rolled sheet having a thickness of 2.0 mm was obtained by continuous hot rolling through rough rolling and finish rolling. This continuous hot finishing and rolling conditions are the same as the roll arrangement conditions shown in (c) of Figure 1, that is, from 711L1 (roll diameter of AI is D: 850mm) to A6 (Da' 279mm).
), the diameter of the rolling rolls was successively reduced (reducing the radius by 20% for each previous roll).
これらの熱延板は、1050°Cで8分間の均一化焼鈍
を施した後急冷処理した。その後250°Cの温間圧延
を含む強冷延を施してo、a m厚の最終冷延板とした
。その後850°Cの湿水素中で脱炭焼鈍を施した後、
MgOを主成分とする焼鈍分離剤を塗布した後、850
°Cから1050℃まで5°C/hで昇温して2次再結
晶させた後、1200°C1で8時間水素中で純化焼鈍
を施した。そのときの製品の磁気特性は次のようであっ
た。These hot-rolled sheets were uniformly annealed at 1050°C for 8 minutes and then rapidly cooled. Thereafter, strong cold rolling including warm rolling at 250° C. was performed to obtain a final cold rolled sheet having a thickness of 0.0 m or 0.0 m. After that, decarburization annealing was performed in wet hydrogen at 850°C,
After applying an annealing separator mainly composed of MgO, 850
After secondary recrystallization by raising the temperature from °C to 1050 °C at a rate of 5 °C/h, purification annealing was performed in hydrogen at 1200 °C for 8 hours. The magnetic properties of the product at that time were as follows.
BIO:1.94 T I Wl?150 :O−97
W/kg実施例8
成分組成が重量%で、OO,042%、 si、 a、
a 。BIO:1.94 T I Wl? 150:O-97
W/kg Example 8 Component composition is in weight%, OO, 042%, si, a,
a.
% 、 Se O,020%、 MO0,018% 、
Sb O,080%を含有するけい素鋼スラブを13
60°Cで加熱後、粗圧延−仕上圧延と経る連続熱間圧
延により2.7+nJシの熱延板とした。なお、連続熱
間仕上圧延の条件は、第1図の(ロ)に示すロール配列
の条件と類似の方法、すなわちA 1.2のロール径は
800 smφ、j63,4のロール径は500闘φ、
應5,6のロール径は400聾φのロール径で熱延した
。これらの熱延板は、950℃で3分間の、均一化焼鈍
を施した後、圧下率約70%の1次冷間圧延を行ない、
950°Cで8分間の中間焼鈍を行なった後圧下率約6
5%の2法令間圧延?施して0.8 fl厚の最終冷延
板とした。その後820°Cで湿水素中で脱炭焼鈍を施
した後、MgOを主成分とする焼鈍分離剤を塗布し、8
50°Cで50時間の2次再結晶焼鈍を行ない、118
0°Cで5時間水素中で純化焼鈍を施した。そのときの
磁気特性は次のようであった。%, SeO,020%, MO0,018%,
13 silicon steel slabs containing 80% SbO
After heating at 60°C, a hot rolled sheet of 2.7+nJ was obtained by continuous hot rolling through rough rolling and finishing rolling. The conditions for continuous hot finish rolling are similar to the roll arrangement conditions shown in Figure 1 (B), namely, the roll diameter for A1.2 is 800 smφ, and the roll diameter for J63.4 is 500 mmφ. φ,
The roll diameters of Nos. 5 and 6 were hot rolled with a roll diameter of 400 mm. These hot-rolled sheets were uniformly annealed at 950°C for 3 minutes, and then subjected to primary cold rolling at a rolling reduction of about 70%.
After intermediate annealing at 950°C for 8 minutes, the reduction rate is approximately 6.
5% two-law rolling? A final cold-rolled sheet with a thickness of 0.8 fl was obtained. After that, decarburization annealing was performed in wet hydrogen at 820°C, and an annealing separator mainly composed of MgO was applied.
