JPS6239229B2 - - Google Patents
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- JPS6239229B2 JPS6239229B2 JP10299182A JP10299182A JPS6239229B2 JP S6239229 B2 JPS6239229 B2 JP S6239229B2 JP 10299182 A JP10299182 A JP 10299182A JP 10299182 A JP10299182 A JP 10299182A JP S6239229 B2 JPS6239229 B2 JP S6239229B2
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Description
本発明は、超細粒フエライト鋼、特に熱間圧延
ままで、しかもNb、Ta、Mo、W等の特殊な合金
元素を含まない亜共析鋼を主体とした超細粒フエ
ライト鋼とその製造方法に関するものである。
ここで言う細粒フエライト組織は大部分、通常
70〜80%以上が微細フエライト結晶粒より成り、
所望の機械的性質によつてはフエライト相以外に
他の微細な組織、例えばパーライト、マルテンサ
イト、残留オーステナイト等のうち一つまたは二
つ以上を有しても良いし、カーバイドやナイトラ
イド等の析出物を有していても良い。
本発明で細粒フエライトと呼ぶ組織は、粒の形
の著しい伸長を伴わず、ほぼ等方的であり、また
原則としていわゆる大傾角粒界で囲まれた結晶粒
からなる組織を指し、亜結晶粒界(小傾角粒界)
は粒界として見なしていない。ただし、このよう
な粒の内部に多少の転位密度の増加と亜粒界の形
成はあり得る。
鋼の種々の強化方法のうちで結晶粒の微細化は
強度と共に靭性をも高くする唯一の方法として知
られており、特に熱延ままで使用される鉄鋼材料
の材質向上を計る際には殆んどの場合に先ず考慮
されねばならない重要な技術である。従来の細粒
化技術で工業的に達成されているのは小さくて4
〜6μm程度である。これは通常制御圧延法と呼
ばれる方法で行われており、Nb等の合金元素を
含む鋼を比較的低温域で強い圧延を行う技術であ
る。この場合Nbが圧延ままで固溶している必要
があるので、圧延前に例えば1200℃以上という高
温で加熱を行なつてNbを固溶させ、しかるのち
に仕上圧延は800℃以下という低温域で行うの
で、鋼板の温度低下を待つため生産効率が著しく
低下し、また圧延時の変形抵抗が著しく高くなる
ために圧延機に対する負荷が大であるなど工業的
に欠点がある。この他に低温域で加熱して圧延を
行う方法、あるいは圧延後強制冷却を行う方法な
ど種々提案されているが、いずれも上記粒径範囲
内に留つており、本発明で言う超微細粒(3〜4
μm以下)を工業的に得るには至つていない。
一方、超微細粒組織を実験的に得る方法が最近
検討されている。例えば、Ni鋼などで、変態点
前後で数回繰り返し焼鈍を行う方法などである。
しかしこのような熱処理は、経済性から見て工業
的に実施することは困難であることは明らかであ
る。
本発明は実際に工業的に得られるこのような画
期的な超細粒鋼に関するものであり、とくに特殊
な合金元素を用いずCを主成分とする亜共析鋼
で、しかも熱間加工ままで得られる鋼に関するも
ので、とくにP、S、N等の不純物を低減するこ
とにより容易に製造できるという画期的な技術に
関するものである。
すなわち、本発明の要旨とするところは下記の
とおりである。
(1) 重量%でC:0.3%以下、Si:1.5%以下、
Mn:2%以下、N:0.002%未満、残部Feおよ
び不可避的不純物よりなり、その金属組織中に
平均4μm以下の大傾角粒界に囲まれた加工誘
起等軸フエライト結晶粒を体積率で70%以上含
むことを特徴とする高強度でしかも延性のすぐ
れた超細粒フエライト鋼。
(2) 重量%でC:0.3%以下、Si:1.5%以下、
Mn:2%以下、N:0.002%未満、残部Feおよ
び不可避的不純物からなる鋼をAc3変態点以上
の温度に加熱してから冷却する過程において熱
間加工を行い、その終段において、600℃〜
(Ar3+100℃)の温度域で1秒以内に1回また
は2回以上の合計減面率が35%以上であるよう
な加工を加えることを特徴とする高強度でしか
も延性のすぐれた超細粒フエライト鋼の製造方
法。
以下に本発明の詳細について説明する。
本発明鋼は上述のような超細粒フエライト鋼で
あるが、本発明で細粒フエライトと呼ぶ組織は粒
の形の著しい伸長は伴わず、ほぼ等方向であり、
また、原則としていわゆる大傾角粒界で囲まれた
結晶粒からなる組織を指し、亜結晶粒界(小傾角
粒界)は粒界と見なしていない。
本発明で鋼の化学成分を規定した理由は次の通
りである。
C含有量を0.3%以下とした理由は、一般にC
量が大きくなるとフエライト量が減少し、パーラ
イトが主体の鋼となるが、本発明鋼では同一C量
でも通常の場合よりはるかにフエライト量を増す
ことができるので、C:0.3%まではフエライト
主体の組織を得ることができるが、これを超える
とパーライト等の量が多くなりフエライト主体の
鋼を得ることは難しくなるからである。
Siは鋼に通常脱酸等の目的で添加され多少は含
有されており、また本発明においてはフエライト
量を増加させる効果があるので故意に添加する場
合もある。しかし1.5%を超えて添加するとフエ
ライト結晶粒が粗大化しやすくなるので1.5%以
下とした。
Mnは変態点を調節し、加工誘起変態を起こし
やすくし、また加工誘起フエライトの急速な粒成
長を防止することにより細粒化に寄与するが、2
%を超えて添加すると変態温度が下りすぎてフエ
ライト量が70%に達しない場合が生ずるので2%
以下とした。
PおよびSは通常鋼中に多少は含有される元素
であるが、多量に含有されれば鋼の延靭性を損
う。本発明においては特にその量は少いほど好ま
しい。それはP、Sが少いほど本発明鋼の生成機
構である加工誘起変態および再結晶が起りやすい
からであり、Pが0.015%以下、Sが0.010%以下
であることが望ましい。
Nは不純物元素として鋼中に多少は含有される
が、上述のP、Sと同様の理由で低いほど特性が
優れるとともに本発明鋼が得られやすくなる。こ
の量が0.002%以上になると特にAl、Tiなどの窒
化物形成元素を含む鋼において工業的にかなりむ
ずかしい大圧下の熱間加工を与えないと本発明鋼
が生成しにくくなるため、本発明鋼では0.002%
未満とした。
Alは通常脱酸のため鋼中に多少は含まれてい
るが、通常含有される程度0.1%ならば、一般に
