JPH0826398B2 - Method for producing unidirectional electrical steel sheet with extremely high magnetic flux density - Google Patents
Method for producing unidirectional electrical steel sheet with extremely high magnetic flux densityInfo
- Publication number
- JPH0826398B2 JPH0826398B2 JP62083852A JP8385287A JPH0826398B2 JP H0826398 B2 JPH0826398 B2 JP H0826398B2 JP 62083852 A JP62083852 A JP 62083852A JP 8385287 A JP8385287 A JP 8385287A JP H0826398 B2 JPH0826398 B2 JP H0826398B2
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- steel sheet
- annealing
- magnetic flux
- flux density
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Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明はトランス等の鉄芯に用いられる高磁束密度一
方向性電磁鋼板の製造方法に関するものである。The present invention relates to a method for producing a high magnetic flux density unidirectional electrical steel sheet used for an iron core of a transformer or the like.
一方向性電磁鋼板は軟磁性材料として主にトランスそ
の他の電気機器の鉄芯材料に使用されているもので、磁
気特性として励磁特性と鉄損特性が良好でなくてはなら
ない。The unidirectional electrical steel sheet is mainly used as a soft magnetic material for iron core materials of transformers and other electric devices, and it must have good magnetic excitation characteristics and iron loss characteristics.
この励磁特性を表わす数値として通常B8(磁場の強さ
800A/mにおける磁束密度)を用い、鉄損特性を表わす数
値としてW17/50(50Hzで1.7Tまで磁化させた時の1kg当
りの鉄損)を用いている。Normally, B 8 (magnetic field strength
Magnetic flux density at 800A / m) is used, and W17 / 50 (iron loss per 1kg when magnetized to 1.7T at 50Hz) is used as a numerical value to represent iron loss characteristics.
この一方向性電磁鋼板は最終仕上焼鈍工程で2次再結
晶現象を起こさせ、鋼板面に{110}面、圧延方向に<0
01>軸をもったいわゆるゴス組織を発達させることによ
って得られている。良好な磁気特性を得るためには磁化
容易軸である<001>軸を圧延方向に高度に揃える事が
重要である。又板厚、結晶粒度、固有抵抗、表面被膜、
鋼板の純度等も磁気特性に大きな影響を及ぼす。This unidirectional electrical steel sheet causes a secondary recrystallization phenomenon in the final finishing annealing step, causing the steel sheet surface to have a {110} plane and the rolling direction to have a <0.
It is obtained by developing a so-called Goth tissue with 01> axis. In order to obtain good magnetic properties, it is important to highly align the <001> axis, which is the easy axis of magnetization, in the rolling direction. In addition, plate thickness, grain size, specific resistance, surface coating,
The purity of the steel sheet also has a great influence on the magnetic properties.
方向性については、MnS,AlNをインヒビターとして利
用する最終強圧下冷間圧延を特徴とする方法によって大
幅に向上し、それに伴って鉄損特性も著しく向上してき
た。The directionality has been significantly improved by the method characterized by final high-pressure cold rolling using MnS and AlN as inhibitors, and the iron loss characteristics have also been significantly improved.
一方近年エネルギー価格の高騰を背景として、トラン
スメーカーは低鉄損トランス用素材への指向を一段と強
めている。低鉄損素材としてアモルファス合金や6.5%S
i鋼等の開発も進められているが、トランス用材料とし
て工業的に使用するには解決すべき問題を残している。
他方レーザー等を用いた磁区制御技術が近年開発され、
それによって鉄損特性が大幅に向上した。また製品の磁
束密度が高いほど磁区制御技術の効果が大きいため、磁
束密度の極めて高い製品を開発する必要性が高まってき
た。On the other hand, in recent years, against the backdrop of soaring energy prices, transformer manufacturers are increasingly focusing on materials for low iron loss transformers. Amorphous alloy or 6.5% S as low iron loss material
Although the development of i-steel and the like is in progress, there are still problems to be solved for industrial use as a transformer material.
On the other hand, magnetic domain control technology using laser etc. has been recently developed,
As a result, the iron loss characteristics were significantly improved. Further, the higher the magnetic flux density of the product, the greater the effect of the magnetic domain control technology, so that it is necessary to develop a product having an extremely high magnetic flux density.
含Al一方向性電磁鋼板を製造する方法において、最終
仕上焼鈍における昇温速度を低めとすることによって磁
束密度を高める方法が提案されているが(特公昭56-334
50)、被膜形成が困難になる等解決すべき問題を残して
いる。As a method for producing an Al-containing grain-oriented electrical steel sheet, a method has been proposed in which the magnetic flux density is increased by decreasing the temperature rising rate in final finishing annealing (Japanese Patent Publication No. 56-334).
