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JPH0380848B2 - - Google Patents
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JPH0380848B2 - - Google Patents

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Publication number
JPH0380848B2
JPH0380848B2 JP8198985A JP8198985A JPH0380848B2 JP H0380848 B2 JPH0380848 B2 JP H0380848B2 JP 8198985 A JP8198985 A JP 8198985A JP 8198985 A JP8198985 A JP 8198985A JP H0380848 B2 JPH0380848 B2 JP H0380848B2
Authority
JP
Japan
Prior art keywords
transformation
cooling
temperature
steel
ferrite
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP8198985A
Other languages
Japanese (ja)
Other versions
JPS61243125A (en
Inventor
Masayoshi Suehiro
Hiroshi Yada
Giichi Matsumura
Toshihiko Aryoshi
Katsuhiro Kawashima
Masaaki Hatsuta
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nippon Steel Corp
Original Assignee
Nippon Steel Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP8198985A priority Critical patent/JPS61243125A/en
Publication of JPS61243125A publication Critical patent/JPS61243125A/en
Publication of JPH0380848B2 publication Critical patent/JPH0380848B2/ja
Granted legal-status Critical Current

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21DMODIFYING 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
    • C21D9/00Heat treatment, e.g. annealing, hardening, quenching or tempering, adapted for particular articles; Furnaces therefor
    • C21D9/52Heat treatment, e.g. annealing, hardening, quenching or tempering, adapted for particular articles; Furnaces therefor for wires; for strips ; for rods of unlimited length
    • C21D9/54Furnaces for treating strips or wire
    • C21D9/56Continuous furnaces for strip or wire
    • C21D9/573Continuous furnaces for strip or wire with cooling
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B21MECHANICAL METAL-WORKING WITHOUT ESSENTIALLY REMOVING MATERIAL; PUNCHING METAL
    • B21BROLLING OF METAL
    • B21B37/00Control devices or methods specially adapted for metal-rolling mills or the work produced thereby
    • B21B37/74Temperature control, e.g. by cooling or heating the rolls or the product
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B21MECHANICAL METAL-WORKING WITHOUT ESSENTIALLY REMOVING MATERIAL; PUNCHING METAL
    • B21BROLLING OF METAL
    • B21B45/00Devices for surface or other treatment of work, specially combined with or arranged in, or specially adapted for use in connection with, metal-rolling mills
    • B21B45/02Devices for surface or other treatment of work, specially combined with or arranged in, or specially adapted for use in connection with, metal-rolling mills for lubricating, cooling, or cleaning