本発明鋼の特性に大きい影響を与えることはな
い。
また、Nb、Ta、Mo、W等はいずれもオーステ
ナイトの再結晶および変態を遅らせる元素として
知られている。本発明鋼では熱間加工時にオース
テナイトの変態および再結晶を促して細粒化する
ものであるから、Nb、Ta、Mo、W等はこれを阻
害する元素であるので、本発明鋼には含まれては
ならないのである。
かかる組成の鋼を次のような製造方法によつて
製造する。
本発明鋼の終段の加工に至る工程にはとくに制
限はない。すなわち通常に溶製された溶鋼は連続
鋳造によつてスラブにされても良いし、造塊―分
塊工程によつてスラブにされても良い。スラブは
高温のまま圧延工程に持ち来たされても良いし、
一旦冷却したものを再加熱しても良い。スラブの
加熱・加工条件としてはスラブが本発明の加工工
程直前にそのオーステナイト粒径が小さい程良く
なるものが一般的に望ましいと言えるが、本発明
の加工工程以前の条件は通常のもので良いので制
限は設けない。
本発明の製造方法の特徴は該鋼を600℃〜
(Ar3+100℃)の温度域において、短時間内の大
圧下を加えることである。ただし、ここでAr3変
態点とは鋼がオーステナイトである温度域から徐
冷途中でフエライト変態を開始する温度を指し、
以下単にAr3と言う)
本発明者等は従来研究の殆んどがなされていな
かつた大圧下加工の熱間加工組織に対する効果を
詳細に研究し、従来全く知られていなかつた新ら
しい知見を得た。その結果を模式的に第1図に示
す。この図で小減面率の領域については比較的よ
く知られていたし、また大圧下でも比較的高温域
ではオーステナイトが動的再結晶を起すことが最
近知られてきた。ところで今回、本発明に従つた
高純鋼を用いると、Ar3+100℃から600℃の間
で、大圧下を加えることにより加工時に変態が起
り、この時生成した細粒のフエライトが圧延中に
更に再結晶して一層細粒化することが知見され
た。
本発明の熱間加工条件の範囲は第1図及び第2
図に明示されている。
即ち、比較例として示した通常純度鋼(P:
0.015〜0.030%、S:0.008〜0.015%、N:
0.0025〜0.0050%)の場合では、適切な温度域に
おいて減面率が50%を超える。動的変態およびフ
エライトの再結晶が生じて3〜4μm以下の平均
フエライト粒径が得られるが、(第1図フエライ
ト動的再結晶域)、本発明に従つた高純鋼の場
合には減面率35%でも同様な細粒が得られ、更に
低温ではフエライトの完全な動的再結晶により細
粒化は更に著しくなり、2μmまたはそれ以下と
いう超微細粒となる(第1図フエライト動的再結
晶域へ拡大)。
これから、本発明に従つて鋼を高純度化するこ
とは極めて効果の大きいことがわかる。
第2図は累積減面率(%)とフエライト平均粒
径の関係を示したものであるが、本発明に従つた
鋼の場合、同一減面率において上記比較鋼に比
し、フエライト粒径が小さくなることを示してい
る。この場合の加工温度は本発明の場合は650〜
700℃、比較鋼の場合は750〜800℃である。
なお、この圧下は厚板圧延のように1パスで加
えるのが最も良いが、第2図に示したように短時
間で多パスで加えた累積歪でもほぼこれに近い効
果があるという知見を得た。この短時間は通常の
圧延においては1秒程度以内であればよいことも
知見した。従つて上記の圧下率は累積された合計
の減面率で置き換えることができる。
なお、このような短時間の累積圧下は第1図の
上部に示すように線材圧延の仕上段階、ホツトス
トリツプ圧延の後半で実際に実現が可能である。
上記の熱間加工は全体の加工の最終段に行われ
ることが望ましいが、場合により圧延材の形状調
整のための少量の熱間または冷間の変形を与えて
も大きくその特性を損うものではない。
加工後の粒成長を抑制するためには大なる冷却
速度で冷却する事が望ましい場合が多い。減面率
が十分に大きいときや加工仕上温度が適正な温度
域内で低温側のときは鋼材断面が小さければ放冷
しても細粒が得られるが、減面率が下限に近いと
きや、製品鋼材断面が大なる場合、また仕上温度
の高い場合は例えば20℃/sec以上の加速冷却が
有効である場合が多い。冷速が大きくて、少しで
も未変態オーステナイトが残存する場合はその部
分が硬い第二相となり、さらに強度を向上する効
果がある。このように目的によつては加速冷却で
材質、とくに強度を向上することができる。この
場合加速冷却を行なう温度域については、フエラ
イトの粒成長、あるいは圧延時に変態しなかつた
部分が冷却中にフエライトまたはパーライトに変
態する500℃以上の温度域を含むべきものである
のは当然である。
なお、本発明鋼は熱間圧延直後にこのような細
粒フエライトであることに特徴があり、徐冷を行
つて結晶粒を成長させることも特定の目的(集合
組織改善など)の場合にはありうる。
次に、このようにして製造された本発明鋼の金
属組織上の特徴について説明する。
上述のように本発明は高純な低炭素鋼を1パス
または多パスで、ある限度以上の圧下を適当な温
度域で加えると、加工により変態が容易に誘起さ
れ、しかもそれが極めて微細であるという新知見
に基づくものである。
このとき加工中に発生した変態核は加工直後に
その変態核境界の移動が直ちに止らないこと、お
よび加工歪(加工により誘起された高密度の転位
による)が直ちには回復しないので、境界面移動
に対する駆動力がある程度維持されること、のた
めに細粒フエライトは加工後にやや成長し、その
体積率も増大する。このような場合実験的に加工
中に変態した動的変態フエライト部と加工に引き
続き成長した準動的変態点フエライト部とを厳密
に区別することは困難であり、実用的にはその必
要もないので、加工後問題となる温度範囲で1秒
程度以内の時間経過後までの状態までを加工誘起
変態と定義することにする。
また、1パスでも特に大圧下加工の場合、また
特に2パス以上の多パス加工の場合には加工の前
半あるいは多パスの最終パス以前に生成したフエ
ライトが引き続き加工を受ける結果、加工歪を回
復するため再結晶が起る場合がある。実際に1パ
スの加工を行つた後、1秒程度以下の短時間内に
次の加工を加えると、これら2パスの合計圧下率
が35%以上と大きい場合には加工中に再結晶核が
発生し、加工ほ前半の状態あるいは前パス加工後
次パス加工前の状態に比べてより細粒のフエライ
トが生ずる場合がある。このような場合において
もやはり加工直後の動的(加工中)に生成した再
結晶核と加工直後に連続して起る成長(準動的再
結晶)との区別は困難である。また、このような
動的および準動的再結晶現象が加わつた組織と前
述の動的および準動的変態のみの組織とは極めて