50), there are still problems to be solved, such as difficulty in film formation.
一方向性電磁鋼板を製造する場合極めて高い磁束密度
をもつ製品を安定して得ることが難しいという問題点を
解決する方法を提供するものである。It is intended to provide a method for solving the problem that it is difficult to stably obtain a product having an extremely high magnetic flux density when producing a grain-oriented electrical steel sheet.
本発明はAlNを主インヒビターとし、珪素鋼熱延板を
必要に応じて焼鈍し、圧下率80超〜95%の強圧下最終冷
間圧延を含む1回以上の冷間圧延と、その間に行なう中
間焼鈍と最終冷間圧延後の脱炭焼鈍、最終仕上焼鈍を施
して一方向性電磁鋼板を製造する方法において、上記最
終仕上焼鈍を行なう際700℃から900〜1050℃の温度域ま
では2〜50℃/hrで、昇温を行ない、ひき続き700〜1000
℃の温度域まで降温させ、次いで1100〜1300℃の仕上焼
鈍温度まで2〜50℃/hrで昇温させることによって極め
て磁束密度の高い一方向性電磁鋼板の製造する方法を提
供するものである。The present invention uses AlN as a main inhibitor, anneales a hot-rolled silicon steel sheet as required, and performs one or more cold rolling processes including a final cold rolling process with a deep reduction of 80 to 95% in rolling reduction, and in between. In a method for producing a grain-oriented electrical steel sheet by performing decarburization annealing after intermediate annealing, final cold rolling, and final finishing annealing, when performing the final finishing annealing, the temperature range from 700 ° C to 900 to 1050 ° C is 2 Raises the temperature at ~ 50 ° C / hr and continues for 700-1000
A method for producing a grain-oriented electrical steel sheet having an extremely high magnetic flux density by lowering the temperature to a temperature range of 0 ° C and then raising the temperature to a finishing annealing temperature of 1100 to 1300 ° C at 2 to 50 ° C / hr is provided. .
即ち本発明者らは、AlNを主インヒビターとする上記
一方向性電磁鋼板の製造方法において、極めて磁束密度
の高い製品を安定して得ることが難しいという問題点を
解決する方法を種々検討した結果、最終仕上焼鈍を行な
う際700℃から900〜1050℃の温度域までは2〜50℃/hr
で昇温を行ない、ひき続き700〜1000℃の温度域まで降
温させ次いで1100〜1300℃の仕上焼鈍温度まで2〜50℃
/hrで昇温させることによって磁束密度が極めて高くな
るという現象を発見した。That is, the present inventors, in the manufacturing method of the above-described grain-oriented electrical steel sheet using AlN as the main inhibitor, various examination results of methods for solving the problem that it is difficult to stably obtain a product with extremely high magnetic flux density. , 2 to 50 ℃ / hr from 700 ℃ to 900 to 1050 ℃ in the final finish annealing
At a temperature of 700 to 1000 ° C and then to a finish annealing temperature of 1100 to 1300 ° C at 2 to 50 ° C.
We discovered a phenomenon in which the magnetic flux density becomes extremely high by raising the temperature at / hr.
以下本発明を詳細に説明する。 The present invention will be described in detail below.
本発明の出発素材である珪素鋼熱延板の成分について
はSi:2.5〜4.0%、C:0.03〜0.10%、酸可溶性Al:0.010
〜0.065%、N:0.0010〜0.0150%、Mn:0.02〜0.30%、S:
0.005〜0.040%を含有する必要がある。Regarding the components of the silicon steel hot-rolled sheet which is the starting material of the present invention, Si: 2.5-4.0%, C: 0.03-0.10%, acid-soluble Al: 0.010
~ 0.065%, N: 0.0010-0.0150%, Mn: 0.02-0.30%, S:
It is necessary to contain 0.005 to 0.040%.
Siは4.0%を超すと脆化が激しく冷間圧延が困難とな
り好ましくない。一方2.5%未満では電気抵抗が低く良
好な鉄損特性を得難い。If Si exceeds 4.0%, brittleness is severe and cold rolling becomes difficult, which is not preferable. On the other hand, if it is less than 2.5%, the electric resistance is low and it is difficult to obtain good iron loss characteristics.