    • B21B45/0203Cooling
    • B21B45/0209Cooling devices, e.g. using gaseous coolants
    • B21B45/0215Cooling devices, e.g. using gaseous coolants using liquid coolants, e.g. for sections, for tubes

Landscapes

  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Mechanical Engineering (AREA)
  • Physics & Mathematics (AREA)
  • Thermal Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Materials Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Heat Treatment Of Strip Materials And Filament Materials (AREA)
  • Control Of Heat Treatment Processes (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

(産業上の利用分野) この発明は冷却中の変態組織を制御することに
より目的とする材質の鋼材を得る方法に関するも
ので、とくに連続熱間圧延後の冷却制御に好適な
ものである。 (従来の技術) 変態で材質が決まる鋼材がどのような変態組織
を持つかはその鋼の成分および種々の製造条件
(熱延鋼材の場合にはスラブ加熱温度、圧延条件、
冷却条件等)により大きく変化するが、その中で
もとくに冷却条件の影響が大きく、その制御が材
質の調整には重要である。 熱延工程では冷却条件の制御法として圧延最終
段の出側温度とコイル巻取温度を管理する方法が
とられているが、その冷却条件の設定には次のよ
うな2種類の方法が用いられている。ひとつは
CCT図やTTT図を用い、目的とする変態組織を
得るための冷却パターンを設定する方法である。
しかし実際の冷却は直線冷却に対応するCCT図
や恒温保定に対応するTTT図のような単純な温
度変化をとるのではなく、より複雑な温度変化
(とくに変態発熱による冷却曲線の変化)をとる
ため、この方法による冷却条件の正確な設定は不
可能である。他の方法は特公昭58−2246号公報や
特開昭56−119741号公報にみられるように、冷却
中の変態進行予測モデルを作成し、目的とする材
質を得るための最適冷却パターンを求める方法で
ある。 (発明が解決しようとする問題点) 以上のような方法は冷却条件のプリセツトによ
る制御法であり、冷却途中での実際の変態量がわ
からないためフイードバツク、フイードフオワー
ドによる制御は困難である。従つて、冷却条件が
設定した条件から変動した場合、目的とする組織
を得ることができなくなる。また、冷却前の製造
条件(スラブ加熱温度、圧延条件)も変態前のオ
ーステナイト組織の変化を介して最終の変態組織
に影響を与えるが、この冷却前の製造条件が変動
した場合にもやはり目的とする組織を得ることが
できなくなる。 本発明はこれらの製造条件の変動による冷却中
の変態進行の変化を冷却ゾーン途中に設定した変
態量計で実測し、これをもとにその後の冷却条件
を修正し、最終の材質を一定に保つ目的でなされ
たものである。 (問題点を解決するための手段、作用) 本発明の要旨は、連続熱間圧延後の鋼材の冷却
を制御する際に、冷却途中の前記鋼材の変態開始
後に、該鋼材の温度と変態量を実測するステツプ
と、この実測値を用いて、下記式(1)〜(3)よりその
後の鋼材の変態の進行を予測するステツプと、予
測される最終的な組織と目標の材質の組織とを比
較するステツプと、この比較結果に基づいて冷却
条件を補正するステツプとから成ることを特徴と
する鋼材の冷却制御方法である。 dx/dt=α(1−X) ……(1) α=A・1/Dγ・GR・(1n1/1−X)2/3 ……(2) α=B・1/Dγ・GRP ……(3) ただし、フエライト変態、ベイナイト変態に対
しては(2)式のαを、パーライト変態に対しては(3)
式のαを(1)に代入し、式中、 X:冷却途中での鋼材の変態量測定値 α:鋼材の成分、初期オーステナイト粒径、冷却
途中での変態量実測値および温度実測値で決ま
る関数 Dγ:変態前のγの粒径 GR:フエライトおよびベイナイトの成長速度 GRP:パーライトの成長速度 A、B:定数 である。 本発明者等は基礎的な加熱(オーステナイト
化)−冷却実験および実際の現場実験を重ねた結
果、一般に鋼材を冷却した場合、通常の拡散によ
る変態速度dX/dtは一般にその時の変態率Xに
より dX/dt=α(1−X) ……(1) と表わされることを見出した。ここでαは成分、
変態前のオーステナイト組織、およびXによつて
決まる関数である。 この式には時間が入つていないので、それまで
の冷却や変態の経過がどのようであつてもそれに
関係なくその時の変態速度を予測できる。また、
αは変態の種類により、具体的にはフアライト変
態、ベイナイト変態に対しては(2)式のように、パ
ーライト変態に対しては(3)式のように記述するこ
とができる。 α=A・1/Dγ・GR・(1n1/1−X)2/3 ……(2) α=B・1/Dγ・GRP ……(3) ただし、Xは変態率、Dγは変態前のγの粒径、
GRはフエライトおよびベイナイトの成長速度、
GRPはパーライトの成長速度である。またA、B
は実測から求まる定数で、等温変曲線または等速
冷却曲線から求めることができる。ここでXは実
測から求まる値であり、Dγは変態前のオーステ
ナイト粒径であり、鉄と鋼70(1984)、P2112で示
されるように熱間圧延条件をもとに加工後の回
復、再結晶の進行を計算することで求まる値であ
る。またGR、GRPは試料成分および湿度から求
まる値であり、ここでは(4)、(5)式(C.Zener:
Trans.AIME,167(1946)、P.550およびM.