類似しており、両者を明確に区別するのは困難で
ある。従つて、本発明においてはこれらを総括し
て加工誘起フエライトと呼ぶことにした。
このような加工誘起フエライトは極めて微細で
あるとともに以下のような特徴を有する。
形態がほぼ等軸的であつて加工により著しい
延伸が見られないこと。
このことは本発明鋼(試番2)の典型的な光
学顕微鏡組織である第3図を見れば明らかであ
る。通常変態域で加工を行なうと圧延方向に延
伸した加工フエライト粒となるが、このような
組織は加工フエライト組織または動的回復組織
と呼ばれ、特殊な腐食液を用いて観察すれば亜
粒界(サブバウンダリー)という組織が観察さ
れるが、これは通常のフエライト粒界(大傾角
粒界)と異なり、粒間相互の方位に差が小さく
機械的性質に対する粒界の効果が全く異なるた
め、細粒による特性向上が殆んど見られないば
かりでなく、延伸により機械的性質が著しい異
方性を呈し、本発明鋼のようなすぐれた特性は
一般に得ることが難しい。
転位密度が平均して高く、一般に不均一であ
ること。
一般に冷却中に起る初析フエライト変態にお
いては、変態温度が600〜700℃と高いため、生
成したフエライト中に転位が極めて少いことが
特徴である。これに対し本発明鋼においては局
部的に転位密度の多い所と少い所があるが総合
的に見ればかなり高い転位密度を示している。
このような高い転位密度は変態温度の低い
(500℃程度以下)ベイナイトまたはマルテンサ
イトで観察されるもので、800℃附近で生成し
たと考えられる第3図の場合極めて異常であ
る。この理由は加工中に発生した動的変態また
は動的再結晶フエライトは、引き続き加工が加
わつて行くため加工の進行とともに転位密度が
増加するためである。このためフエライトの生
成の時期によつて転位密度の差が生じ、このよ
うな不均一な様相を呈するのである。
炭化物が細かくほぼ均一に分布すること。
第1図の本発明鋼の組織では炭素量が0.07%
で95%のフエライトが生成し、明確なパーライ
ト組織は見られていない。後述の試番10では
0.12%Cでは98%のフエライトが得られてい
る。平衡状態図から予測される最大フエライト
量は、この2つの鋼でそれぞれ91%および85%
であり、本発明鋼ではこれをはるかに超えてフ
エライトが生成している。
一方、このような光学顕微鏡組織では炭化物
を多量に含むパーライトやベイナイト組織、あ
るいは炭素を多量に固溶するマルテンサイト組
織は極めて少量しか見られない場合でも、電子
顕微鏡観察によると微細粒間の粒界またはその
中の転位密度の高い部分に微細な析出物(炭化
物)が観察される。このように炭化物は通常の
フエライトパーライト鋼等に比べると微細かつ
均一に析出している。
このような組織を生ずる理由は次の通りであ
る。
上述のように超細粒フエライトは通常の変態
点附近あるいはそれ以上で、しかもその温度で
は生成しないような多量に生成するが、これは
変態を促進するエネルギーが単に化学的なもの
ではなく、加工によつて供給されているためで
ある。また一方で圧延加工のような短い時間内
に多量のフエライトが生成することからわかる
ように、通常のフエライト変態と異なり、炭素
の拡散が追いつかない。(このような場合は炭
素の拡散で変態が起る場合に比べエネルギー的
に不利であるが、この不足分も加工により供給
されている。)このため炭素原子はフエライト
中に過飽和に固溶し、加工後室温まで冷却され
る過程において、マクロ的に見ればかなり均一
に分布するフエライト粒界あるいは高密度の転
移上に析出するものと考えられる。
以上および項に述べたような特徴は通常の
初析フエライトと著しく異なるものである。Cの
拡散がない点は純鉄等で見られる、いわゆるマツ
シブフエライト変態と同様であり、熱間加工中と
いう極めて短時間に変態が進行する点もこれと符
合している。そして転移密度が極めて高いのは、
これが生成と同時に加工を受けるためであり“加
工誘起マツシブフエライト”と呼ぶべき従来鋼の
組織とは全く異なる新しい組織を有する鋼が創成
されたものである。
本発明鋼は種々の熱間加工法で提供できる。た
とえば厚板圧延、ホツトストリツプ圧延、線材圧
延などであり、熱間押出あるいは熱間鍛造などの
圧延以外の加工法でも可能である。
次に本発明の効果について述べる。
前述のように細粒化すると強度靭性が向上する
ことはよく知られているが、これ迄4μm以下と
いう極細粒でその効果を調べた例はない。第4図
は本発明で得られた細粒鋼(黒丸)のデータを従
来鋼のデータとともに示したものである。従来の
データ(丸)はいわゆるPetchの関係式によりよ
く整理できるが、本発明による鋼はこの延長線か
らさらに向上する傾向を示している。そのほかに
も延性が良好であり、後述の実施例に見られるよ
うに同一強度でも比較の通常鋼に対し延性がすぐ
れ、すぐれた強度―延性バランスを示す。これは
上述のような組織的均一性が超微細粒化の効果と
重畳したものと考えられる。
以上の特性以外にも耐久性(疲労強度)、成形
加工性(穴拡げ性、プレス成形性)等の点でもす
ぐれた特性を示すことが観察されるが、これは皆
上述の組織の特徴に由来するものである。
また、とくに2〜3μm以下の超細粒鋼では
600℃以上で著しく延性が向上する超塑性現象を
示すなどの特徴のある特性を示す。
このように本発明鋼では従来鋼をはるかに上回
る特性を示すので本発明の効果はきわめて莫大
で、非常に低コストで合金元素等を添加せずに高
品質の高張力鋼等を容易に製造できるのである。
実施例 1
第1表に示す転炉溶製鋼、を200mmのスラ
ブに連続鋳造し、1100℃に加熱後ホツトストリツ
プミルで圧延して5mm厚の鋼板とした。鋼は特
殊な溶製技術を用いた。
粗圧延では200mmスラブを50mmまで7パスで圧
延し、仕上温度は900〜1000℃であつた。
仕上圧延のパススケジユールを第2表に示す。
A、Bは本発明によるもので、1秒以内に行われ
る5、6番目のパスで合計58%または44%の圧下
を行つた場合である。Cは比較の通常の圧延の例
で、最終2圧下の圧下は合計27%である。
以上の圧延条件の組合せと圧延された鋼板の機
械的性質を第3表に示す。試番2、6を除いては
圧延後の冷却は、ランアウトテーブル上で強力な
スプレイ冷却を行つた。
機械的性質から本発明の効果は明らかで60Kg/
mm2以上の強度を持ち、20%以上のすぐれた延性を
有している。
第3図にその組織写真の例(試番2)を示す
が、1〜3μmの細粒の等軸フエライト粒で殆ん
ど占められており、前述の本発明鋼の典型的な特
徴を示している。
一方比較材の試番4は圧下率が小さいため細粒
フエライトが生成せず焼きが入つて延性が不良で