Cは0.03%未満では脱炭工程以前でのγ量が極めて少
なくなってしまい良好な1次再結晶組織が得難い。一方
0.10%を超えると脱炭不良となり好ましくない。If C is less than 0.03%, the amount of γ before the decarburization step becomes extremely small, and it is difficult to obtain a good primary recrystallization structure. on the other hand
If it exceeds 0.10%, decarburization becomes poor, which is not preferable.
酸可溶性Al,Nは本発明において高磁束密度を得るため
に必須の主インヒビターAlNを得るための基本成分であ
り、上記範囲を外れると2次再結晶が不安定となり好ま
しくないので酸可溶性Alは、0.010〜0.065%、Nは0.00
10〜0.0150%とする。The acid-soluble Al, N is a basic component for obtaining the main inhibitor AlN essential for obtaining a high magnetic flux density in the present invention, and if it deviates from the above range, secondary recrystallization becomes unstable, which is not preferable. , 0.010 to 0.065%, N is 0.00
10 to 0.0150%.
またMnおよびSはインヒビターMnSを形成するために
必要な元素であり、上記範囲を外れると2次再結晶が不
安定となり好ましくないのでMnは0.02〜0.30%、Sは0.
005〜0.040%と定める。Further, Mn and S are elements necessary for forming the inhibitor MnS, and if it is out of the above range, secondary recrystallization becomes unstable, which is not preferable. Therefore, Mn is 0.02 to 0.30% and S is 0.
Specified as 005 to 0.040%.
その他インヒビター構成元素として公知であるSn,Sb,
Se,Te,Cu,Nb,Cr,Ni,B,V,As,Bi等を必要に応じて含有さ
せてよい。Other known Sn, Sb, as inhibitor constituent elements,
If necessary, Se, Te, Cu, Nb, Cr, Ni, B, V, As, Bi, etc. may be contained.
本発明は上記成分を含有する珪素鋼熱延板を出発材と
し、必要に応じて焼鈍し、圧下率80超〜95%の強圧下最
終冷間圧延を含む1回以上の冷間圧延と、その間に行な
う中間焼鈍と最終冷間圧延後の脱炭焼鈍、最終仕上焼鈍
を施す製造工程を前提としている。The present invention uses a silicon steel hot-rolled sheet containing the above components as a starting material, annealed as necessary, and one or more cold rolling operations including a final cold rolling with a reduction ratio of more than 80 to 95%. It is premised on a manufacturing process in which intermediate annealing, decarburization annealing after final cold rolling, and final finishing annealing are performed during that time.
本発明はAlNを主インヒビターとしており、AlNの析出
処理を目的として、700〜1200℃の熱延板焼鈍を必要に
応じて行なう。In the present invention, AlN is used as a main inhibitor, and hot-rolled sheet annealing at 700 to 1200 ° C is performed as necessary for the purpose of precipitation treatment of AlN.
2回以上の冷間圧延を行なう際の冷間圧延の間に行な
う中間焼鈍は700〜1200℃の温度で行なう。The intermediate annealing performed during cold rolling when performing cold rolling twice or more is performed at a temperature of 700 to 1200 ° C.
最終強圧下冷間圧延の圧下率は80超〜95%にする必要
がある。80%以下では高磁束密度が得難く、95%を超え
ると脱炭焼鈍後の集合組織が不適切となるため2次再結
晶に不安定が生じる。The reduction ratio of the final strong cold rolling should be over 80-95%. If it is less than 80%, it is difficult to obtain a high magnetic flux density, and if it exceeds 95%, the texture after decarburization annealing becomes inadequate and secondary recrystallization becomes unstable.
最終強圧下冷間圧延後鋼板に700〜900℃の温度で脱炭
焼鈍を行なう。脱炭焼鈍後の鋼板表面に焼鈍分離剤を塗
布し、次いで最終仕上焼鈍を行ない製品とする。本発明
の特徴はこの最終仕上焼鈍工程にある。After the final high-pressure cold rolling, the steel sheet is decarburized and annealed at a temperature of 700 to 900 ° C. An annealing separator is applied to the surface of the steel sheet after decarburization annealing, and then final finishing annealing is performed to obtain a product. The feature of the present invention lies in this final finish annealing step.
最終仕上焼鈍を行なう際は、700℃から900〜1050℃の
温度域までは2〜50℃/hrで昇温を行ない、ひき続き700
〜1000℃の温度域まで降温させ、次いで1100〜1300℃の
仕上焼鈍温度まで2〜50℃/hrで昇温させる必要があ
る。以下最終仕上焼鈍条件の限定理由を説明する。When performing the final finishing annealing, the temperature is raised at 2 to 50 ° C / hr from 700 ° C to 900 to 1050 ° C, and then 700
It is necessary to lower the temperature to a temperature range of up to 1000 ° C and then raise the temperature to a finishing annealing temperature of 1100 to 1300 ° C at 2 to 50 ° C / hr. The reasons for limiting the final finish annealing conditions will be described below.