Hillert:Jernkonl.Ann.,141(1957)、P.757)を
用い求める。 GR=1/r・Cγα−Cγ/Cγ−Cα・exp(−Q0/T)
……(4) GRP=(TA1−T)・(Cγα −Cγβ)・exp(−Q0/T) ……(5) ただし、Q0は定数であり、Tはランアウトテ
ーブル上での鋼材温度、TA1は鋼材の成分によ
つて決まるA1変態温度である。Cγα、Cα、Cγβ、
rは鋼材の成分、温度をもとに通常の熱力学的計
算を行うことによつて求まる値であり、成長速度
を規定するそれぞれの相の界面での炭素量(炭素
以外の添加元素により変化する炭素量)に相当す
る。またCγは鋼材の添加炭素量から(6)式により
計算される値である。 Cγ=(Co−XFCα)/(1−XF) ……(6) ここでCoは添加炭素量、XFはフエライトへ変
態した分率である。 一般に亜共析鋼を高温のオーステナイト状態か
ら冷却すると最初にフエライトへ変態し、その後
未変態のオーステナイトはパーライト、ベイナイ
トあるいはマルテンサイトへと変態する。上記の
冷却過程での変態の様子を、一例として、横軸に
鋼材の温度を取り、たて軸に鋼材の変態率を取つ
て、第3図に示す。図中Bs、Msは後述するベイ
ナイト変態開始温度(Bs)、マルテンサイト変態
温度(Ms)である。 この時の変態の進行を次のように計算する。 冷却中の温度変化は階段状に分割し、微少時間
Δtの間の恒温保持の集まりと考える。フエライ
ト変態の開始は熱力学データより決まるAe3温度
と考え、冷却途中の温度がAe3温度に達したとこ
ろで変態進行の計算を開始する。その後の変態進
行は微少時間Δtでの変態量をdx/dt・Δtとして
(1)式を用い求め、変態開始からの累積により求め
る。この時まず最初にフエライト変態進行を(1)、
(2)、(4)式を用い計算するが、この時変態進行に伴
う未変態オーステナイト中への固溶炭素の濃縮を
考え、未変態オーステナイト中の平均固溶炭素量
を(6)式を用い計算し、この固溶炭素量が成分と温
度をもとに熱力学的計算から求まる臨界値に達し
た時にパーライト変態が開始すると考える。その
後の変態進行は(1)、(3)、(5)式を用いフエライト変
態の場合と同様微少時間Δtの変態進行量を、
dx/dt・Δtにより求め累積することにより計算
する。ベイナイト変態は冷却途中の温度が(7)式か
ら求まる成分によつて決まるベイナイト変態開始
温度Bsに達した時に開始し、その後の変態進行
は(1)、(2)、(4)式を用いフエライト変態と同様の手
続で計算する。 Bs(℃)=727.5−425[wt%C] −42.5[wt%Mn] ……(7) ここで[wt%C]は添加炭素量であり[wt%
Mn]は添加Mn量である。 マルテンサイト変態に関しては、冷却途中の温
度が成分によつて決まるマルテンサイト変態温度
(Ms)、に達した時残つている未変態オーステナ
イトがすべてマルテンサイトに変態するとして求
める。 本法においては最終の組織制御を行うが、その
狙いは最終の鋼材強度(TS)を制御することに
あるため、組織と鋼材強度とを対応付けることが
必要となる。そのために、本法では次式を用い
る。 TS=k1{fF・(HF+k2-1/2) +fP・HP+fB・HB+fM・HM} ……(8) ここでk1、k2は鋼種により決まる定数で、fは
各相の比率で上述の計算から求まる値、Hは各相
の強度である。ただしF、P、B、Mはそれぞれ
フエライト、パーライト、ベイナイトおよびマル
テンサイトを表す。またDαは冷却後のフエライ
ト粒径を示すがこの値は次式から求まる。 Dα={5.51×1010・Dγ1.75・ exp(−21430/T5)・fF1/3 ……(9) ここでDγは変態前のオーステナイト粒径であ
り、前述したようにたとえば鉄と鋼70(1984)、
P2112で示されるような方法で求まる値である。 T5は、前述の変態進行の計算において変態率
が最終のフエライト粒径を決定するフエライトの
核の生成が完了していると考えられる5%にした
時の温度でありfFはフエライト変態率である。 本予測法の基本となる変態予測式は、ある時刻
での変態進行速度を冷却開始からの時間を含まな
い関数、言いかえれば成分、温度および変態率の
関数としているため、冷却途中(変態途中)での
温度・変態率を実測することによりその後の変態
進行を容易に予測できる。 本発明は以上の画期的な発見に基づいたもの
で、変態途中での温度・変態率を実測することに
よりそれまでの種々の製造条件の変動による予測
とのずれをその後の冷却条件で補い、最終の材質
のばらつきを極力おさえることを可能ならしめた
ものである。 本発明の具体的な例を連続熱間圧延ミルに関し
て以上説明する。 第1図に全体のシステムを示す。鋼材の成分お
よび仕上圧延後のオーステナイト粒径から希望す
る材質に相当する組織を得るための冷却パターン
を前述の予測法であらかじめ求めておき、この温
度パターンが得られるように冷却条件を設定する
(→→)。次に冷却ゾーン途中に設置した温
度計および変態率計により温度、変態率を測定す
る。この実測の温度および変態率が予測していた
温度、変態率と相違なければ、最初に設定した冷
却条件通りその後の冷却を行う。実測の温度、変
態率が予測の温度、変態率と異なる場合は、実測
の温度、変態率をもとに、式(1)を用い希望する材
質に相当する組織比率またはフアライト粒径を得
るための冷却条件を再度求め、冷却条件を変更す