Secondary recrystallization annealing was performed at 50°C for 50 hours, and 118
Purification annealing was performed in hydrogen at 0°C for 5 hours. The magnetic properties at that time were as follows.
B、。: 1,92T 、 ”x715o : 0−9
7W/に9(発明の効果)
以上説明したように、本発明は、(110)<OO1>
方位の2次再結晶粒の発生源となる結晶核の集積・位置
を板厚中心部へ移行させる連続熱間仕上圧延により、細
粒の2次再結晶を発達させて、81.90’I’以上、
Wエフ150 ”0以下の磁束密度が極めて高く、鉄損
の低い一方向性けい素劇板を有利に製造することかでき
る。B. : 1,92T,"x715o: 0-9
7W/9 (Effect of the invention) As explained above, the present invention provides (110)<OO1>
Continuous hot finish rolling moves the accumulation and position of crystal nuclei, which are the source of oriented secondary recrystallized grains, to the center of the plate thickness, developing secondary recrystallization of fine grains, resulting in 81.90'I 'that's all,
W F150'' It is possible to advantageously produce a unidirectional silicon dynamic plate with extremely high magnetic flux density of 0 or less and low iron loss.
第1図は、従来法(イ)、本発明法(ロ)、(ハ)に従
う連続熱間仕上圧延機のロール配列を示す路線図、第2
図は、従来法と本発明法との磁束密度の比較を示すグラ
フ、
第3図は、従来法と本発明法との鉄損の比較を示すグラ
フへ
第4図は、従来法と本発明法との(11,0)面強度変
化を示すグラフ、
第5図は、仕上圧延ロール径比を変化させたとl・きの
鉄損特性の変化を示すグラフである。
第2図
第3図
第4図
○慌来沫(A)
・木ダ明試(B)
■オ、定明は(の
1
芭ε1゜
、11゜
V″如FIG. 1 is a route map showing the roll arrangement of a continuous hot finishing mill according to the conventional method (a), the method of the present invention (b), and (c);
The figure is a graph showing a comparison of magnetic flux density between the conventional method and the present invention method. Figure 3 is a graph showing a comparison of iron loss between the conventional method and the present invention method. Figure 4 is a graph showing the comparison between the conventional method and the present invention method. Figure 5 is a graph showing changes in iron loss characteristics when the finishing roll diameter ratio is changed. Figure 2 Figure 3 Figure 4 ○ Rushing water (A) ・Kida Ming test (B)
Claims (1)
間圧延をし、1回もしくは2回の冷間圧延によって最終
板厚とし、次いで脱炭・1次再結晶焼鈍後焼鈍分離剤を
塗布して最終焼鈍を施す一連の方向性けい素鋼板の製造
方法において、 上記熱間仕上圧延段階で、熱延鋼板表面近傍に優先生成
する(110)<001>方位の2次再結晶粒発生源と
なる結晶核の集積部を、板厚中心寄りに生成させること
を特徴とする高磁束密度、低鉄損の方向性けい素鋼板の
製造方法。 区 上記結晶核集積部の位置は、(110)面強度の最
大値を示す位置が鋼板表面から板厚中心方向へξ〜外の
所であることを特徴とする特許請求の範囲1記載の方法
− & 含けい素鋼スラブを粗圧延、連続仕上圧延と経て熱
間圧延をし、1回もしくは2回の冷間圧延によつ゛C最
終板厚とし、次いで脱炭・1次再結晶焼鈍後焼鈍分離剤
を塗布して最終焼鈍を施す一連の方向性けい素鋼板の製
造方法において、 上記熱間仕上圧延に当り、連続仕上圧延機の圧延ロール
径を上流側に位置するものを大きく下流側に位置するも
のについては小さい径のもので圧延することにより、熱
延鋼板表面近傍に優先生成する( 110 )<OO1
>方位の2次再結晶粒発生源となる結晶核の集積部を、
板厚中心寄りに生成させることを特徴とする高磁束密度
、低鉄損の方向性けい素鋼板の製造方法。 表 上記圧延ロールが、上流側から下流側に向って順次
に小径化するように配置されることを特徴とする特許請
求の範囲3記載の方法。 乙 上記圧延ロールが、上流側に位置する複数のものが
同径で、引続く下流側に位置する複数が順次に小径化す
るように配置されることを特徴とする特許請求の範囲3
記載の方法。 α 上流側、下流側に位置する各仕」ユ圧延ロール径の
比が、1.1〜5倍の範囲内である特δ′「d〜求の範
囲4または5記載の方法。 1、 順次小径化するロール配列として、2個以上の組
ごとに順次小径にすることを特徴とする特許請求の範囲
4記載の方法。[Claims] L A silicon-containing steel slab is rough rolled, continuously finished rolled, then hot rolled, cold rolled once or twice to achieve the final thickness, and then decarburized and primary recrystallized. In a series of methods for producing grain-oriented silicon steel sheets in which an annealing separator is applied after annealing and final annealing is performed, the (110)<001> orientation is preferentially generated near the surface of the hot-rolled steel sheet in the hot finish rolling step. A method for producing a grain-oriented silicon steel sheet with high magnetic flux density and low core loss, characterized in that an accumulation part of crystal nuclei, which is a source