本発明者らは、2次再結晶挙動を詳細に調査した結果
次のような新しい知見を得た。第1図に2次再結晶開始
初期及び2次再結晶完了期の2次再結晶粒の方位の一例
を示す。2次再結晶開始初期の2次再結晶粒の方位は
{110}<001>に極めて近く、2次再結晶が進行するに
従って{110}<001>方位から分散した方位粒が2次再
結晶してくるのがわかる。2次再結晶現象は本質的には
鉄の拡散による現象であり、温度によって大きな影響を
受ける。本発明者らは2次再結晶開始初期の2次再結晶
粒が{110}<001>に極めて近いことに着目し、2次再
結晶開始直前又は開始初期に温度を降下させることによ
って鉄の拡散を抑制し{110}<001>に極めて近い方位
粒のみを2次再結晶させることが可能ではないかと推定
して広範な実験を行なった。以下実験結果に基づいて詳
細に説明する。As a result of detailed investigation of the secondary recrystallization behavior, the present inventors have obtained the following new findings. FIG. 1 shows an example of the orientation of secondary recrystallized grains in the initial stage of secondary recrystallization and the stage of completion of secondary recrystallization. The orientation of the secondary recrystallized grains at the beginning of the secondary recrystallization is very close to {110} <001>. As the secondary recrystallization progresses, the oriented grains dispersed from the {110} <001> orientation are secondary recrystallized. I can see it coming. The secondary recrystallization phenomenon is essentially a phenomenon due to iron diffusion, and is greatly affected by temperature. The present inventors have noticed that the secondary recrystallized grains in the initial stage of the secondary recrystallization are very close to {110} <001>. Extensive experiments were conducted assuming that it would be possible to suppress the diffusion and to recrystallize only the grains oriented very close to {110} <001>. The details will be described below based on the experimental results.
第2図に最終仕上焼鈍の途中過程で降温を始めた温度
と製品の磁束密度との関係を示す。この場合Si:3.27
%、C:0.078%、酸可溶性Al:0.026%、N:0.0085%、Mn:
0.071%、S:0.025%を含有する2.3mm厚の熱延板を出発
材とし、かかる熱延板を1100℃2分間の焼鈍後急冷し、
0.225mmの最終厚みまで冷間圧延し、ついで脱炭焼鈍を
行なった後MgOを主成分とする焼鈍分離剤を塗布し、15
℃/hrの昇温速度で、第2図に示す各温度まで昇温した
後、800℃まで降温した。800℃に達した時点で再び15℃
/hrの昇温速度で昇温を始め、1200℃まで昇温を行なっ
た後20時間1200℃に保持した。ここでの焼鈍雰囲気は、
室温から1200℃までは25%N2+75%H2とし、1200℃での
保定中は100%H2とした。第2図から明らかなように降
温開始温度900〜1050℃の範囲で磁束密度の向上効果が
見られ、第2図を基に降温開始温度を規定した。FIG. 2 shows the relationship between the temperature at which the temperature starts to be lowered during the final annealing and the magnetic flux density of the product. In this case Si: 3.27
%, C: 0.078%, acid-soluble Al: 0.026%, N: 0.0085%, Mn:
Starting material is a hot rolled sheet having a thickness of 2.3 mm containing 0.071% and S: 0.025%, and the hot rolled sheet is annealed at 1100 ° C. for 2 minutes and then rapidly cooled,
Cold rolled to a final thickness of 0.225 mm, then decarburized and annealed with MgO-based annealing separator,
After the temperature was raised to each temperature shown in FIG. 2 at a temperature rising rate of ° C / hr, the temperature was lowered to 800 ° C. 15 ℃ again when 800 ℃ is reached
The temperature was raised at a heating rate of / hr, the temperature was raised to 1200 ° C, and then the temperature was kept at 1200 ° C for 20 hours. The annealing atmosphere here is
From room temperature to 1200 ° C, 25% N 2 + 75% H 2 was used, and during retention at 1200 ° C, 100% H 2 was used. As is clear from FIG. 2, the effect of improving the magnetic flux density was observed in the temperature-fall start temperature range of 900 to 1050 ° C., and the temperature-fall start temperature was specified based on FIG.