ある。鋼の試番5は圧下率が本発明の要件を満
しているが不純物元素が多いためフエライトが動
的再結晶しないので十分な細粒化が起らず延性が
不良である。また試番6はフエライトの動的再結
晶が起らず伸長したフエライトとなり強度は高く
なるが延性はきわめて多くなる。
The present invention relates to ultra-fine-grained ferritic steel, especially ultra-fine-grained ferritic steel that is as hot-rolled and that does not contain special alloying elements such as Nb, Ta, Mo, and W, and its production. It is about the method. The fine-grained ferrite structure mentioned here is mostly
More than 70-80% consists of fine ferrite crystal grains,
Depending on the desired mechanical properties, in addition to the ferrite phase, one or more of other fine structures such as pearlite, martensite, retained austenite, etc. may be present, or carbide, nitride, etc. may be present. It may contain precipitates. The structure called fine-grained ferrite in the present invention is almost isotropic without significant elongation of the grain shape, and in principle refers to a structure consisting of crystal grains surrounded by so-called high-angle grain boundaries, and is subcrystalline. Grain boundary (low angle grain boundary)
are not considered as grain boundaries. However, there may be some increase in dislocation density and formation of subgrain boundaries inside such grains. Among the various strengthening methods for steel, grain refinement is known to be the only method to increase both strength and toughness, and is most often used to improve the quality of steel materials used as hot-rolled. This is an important technology that must be considered first in most cases. What has been achieved industrially with conventional grain refining technology is as small as 4
It is about 6 μm. This is usually carried out using a method called controlled rolling, which is a technique for strongly rolling steel containing alloying elements such as Nb at relatively low temperatures. In this case, Nb needs to be in solid solution as rolled, so heating is performed at a high temperature of 1200°C or higher before rolling to dissolve Nb, and then finish rolling is performed at a low temperature of 800°C or lower. This method has industrial disadvantages, such as waiting for the temperature of the steel plate to drop, resulting in a significant drop in production efficiency, and a significant increase in deformation resistance during rolling, resulting in a heavy load on the rolling mill. In addition, various methods have been proposed, such as heating and rolling in a low temperature range or forced cooling after rolling, but all of these methods remain within the above grain size range, and the ultrafine grains ( 3-4
μm or less) has not yet been obtained industrially. On the other hand, methods for experimentally obtaining ultrafine grain structures have recently been studied. For example, there is a method of repeatedly annealing Ni steel or the like several times before and after the transformation point.