る(→→)。 変態量計としては種々の方式が考えられるが、
例えば透過渦流法によるものを用いて板厚10mm程
度以上の鋼板の変態量をオンラインで測定するこ
とが可能である。この方法は鋼の磁気的性質の変
化を感知することにより変態量を測定するもので
ある。装置は発振用のコイルおよび受信用のセン
サーからなり、この2種の装置で鋼板をはさむよ
うな形で設置する。この装置の特徴としては鋼材
通板時のばたつきに強い、鋼板が冷却水でぬれて
いてもよい、装置自体が簡単なものであるなどが
あげられる。この方法では測定は鉄のキユーリー
点(約770℃)以下でしか行えないので、鋼材が
この温度以下になるような位置に変態量計を設置
するのがよい。連続熱延の場合にはランアウトテ
ーブル(ROT)の中間程度に設置するのが良い。
この位置には通常、温度計が設置されており、本
発明法を適用するのには透過渦流法の変態量計は
最適である。 (実施例) 第1表に示す成分の鋼について本発明法を適用
した、引張強さ55Kg/mm2の熱間圧延鋼板を製造し
た実施例を、従来法を適用した場合と比較して説
明する。 式(1)〜(7)を用い、種々の冷却パターンにおける
組織および材質を計算することから、上記の材質
を得る条件としてプリセツトした最終組織はフエ
ライト率80%、パーライト率17%、ベイナイト率
3%、フエライト粒径10μmであつた。また圧延
条件のプリセツト値は、最終圧延出側温度870℃、
ランアウトテーブル途中での変態率70%、ランア
ウトテーブル途中での温度670℃、取巻時の温度
600℃であつた。第2表に現場実験を行つた結果
を示すが、この表から明らかなように本発明法に
より最終材質のばらつきが従来法を適用した場合
よりも大きく減少する。 このときの本法および従来法による組織と特性
の変動の例を第2図に示す。第2図aはプリセツ
トした条件で圧延・冷却が行われていた部分の例
で、予定の材質となつている。同図bは従来法の
例で、圧延Top部に相当する。この部分では圧延
速度が遅く、最終圧延出側温度が高くなつていた
ため、オーステナイト粒径が大きくなり、その後
の冷却により最終組織のフエライト量が少なくな
つており、その結果強度が高くなつている。これ
に対し本法を適用した例では、冷却ゾーン中間に
設置した温度計および変態量計で温度、変態量を
実測し、この時点までの実測値をすべて総合し、
それ以後の冷却条件がプリセツトのまま進行した
場合の最終組織を(1)〜(7)式を用い計算し、プリセ
ツトの組織と比較する。この場合、Top部の最終
組織の予測値はフエライト率61%、パーライト率
0%、ベイナイト率39%、フエライト粒径8μm
であり、プリセツトの値と大きく異なつており、
その差を補正するため、温度および変態量を実測
した時点からの冷却条件(冷却速度、巻取温度)
を変えて冷却した場合の最終組織を(1)〜(7)式を用
い計算し、プリセツトの最終組織と近い最終組織
を与える冷却条件を選び、この冷却条件を与える
ように水量を調節したため(冷速の減少と巻取温
度の上昇)、圧延Top部で第2図cのような希望
する組織となり、その結果材質は希望する鋼材強
度となつた。
(Industrial Application Field) The present invention relates to a method for obtaining a steel material of a desired quality by controlling the transformed structure during cooling, and is particularly suitable for cooling control after continuous hot rolling. (Prior art) The type of transformation structure of a steel whose material quality is determined by transformation depends on the composition of the steel and various manufacturing conditions (in the case of hot-rolled steel, slab heating temperature, rolling conditions,
Among them, the influence of cooling conditions is particularly large, and its control is important for adjusting the material quality. In the hot rolling process, the cooling conditions are controlled by controlling the exit temperature of the final rolling stage and the coil winding temperature, but the following two methods are used to set the cooling conditions. It is being one is
This method uses CCT diagrams and TTT diagrams to set a cooling pattern to obtain the desired transformed structure.