そこで、900〜1050℃の温度域から700〜1000℃の温度
域まで降温させる。純化を目的として鋼板を1100℃以上
にする必要上、700℃未満にまで降温させると製造コス
トが増加するため好ましくなく、1000℃を超えると2次
再結晶の進行が速いため効果が得難いので700〜1000℃
の温度域まで降温させると規定した。Therefore, the temperature is lowered from 900 to 1050 ° C to 700 to 1000 ° C. Since it is necessary to raise the temperature of the steel sheet to 1100 ° C or higher for the purpose of purification, lowering the temperature to less than 700 ° C increases the manufacturing cost, which is not preferable, and if it exceeds 1000 ° C, it is difficult to obtain the effect because the progress of secondary recrystallization is fast. ~ 1000 ° C
It was specified that the temperature be lowered to the temperature range of.
続いて、700〜1000℃の温度域から1100〜1300℃の仕
上焼鈍温度まで昇温させる。1100℃未満で純化を行なう
と時間がかかりすぎ好ましくなく、純化の点で1300℃超
まで温度を上げる必要がない上製造コストが増加して好
ましくない。Subsequently, the temperature is raised from the temperature range of 700 to 1000 ° C to the finishing annealing temperature of 1100 to 1300 ° C. Purification at less than 1100 ° C is not preferable because it takes too much time, and in terms of purification, it is not necessary to raise the temperature to more than 1300 ° C and the manufacturing cost increases.
700℃から900〜1050℃の温度域までの昇温速度は2〜
50℃/hrとした。2℃/hr未満では2次再結晶が不安定と
なり好ましくなく、50℃/hrを超えると2次再結晶の核
発生が過度となり、{110}<001>方位から分散したも
のまで容易に核発生し結果として磁束密度が低下して好
ましくない。The rate of temperature rise from 700 ℃ to 900-1050 ℃ is 2
It was set to 50 ° C./hr. If it is less than 2 ° C / hr, the secondary recrystallization becomes unstable, which is not preferable, and if it exceeds 50 ° C / hr, the nucleation of the secondary recrystallization becomes excessive, and the nuclei easily disperse from the {110} <001> orientation. As a result, the magnetic flux density is lowered, which is not preferable.
700〜1000℃の温度域から1100〜1300℃の仕上焼鈍温
度までの昇温速度は2〜50℃/hrとした。2℃/hr未満で
は2次再結晶が不安定となり、好ましくなく、50℃/hr
を超えると、2次再結晶の核が過度に発生しやすくな
り、{110}<001>方位から分散したものまで容易に核
発生し結果として磁束密度が低下して好ましくない。The heating rate from the temperature range of 700 to 1000 ° C to the finishing annealing temperature of 1100 to 1300 ° C was 2 to 50 ° C / hr. If it is less than 2 ° C / hr, secondary recrystallization becomes unstable, which is not preferable, and 50 ° C / hr
When it exceeds, the secondary recrystallization nuclei are likely to be excessively generated, and nuclei are easily generated from the {110} <001> orientation to dispersed ones, resulting in a decrease in magnetic flux density, which is not preferable.
本発明の特徴である900〜1050℃の温度域から700〜10
00℃の温度域まで降温させる効果のメカニズムについて
は必ずしも明らかではないが、本発明者らは以下のよう
に考えている。第1図に示すように、2次再結晶開始初
期の2次再結晶粒の方位は{110}<001>方位に極めて
近い。これは{110}<001>に極めて近い方位粒の核発
生が{110}<001>から分散した方位の核発生よりも早
期に起ることを示唆している。2次再結晶の核の発生に
関してはいくつかの考え方があるが、鉄の拡散を必要と
するという点では共通している。拡散現象自体温度に強
く依存することは知られており、{110}<001>に極め
て近い方位粒の核が発生した段階で温度を下げると{11
0}<001>から分散した方位粒の核発生が生じなくなる
ものと考えられる。700〜1000℃のいずれかの温度から1
100〜1300℃のいずれかの温度までの昇温中既に核発生
している{110}<001>に極めて近い方位粒は容易に2
次再結晶粒となり粒成長していくのに対して、{110}
<001>から分散した方位粒は降温を始めた温度以上に
達っした時にようやく核発生時期を迎えることになる。
そしてその時点では{110}<001>に極めて近い2次再
結晶粒が鋼板のかなりの部分を占めてしまって{110}
<001>から分散した方位粒の核発生が可能な鋼板部分
が少なくなっていると考えられる。従って本発明の効果
は{110}<001>から分散した方位粒の核発生を積極的
に抑制することによって、{110}<001>に極めて近い
2次再結晶粒が鋼板を占める割合を増加させたことによ
ると考えられる。From the temperature range of 900 to 1050 ° C, which is a feature of the present invention,
Although the mechanism of the effect of lowering the temperature to the temperature range of 00 ° C is not always clear, the present inventors consider as follows. As shown in FIG. 1, the orientation of the secondary recrystallized grains at the initial stage of the secondary recrystallization is very close to the {110} <001> orientation. This suggests that nucleation of grains oriented very close to {110} <001> occurs earlier than nucleation of grains dispersed from {110} <001>. There are some ideas regarding the generation of secondary recrystallization nuclei, but they are common in that they require diffusion of iron. It is known that the diffusion phenomenon itself strongly depends on the temperature, and if the temperature is lowered at the stage when nuclei of oriented grains very close to {110} <001> are generated, {11
It is considered that nucleation of dispersed oriented grains does not occur from 0} <001>. 1 from any temperature from 700 to 1000 ℃
It is easy to obtain oriented grains that are extremely close to {110} <001>, which has already nucleated during heating to any temperature between 100 and 1300 ℃.