However, it is clear that such heat treatment is difficult to implement industrially from an economic standpoint. The present invention relates to such an epoch-making ultra-fine-grained steel that can actually be obtained industrially, and in particular is a hypo-eutectoid steel whose main component is C without using any special alloying elements. It relates to steel that can be obtained as is, and in particular to an epoch-making technology that allows for easy production by reducing impurities such as P, S, and N. That is, the gist of the present invention is as follows. (1) C: 0.3% or less, Si: 1.5% or less, in weight%
Consisting of Mn: 2% or less, N: less than 0.002%, balance Fe and unavoidable impurities, the metal structure contains deformation-induced equiaxed ferrite crystal grains surrounded by large-angle grain boundaries with an average size of 4 μm or less at a volume fraction of 70%. Ultra-fine grained ferrite steel with high strength and excellent ductility. (2) C: 0.3% or less, Si: 1.5% or less, in weight%
Steel consisting of Mn: 2% or less, N: less than 0.002%, the balance Fe and unavoidable impurities is heated to a temperature above the Ac 3 transformation point, and then hot worked in the process of cooling. ℃〜
(Ar 3 + 100°C) temperature range, one or more times within 1 second with a total area reduction of 35% or more. Method for manufacturing fine-grained ferrite steel. The details of the present invention will be explained below. The steel of the present invention is an ultra-fine-grained ferrite steel as described above, but the structure called fine-grained ferrite in the present invention does not involve significant elongation of the grain shape and is almost isodirectional.
Furthermore, as a general rule, it refers to a structure consisting of crystal grains surrounded by so-called high-angle grain boundaries, and subgrain boundaries (low-angle grain boundaries) are not considered grain boundaries. The reason for specifying the chemical composition of steel in the present invention is as follows. The reason for setting the C content to 0.3% or less is that C
When the amount of C increases, the amount of ferrite decreases and the steel becomes mainly pearlite. However, in the steel of the present invention, the amount of ferrite can be increased much more than usual even with the same amount of C. However, if this amount is exceeded, the amount of pearlite etc. increases and it becomes difficult to obtain a steel mainly composed of ferrite. Si is usually added to steel for the purpose of deoxidizing and is contained to some extent, and in the present invention, it is sometimes added intentionally because it has the effect of increasing the amount of ferrite. However, if it is added in an amount exceeding 1.5%, the ferrite crystal grains tend to become coarse, so the content was set at 1.5% or less. Mn adjusts the transformation point, makes deformation-induced transformation more likely to occur, and also contributes to grain refinement by preventing rapid grain growth of deformation-induced ferrite.
If it is added in excess of 2%, the transformation temperature may drop too much and the ferrite amount may not reach 70%.
The following was made. P and S are elements that are normally contained in steel to some extent, but if they are contained in large amounts, they impair the ductility and toughness of steel. In the present invention, the smaller the amount, the more preferable. This is because deformation-induced transformation and recrystallization, which are the formation mechanisms of the steel of the present invention, are more likely to occur as P and S are reduced, and it is desirable that P and S be at most 0.015% and 0.010%, respectively. Although some amount of N is contained in steel as an impurity element, for the same reason as P and S mentioned above, the lower the content, the better the properties and the easier it is to obtain the steel of the present invention. If this amount exceeds 0.002%, it becomes difficult to produce the inventive steel unless hot working under large pressure, which is industrially quite difficult, is applied, especially in steels containing nitride-forming elements such as Al and Ti. So 0.002%
less than Al is usually contained to some extent in steel for deoxidization, but if it is normally contained at 0.1%, it generally does not have a large effect on the properties of the steel of the present invention. Further, Nb, Ta, Mo, W, etc. are all known as elements that delay the recrystallization and transformation of austenite. Since the steel of the present invention promotes transformation and recrystallization of austenite during hot working to make the grains finer, Nb, Ta, Mo, W, etc. are elements that inhibit this, so they are not included in the steel of the present invention. It must not be allowed to happen. Steel having such a composition is manufactured by the following manufacturing method. There are no particular restrictions on the steps leading to the final processing of the steel of the present invention. That is, normally produced molten steel may be made into a slab by continuous casting, or may be made into a slab by an ingot making-slaking process. The slab may be brought to the rolling process while still at high temperature, or
It may be reheated once cooled. It can be said that it is generally desirable that the heating and processing conditions for the slab be such that the austenite grain size of the slab becomes smaller just before the processing step of the present invention, but normal conditions may be used before the processing step of the present invention. Therefore, there are no restrictions. The feature of the manufacturing method of the present invention is that the steel is heated to 600°C
(Ar 3 +100°C), applying a large pressure for a short period of time. However, the Ar 3 transformation point here refers to the temperature at which the steel starts to transform into ferrite during slow cooling from the temperature range where it is austenite.