of secondary recrystallized grains, is generated near the center of the sheet thickness. The method according to claim 1, wherein the position of the crystal nucleus accumulation portion is such that the position exhibiting the maximum value of the (110) plane strength is at a distance of ξ from the steel plate surface toward the center of the plate thickness. - & A silicon-containing steel slab is rough rolled, continuous finish rolled, hot rolled, cold rolled once or twice to obtain a final thickness of ゛C, and then decarburized and primary recrystallized annealed. In a series of methods for producing grain-oriented silicon steel sheets in which an annealing separator is applied and final annealing is performed, the diameter of the rolling roll of the continuous finishing mill is changed to the diameter of the rolling roll located on the upstream side during the hot finishing rolling described above. (110)<OO1
> The accumulation area of crystal nuclei that becomes the source of secondary recrystallized grains in the orientation is
A method for producing a grain-oriented silicon steel sheet with high magnetic flux density and low core loss, characterized in that the magnetic flux is generated near the center of the sheet thickness. 4. The method according to claim 3, wherein the rolling rolls are arranged so that their diameters decrease sequentially from the upstream side to the downstream side. B. Claim 3, characterized in that the above-mentioned rolling rolls are arranged so that a plurality of rolls located on the upstream side have the same diameter, and a plurality of rolling rolls located on the downstream side successively have a smaller diameter.
Method described. The method according to 4 or 5, wherein the ratio of the diameters of the rolling rolls located on the upstream side and the downstream side is within the range of 1.1 to 5 times. 5. The method according to claim 4, wherein the diameter is successively reduced in sets of two or more rolls in the arrangement of the rolls.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20983583A JPS60103121A (en) | 1983-11-10 | 1983-11-10 | Production of grain oriented silicon steel sheet having high magnetic flux density and low iron loss |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20983583A JPS60103121A (en) | 1983-11-10 | 1983-11-10 | Production of grain oriented silicon steel sheet having high magnetic flux density and low iron loss |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60103121A true JPS60103121A (en) | 1985-06-07 |
| JPH0332603B2 JPH0332603B2 (en) | 1991-05-14 |
Family
ID=16579404
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP20983583A Granted JPS60103121A (en) | 1983-11-10 | 1983-11-10 | Production of grain oriented silicon steel sheet having high magnetic flux density and low iron loss |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60103121A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US12110569B2 (en) | 2019-03-20 | 2024-10-08 | Nippon Steel Corporation | Non oriented electrical steel sheet and method for producing thereof |
-
1983
- 1983-11-10 JP JP20983583A patent/JPS60103121A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US12110569B2 (en) | 2019-03-20 | 2024-10-08 | Nippon Steel Corporation | Non oriented electrical steel sheet and method for producing thereof |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0332603B2 (en) | 1991-05-14 |
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