Next recrystallized grains become grains and grow, whereas {110}
The oriented grains dispersed from <001> will finally reach the nucleation time when the temperature reaches or exceeds the temperature at which the temperature begins to drop.
At that time, secondary recrystallized grains very close to {110} <001> occupied a large part of the steel sheet {110}.
It is considered that the number of steel sheet parts where nuclei of oriented grains dispersed from <001> can be generated has decreased. Therefore, the effect of the present invention is to positively suppress the nucleation of oriented grains dispersed from {110} <001>, thereby increasing the proportion of secondary recrystallized grains extremely close to {110} <001> in the steel sheet. It is thought that this is due to what was done.
1100〜1300℃の仕上焼鈍温度まで昇温した後はS,N等
の不純物の純化のために1100〜1300℃の温度範囲に5時
間以上保持する。After the temperature is raised to the finishing annealing temperature of 1100 to 1300 ° C, the temperature is kept at 1100 to 1300 ° C for 5 hours or more to purify impurities such as S and N.
最終仕上焼鈍中の雰囲気については特に限定しない
が、室温から900〜1050℃の温度域までの昇温過程、ひ
き続く700〜1000℃の温度域までの降温過程、ひき続く1
100〜1300℃の仕上焼鈍温度までの昇温過程において焼
鈍雰囲気に5%以上の窒素ガスが含まれていることは2
次再結晶の安定化の点で好ましい。The atmosphere during the final finish annealing is not particularly limited, but the temperature raising process from room temperature to 900 to 1050 ° C, the temperature lowering process to 700 to 1000 ° C, and the subsequent 1
It is 2 that the annealing atmosphere contains 5% or more of nitrogen gas during the temperature rising process up to the finishing annealing temperature of 100 to 1300 ℃.
It is preferable from the viewpoint of stabilizing the subsequent recrystallization.
最終仕上焼鈍後に鋼板に張力を付加するコーティング
を行なうと鉄損特性が一層向上する。本発明によって製
造された製品は極めて磁束密度が高いため、レーザー等
を用いた磁区制御を行なうと極めて鉄損特性の優れた製
品になる。The iron loss characteristics are further improved by coating the steel sheet with tension after the final finish annealing. Since the magnetic flux density of the product manufactured by the present invention is extremely high, magnetic domain control using a laser or the like makes the product extremely excellent in iron loss characteristics.
以下実施例について述べる。Examples will be described below.
実施例1 Si:3.25%、C:0.078%、酸可溶性Al:0.026%、N:0.00
85%、Mn:0.071%、S:0.025%、Sn:0.12%、Cu:0.07%
を含む板厚2.3mmの熱延板に1100℃2分間の焼鈍後0.225
mmの最終厚みまで冷間圧延し、ついで脱炭焼鈍し、ひき
続きMgOを主成分とする焼鈍分離剤を塗布し、1200℃
まで15℃/hrで昇温、950℃まで15℃/hrで昇温後800℃
まで降温し再び15℃/hrで1200℃まで昇温、1000℃ま
で15℃/hrで昇温後800℃まで降温し再び15℃/hrで1200
℃まで昇温の3通りの処理後ひき続き1200℃で20時間保
持した。焼鈍雰囲気は1200℃以下では25%N2+75%H2と
し1200℃になった時点で100%H2とした。処理条件と製
品の磁束密度との関係を第1表に示す。Example 1 Si: 3.25%, C: 0.078%, acid-soluble Al: 0.026%, N: 0.00
85%, Mn: 0.071%, S: 0.025%, Sn: 0.12%, Cu: 0.07%
0.225 after annealing at 1100 ℃ for 2 minutes on a hot rolled sheet with a thickness of 2.3mm
Cold rolled to a final thickness of mm, then decarburized and annealed, and subsequently annealed and separated with MgO as the main component and applied at 1200 ° C.