(hereinafter simply referred to as Ar 3 ) The present inventors conducted a detailed study on the effect of large reduction on the hot-worked structure, which had not been studied in the past, and discovered new knowledge that was completely unknown in the past. Obtained. The results are schematically shown in FIG. The region of small area reduction in this figure is relatively well known, and it has recently been known that austenite undergoes dynamic recrystallization at relatively high temperatures even under high pressure. By the way, when high-purity steel according to the present invention is used, transformation occurs during processing by applying a large reduction between Ar 3 +100°C and 600°C, and the fine-grained ferrite produced at this time is further regenerated during rolling. It was found that the particles crystallized and became even finer. The range of hot working conditions of the present invention is shown in Figures 1 and 2.
clearly shown in the diagram. That is, normal purity steel (P:
0.015-0.030%, S: 0.008-0.015%, N:
0.0025 to 0.0050%), the area reduction rate exceeds 50% in an appropriate temperature range. Dynamic transformation and recrystallization of ferrite occur to obtain an average ferrite grain size of 3 to 4 μm or less (Fig. 1 ferrite dynamic recrystallization region), but in the case of high purity steel according to the present invention, the area reduction rate is Similar fine grains can be obtained even at 35%, and at lower temperatures, the grain refinement becomes even more remarkable due to complete dynamic recrystallization of ferrite, resulting in ultrafine grains of 2 μm or less (Fig. 1 Ferrite dynamic recrystallization ). From this, it can be seen that purifying steel according to the present invention is extremely effective. Figure 2 shows the relationship between the cumulative area reduction rate (%) and the average ferrite grain size.In the case of the steel according to the present invention, the ferrite grain size shows that it becomes smaller. In this case, the processing temperature of the present invention is 650~
700℃, and 750-800℃ for comparative steel. Although it is best to apply this reduction in one pass as in thick plate rolling, we have found that cumulative strain applied in multiple passes over a short period of time can have almost the same effect as shown in Figure 2. Obtained. It has also been found that this short time may be within about 1 second in normal rolling. Therefore, the above rolling reduction rate can be replaced by the accumulated total area reduction rate. Incidentally, such a short-time cumulative reduction can actually be realized at the finishing stage of wire rod rolling or in the latter half of hot strip rolling, as shown in the upper part of FIG. It is desirable that the above hot working is carried out at the final stage of the overall working, but in some cases even a small amount of hot or cold deformation to adjust the shape of the rolled material may significantly impair its properties. isn't it. In order to suppress grain growth after processing, it is often desirable to cool at a high cooling rate. When the area reduction rate is sufficiently large or when the finishing temperature is on the low side within the appropriate temperature range, fine grains can be obtained even if the steel material cross section is small, even if it is allowed to cool. However, when the area reduction rate is close to the lower limit, When the cross section of the product steel material is large or the finishing temperature is high, accelerated cooling at a rate of 20°C/sec or more is often effective, for example. If the cooling rate is high and even a small amount of untransformed austenite remains, that part becomes a hard second phase, which has the effect of further improving the strength. As described above, depending on the purpose, accelerated cooling can improve the material quality, especially the strength. In this case, it goes without saying that the temperature range for accelerated cooling should include a temperature range of 500°C or higher, where ferrite grain growth or portions that are not transformed during rolling transform into ferrite or pearlite during cooling. be. The steel of the present invention is characterized by the formation of such fine-grained ferrite immediately after hot rolling, and for specific purposes (improving texture, etc.) It's possible. Next, the metallographic characteristics of the steel of the present invention produced in this manner will be explained. As mentioned above, the present invention is characterized in that when high-purity low-carbon steel is subjected to a reduction exceeding a certain limit in one pass or multiple passes at an appropriate temperature range, transformation is easily induced during processing, and the transformation is extremely fine. This is based on new knowledge that there is. At this time, the transformation nuclei generated during machining do not stop moving immediately after machining, and the machining strain (due to high-density dislocations induced by machining) does not recover immediately, so the boundary surface moves. Because the driving force is maintained to a certain extent, the fine-grained ferrite grows slightly after processing, and its volume fraction also increases. In such cases, it is difficult to experimentally strictly distinguish between the dynamically transformed ferrite part that has transformed during processing and the quasi-dynamic transformation point ferrite part that has grown following processing, and there is no practical need to do so. Therefore, the state up to a time period of about 1 second or less in the temperature range that becomes a problem after processing is defined as processing-induced transformation. In addition, in the case of high reduction machining even in one pass, and especially in the case of multi-pass machining of two or more passes, the ferrite generated in the first half of the machining or before the final pass of the multi-pass continues to undergo machining, and as a result, the machining distortion is recovered. Therefore, recrystallization may occur. In fact, after one pass is processed, if the next process is added within a short time of about 1 second or less, if the total reduction ratio of these two passes is as large as 35% or more, recrystallization nuclei will form during the process. This may result in finer grained ferrite compared to the state in the first half of processing or the state after the previous pass and before the next pass. Even in such a case, it is still difficult to distinguish between recrystallization nuclei that are dynamically generated immediately after processing (during processing) and growth that occurs continuously immediately after processing (quasi-dynamic recrystallization). Furthermore, the structure in which such dynamic and quasi-dynamic recrystallization phenomena are added is extremely similar to the structure in which only the dynamic and quasi-dynamic transformations are described above, and it is difficult to clearly distinguish between the two. . Therefore, in the present invention, these are collectively referred to as deformation-induced ferrite. Such processing-induced ferrite is extremely fine and has the following characteristics. The shape is approximately equiaxed and no significant stretching is observed during processing. This is clear from FIG. 3, which is a typical optical microscopic structure of the steel of the present invention (sample number 2). When processing is carried out in the normal transformation region, processed ferrite grains are formed that are stretched in the rolling direction. Such a structure is called a processed ferrite structure or a dynamic recovery structure, and when observed using a special corrosive solution, subgrain boundaries can be detected. A structure called (sub-boundary) is observed, but unlike normal ferrite grain boundaries (high-angle grain boundaries), there is little difference in the mutual orientation between grains, and the effect of grain boundaries on mechanical properties is completely different. Not only is there almost no improvement in properties due to fine grains, but the mechanical properties exhibit significant anisotropy due to stretching, and it is generally difficult to obtain excellent properties such as those of the steel of the present invention. Dislocation density is high on average and generally non-uniform. In the pro-eutectoid ferrite transformation that generally occurs during cooling, the transformation temperature is as high as 600 to 700°C, so it is characterized by extremely few dislocations in the produced ferrite. On the other hand, in the steel of the present invention, although there are some places where the dislocation density is high and some places where the dislocation density is low, overall it shows a considerably high dislocation density.