Up to 15 ° C / hr, up to 950 ° C at 15 ° C / hr, then 800 ° C
Then, the temperature is lowered to 15 ° C / hr to 1200 ° C again, the temperature is raised to 1000 ° C at 15 ° C / hr and then lowered to 800 ° C, and again at 15 ° C / hr to 1200 ° C.
After three kinds of treatments of raising the temperature to ℃, the temperature was continuously maintained at 1200 ℃ for 20 hours. The annealing atmosphere was 25% N 2 + 75% H 2 below 1200 ° C and 100% H 2 at 1200 ° C. Table 1 shows the relationship between the processing conditions and the magnetic flux density of the product.
実施例2 Si:3.51%、C:0.084%、酸可溶性Al:0.025%、N:0.00
80%、Mn:0.075%、S:0.024%、Sn:0.16%を含む板厚2.
3mmの熱延板に1100℃2分間の焼鈍後0.225mmの最終厚み
まで冷間圧延し、ついで脱炭焼鈍し、ひき続きMgOを主
成分とする焼鈍分離剤を塗布し、1200℃まで15℃/hr
で昇温、950℃まで15℃/hrで昇温後800℃まで降温し
再び15℃/hrで1200℃まで昇温の2通りの処理後ひき続
き1200℃で20時間保持した。焼鈍雰囲気は1200℃以下で
は25%N2+75%H2とし1200℃になった時点で100%H2と
した。処理条件と製品の磁束密度との関係を第2表に示
す。 Example 2 Si: 3.51%, C: 0.084%, acid-soluble Al: 0.025%, N: 0.00
Plate thickness including 80%, Mn: 0.075%, S: 0.024%, Sn: 0.16% 2.
3mm hot rolled sheet was annealed at 1100 ℃ for 2 minutes, cold-rolled to a final thickness of 0.225mm, then decarburized and annealed with MgO-based annealing separator. / hr
Then, the temperature was raised to 950 ° C. at 15 ° C./hr, then lowered to 800 ° C., and again raised to 1200 ° C. at 15 ° C./hr. After two treatments, the temperature was kept at 1200 ° C. for 20 hours. The annealing atmosphere was 25% N 2 + 75% H 2 below 1200 ° C and 100% H 2 at 1200 ° C. Table 2 shows the relationship between the processing conditions and the magnetic flux density of the product.
実施例3 Si:3.29%、C:0.075%、酸可溶性Al:0.026%、N:0.00
85%、Mn:0.071%、S:0.025%、Sn:0.12%、Cu:0.06%
を含む板厚2.3mmの熱延板に1100℃2分間の焼鈍後0.225
mmの最終厚みまで冷間圧延し、ついで脱炭焼鈍し、ひき
続きMgOを主成分とする焼鈍分離剤を塗布し、1200℃
まで15℃/hrで昇温、1000℃まで15℃/hrで昇温し、10
00℃で15時間保持後15℃/hrで1200℃まで昇温、1000
℃まで15℃/hrで昇温後800℃まで降温し、再び15℃/hr
で1200℃まで昇温の3通りの処理後ひき続き1200℃で20
時間保持した。焼鈍雰囲気は1200℃以下では25%N2+75
%H2として1200℃になった時点で、100%H2とした。処
理条件と製品の磁束密度との関係を第3表に示す。 Example 3 Si: 3.29%, C: 0.075%, acid-soluble Al: 0.026%, N: 0.00
85%, Mn: 0.071%, S: 0.025%, Sn: 0.12%, Cu: 0.06%
0.225 after annealing at 1100 ℃ for 2 minutes on a hot rolled sheet with a thickness of 2.3mm
Cold rolled to a final thickness of mm, then decarburized and annealed, and subsequently annealed and separated with MgO as the main component and applied at 1200 ° C.
Up to 15 ° C / hr, up to 1000 ° C at 15 ° C / hr,
After holding at 00 ℃ for 15 hours, heat up to 1200 ℃ at 15 ℃ / hr, 1000
After increasing the temperature to 15 ℃ / hr at 15 ℃ / hr, decrease the temperature to 800 ℃ and then again at 15 ℃ / hr.