Such a high dislocation density is observed in bainite or martensite, which has a low transformation temperature (approximately 500°C or less), and is extremely abnormal in the case of Figure 3, which is thought to have been formed at around 800°C. The reason for this is that dynamic transformation or dynamic recrystallization of ferrite that occurs during processing continues to be processed, so that the dislocation density increases as processing progresses. For this reason, differences in dislocation density occur depending on the timing of ferrite formation, resulting in such a non-uniform appearance. Carbide particles are finely distributed and almost uniformly distributed. In the structure of the invention steel shown in Figure 1, the carbon content is 0.07%.
95% ferrite is produced, and no clear pearlite structure is observed. In trial number 10 described below
At 0.12% C, 98% ferrite was obtained. The maximum ferrite content predicted from the equilibrium phase diagram is 91% and 85% for these two steels, respectively.
In the steel of the present invention, ferrite is generated far more than this. On the other hand, even if only a very small amount of pearlite or bainite structure containing a large amount of carbide, or martensite structure containing a large amount of carbon as a solid solution is seen in such an optical microscopic structure, electron microscopic observation shows that the grains between fine grains are visible. Fine precipitates (carbides) are observed in the boundaries or in areas with high dislocation density. In this way, carbides are precipitated finer and more uniformly than in ordinary ferrite pearlite steel. The reason for the formation of such an organization is as follows. As mentioned above, ultrafine-grained ferrite is produced near or above the normal transformation point, and in large quantities that would not be produced at that temperature.This is because the energy that promotes transformation is not simply chemical, but processing. This is because it is supplied by. On the other hand, as can be seen from the fact that a large amount of ferrite is produced within a short period of time, such as during rolling, unlike normal ferrite transformation, carbon diffusion cannot keep up. (In such a case, it is disadvantageous in terms of energy compared to the case where transformation occurs due to carbon diffusion, but this shortage is also supplied through processing.) Therefore, carbon atoms are dissolved in supersaturated solid solution in ferrite. It is thought that during the process of cooling to room temperature after processing, precipitation occurs on ferrite grain boundaries or high-density dislocations that are fairly uniformly distributed from a macroscopic perspective. The characteristics described above and in the section above are significantly different from ordinary pro-eutectoid ferrite. The fact that there is no diffusion of C is similar to the so-called mushy ferrite transformation seen in pure iron, etc., and the fact that the transformation progresses in an extremely short period of time during hot working is also consistent with this. And the reason why the metastasis density is extremely high is
This is because the steel undergoes processing at the same time as it is formed, and a steel with a new structure completely different from that of conventional steel, which can be called "deformation-induced pine ferrite", has been created. The steel of the invention can be provided by various hot working methods. Examples include thick plate rolling, hot strip rolling, wire rod rolling, etc., and processing methods other than rolling such as hot extrusion or hot forging are also possible. Next, the effects of the present invention will be described. As mentioned above, it is well known that strength and toughness are improved by making the grains finer, but so far there has been no study of this effect using ultrafine grains of 4 μm or less. FIG. 4 shows the data for the fine-grained steel (black circles) obtained by the present invention together with the data for the conventional steel. Conventional data (circles) can be well organized by the so-called Petch relation, but the steel according to the present invention shows a tendency to further improve from this extension. In addition, it has good ductility, and as seen in the examples below, even at the same strength, it has superior ductility compared to conventional steel, showing an excellent strength-ductility balance. This is considered to be due to the combination of the above-mentioned structural uniformity and the effect of ultra-fine grain formation. In addition to the above properties, it has been observed that it also exhibits excellent properties in terms of durability (fatigue strength), formability (hole expandability, press formability), etc., but these are all due to the characteristics of the structure mentioned above. It is derived from In addition, especially in ultra-fine grain steel of 2 to 3 μm or less,
It exhibits distinctive properties such as a superplastic phenomenon in which ductility increases significantly at temperatures above 600℃. In this way, the steel of the present invention exhibits properties that far exceed those of conventional steel, so the effects of the present invention are extremely large, making it possible to easily produce high-quality, high-strength steel, etc. at a very low cost and without adding alloying elements. It can be done. Example 1 The converter melted steel shown in Table 1 was continuously cast into a 200 mm slab, heated to 1100°C, and then rolled in a hot strip mill to form a 5 mm thick steel plate. The steel was made using a special melting technique. In rough rolling, a 200 mm slab was rolled to 50 mm in 7 passes, and the finishing temperature was 900 to 1000°C. Table 2 shows the pass schedule for finish rolling.
A and B are according to the present invention, and are cases where a total reduction of 58% or 44% was performed in the 5th and 6th passes performed within 1 second. C is an example of normal rolling for comparison, and the total reduction in the final two reductions is 27%. Table 3 shows the combinations of the above rolling conditions and the mechanical properties of the rolled steel sheets. With the exception of trial numbers 2 and 6, cooling after rolling was performed by powerful spray cooling on a run-out table. The effect of the present invention is clear from the mechanical properties.
It has a strength of more than mm 2 and excellent ductility of more than 20%. Fig. 3 shows an example of the microstructure photograph (trial number 2), which is mostly occupied by fine equiaxed ferrite grains of 1 to 3 μm, showing the typical characteristics of the steel of the present invention described above. ing. On the other hand, in the comparative material Trial No. 4, since the reduction ratio was small, fine grained ferrite was not generated and quenching occurred, resulting in poor ductility. Steel trial No. 5 has a rolling reduction that satisfies the requirements of the present invention, but due to the large amount of impurity elements, the ferrite does not dynamically recrystallize, so sufficient grain refinement does not occur and the ductility is poor. In sample No. 6, dynamic recrystallization of ferrite does not occur, resulting in elongated ferrite, which has high strength but extremely high ductility.
【表】【table】
【表】【table】
【表】【table】
【表】
以上から本発明の効果が顕著であることが明ら
かである。[Table] From the above, it is clear that the effects of the present invention are remarkable.
第1図は0.07C―1Mn鋼の熱間加工時の歪量、
温度と加工直後の組織の関係を示す図、第2図は
0.07C―1Mn鋼の熱間加工時の歪量とフエライト
平均粒径の関係を示す図、第3図は本発明鋼の光
学顕微鏡による金属組織を示す写真図、第4図は
0.07―1Mn鋼のフエライト粒径と降伏応力、靭性
の関係を示す図である。
Figure 1 shows the amount of strain during hot working of 0.07C-1Mn steel.
Figure 2 shows the relationship between temperature and structure immediately after processing.
A diagram showing the relationship between the amount of strain during hot working and the average ferrite grain size of 0.07C-1Mn steel, Figure 3 is a photograph showing the metallographic structure of the invention steel taken with an optical microscope, and Figure 4 is
FIG. 2 is a diagram showing the relationship between ferrite grain size, yield stress, and toughness of 0.07-1Mn steel.
Claims (1)
Mn:2%以下、N:0.002%未満、残部Feおよび
不可避的不純物よりなり、その金属組織中に平均
4μm以下の大傾角粒界に囲まれた加工誘起等軸
フエライト結晶粒を体積率で70%以上含むことを
特徴とする高強度でしかも延性のすぐれた超細粒
フエライト鋼。 2 重量%でC:0.3%以下、Si:1.5%以下、
Mn:2%以下、N:0.002%未満、残部Feおよび
不可避的不純物からなる鋼をAc3変態点以上の温
度に加熱してから冷却する過程において熱間加工
を行い、その終段において、600℃〜(Ar3+100
℃)の温度域で1秒以内に1回または2回以上の
合計減面率が35%以上であるような加工を加える
ことを特徴とする高強度でしかも延性のすぐれた
超細粒フエライト鋼の製造方法。[Claims] 1% by weight: C: 0.3% or less, Si: 1.5% or less,
Consisting of Mn: 2% or less, N: less than 0.002%, balance Fe and unavoidable impurities, the metal structure contains deformation-induced equiaxed ferrite crystal grains surrounded by large-angle grain boundaries with an average size of 4 μm or less at a volume fraction of 70%. Ultra-fine grained ferrite steel with high strength and excellent ductility. 2 C: 0.3% or less, Si: 1.5% or less, in weight%
Steel consisting of Mn: 2% or less, N: less than 0.002%, the balance Fe and unavoidable impurities is heated to a temperature above the Ac 3 transformation point, and then hot worked in the process of cooling. ℃〜(Ar 3 +100
Ultra-fine grained ferrite steel with high strength and excellent ductility, characterized by being processed once or twice or more in a temperature range of 35% or more within 1 second in a temperature range of 35% or more. manufacturing method.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10299182A JPS58221258A (en) | 1982-06-17 | 1982-06-17 | Hyperfine-grained ferrite steel and its manufacture |
| US06/481,453 US4466842A (en) | 1982-04-03 | 1983-04-01 | Ferritic steel having ultra-fine grains and a method for producing the same |
| DE3312257A DE3312257A1 (en) | 1982-04-03 | 1983-04-05 | FERRITIC STEEL WITH ULTRAFINE GRAIN AND METHOD FOR THE PRODUCTION THEREOF |
| FR8305500A FR2524493B1 (en) | 1982-04-03 | 1983-04-05 | FERRITIC STEEL WITH ULTRA-FINE GRAINS AND PROCESS FOR PRODUCING THE SAME |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10299182A JPS58221258A (en) | 1982-06-17 | 1982-06-17 | Hyperfine-grained ferrite steel and its manufacture |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58221258A JPS58221258A (en) | 1983-12-22 |
| JPS6239229B2 true JPS6239229B2 (en) | 1987-08-21 |
Family
ID=14342163
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10299182A Granted JPS58221258A (en) | 1982-04-03 | 1982-06-17 | Hyperfine-grained ferrite steel and its manufacture |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58221258A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02302940A (en) * | 1989-05-17 | 1990-12-14 | Sanyo Electric Co Ltd | Optical head |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TW580519B (en) * | 1997-09-22 | 2004-03-21 | Nat Res Inst Metals | Super fine structure steel and manufacturing method thereof |
-
1982
- 1982-06-17 JP JP10299182A patent/JPS58221258A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02302940A (en) * | 1989-05-17 | 1990-12-14 | Sanyo Electric Co Ltd | Optical head |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58221258A (en) | 1983-12-22 |
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