After the temperature is raised to 1200 ° C, the temperature is increased to 1200 ° C and the temperature is increased to 1200 ° C for 20
Held for hours. The annealing atmosphere is 25% N 2 +75 below 1200 ° C.
When it reached 1200 ° C. as% H 2 , it was set to 100% H 2 . Table 3 shows the relationship between the processing conditions and the magnetic flux density of the product.
〔発明の効果〕 以上のとおり、本発明によれば、最終仕上焼鈍工程の
熱サイクルに降温部を付加することによって極めて磁束
密度の高い一方向性電磁鋼板を安定して製造することが
できるので、その工業的効果は大きい。 [Advantages of the Invention] As described above, according to the present invention, it is possible to stably produce a grain-oriented electrical steel sheet having an extremely high magnetic flux density by adding a temperature lowering section to the heat cycle of the final finishing annealing step. , Its industrial effect is great.
第1図は2次再結晶開始初期と2次再結晶完了期の2次
再結晶粒の方位の比較図。第2図は最終仕上焼鈍の工程
中降温を開始する温度と製品の磁束密度との関係図であ
る。FIG. 1 is a comparison diagram of the orientations of secondary recrystallized grains at the initial stage of secondary recrystallization and at the stage of completion of secondary recrystallization. FIG. 2 is a diagram showing the relationship between the temperature at which the temperature starts to be lowered during the final finish annealing step and the magnetic flux density of the product.
Claims (1)
%、solAl:0.010〜0.065%、N:0.0010〜0.0150%、Mn:
0.02〜0.30%、S:0.005〜0.040%および残部が実質的に
Feからなる珪素鋼熱延板を、圧下率:80超〜95%の強圧
下最終冷間圧延を含む1回或は中間焼鈍過程を介挿する
2回以上の冷間圧延を行い、次いで脱炭焼鈍、焼鈍分離
剤塗布さらに最終仕上焼鈍を施して一方向性電磁鋼板を
製造する方法において、前記最終仕上焼鈍を行うに際
し、上記成分を有する珪素鋼板を700℃から900〜1050℃
の温度域内までを2〜50℃/hrの昇温速度で加熱し、次
いで700〜1000℃の温度域内まで降温せしめさらに、110
0〜1300℃の仕上焼鈍温度まで2〜50℃/hrの昇温速度で
加熱することを特徴とする磁束密度の極めて高い一方向
性電磁鋼板の製造方法。1. By weight%, Si: 2.5-4.0%, C: 0.03-0.10
%, SolAl: 0.010 to 0.065%, N: 0.0010 to 0.0150%, Mn:
0.02-0.30%, S: 0.005-0.040% and the balance is substantially
Hot-rolled silicon steel sheet made of Fe is subjected to one or more cold rolling including a final cold rolling under a strong reduction with a rolling reduction ratio of over 80 to 95%, or two or more cold rolling steps followed by de-rolling. Charcoal annealing, a method for producing a unidirectional electrical steel sheet by applying final finishing annealing, further applying an annealing separator, in performing the final finishing annealing, the silicon steel sheet having the above components from 700 ℃ to 900 ~ 1050 ℃
Within a temperature range of 2 to 50 ° C / hr and then to a temperature range of 700 to 1000 ° C.
A method for producing a grain-oriented electrical steel sheet having an extremely high magnetic flux density, which comprises heating to a finishing annealing temperature of 0 to 1300 ° C at a temperature rising rate of 2 to 50 ° C / hr.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62083852A JPH0826398B2 (en) | 1987-04-07 | 1987-04-07 | Method for producing unidirectional electrical steel sheet with extremely high magnetic flux density |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62083852A JPH0826398B2 (en) | 1987-04-07 | 1987-04-07 | Method for producing unidirectional electrical steel sheet with extremely high magnetic flux density |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63250420A JPS63250420A (en) | 1988-10-18 |
| JPH0826398B2 true JPH0826398B2 (en) | 1996-03-13 |
Family
ID=13814225
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62083852A Expired - Lifetime JPH0826398B2 (en) | 1987-04-07 | 1987-04-07 | Method for producing unidirectional electrical steel sheet with extremely high magnetic flux density |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0826398B2 (en) |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5855212A (en) * | 1981-09-29 | 1983-04-01 | Toyota Motor Corp | Molding of model |
-
1987
- 1987-04-07 JP JP62083852A patent/JPH0826398B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63250420A (en) | 1988-10-18 |
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