However, actual cooling does not take simple temperature changes such as the CCT diagram corresponding to linear cooling or the TTT diagram corresponding to constant temperature maintenance, but more complex temperature changes (especially changes in the cooling curve due to transformation heat generation). Therefore, it is impossible to accurately set cooling conditions using this method. Another method, as seen in Japanese Patent Publication No. 58-2246 and Japanese Patent Application Laid-Open No. 56-119741, is to create a model to predict the progression of transformation during cooling and find the optimal cooling pattern to obtain the desired material quality. It's a method. (Problems to be Solved by the Invention) The method described above is a control method by presetting cooling conditions, and since the actual amount of transformation during cooling is not known, it is difficult to control by feedback or feedback. Therefore, if the cooling conditions vary from the set conditions, it becomes impossible to obtain the desired tissue. In addition, the manufacturing conditions before cooling (slab heating temperature, rolling conditions) also affect the final transformed structure through changes in the austenite structure before transformation, but even if the manufacturing conditions before cooling change, the objective It will not be possible to obtain the desired organization. In the present invention, changes in the progress of transformation during cooling due to variations in manufacturing conditions are actually measured using a transformation amount meter set in the middle of the cooling zone, and based on this, subsequent cooling conditions are corrected to maintain a constant final material quality. This was done for the purpose of preserving. (Means and effects for solving the problem) The gist of the present invention is to control the temperature and amount of transformation of the steel material after the start of transformation of the steel material during cooling, when controlling the cooling of the steel material after continuous hot rolling. a step of actually measuring the actual value, a step of predicting the subsequent progress of transformation of the steel material using the following formulas (1) to (3), and a step of predicting the predicted final structure and the target material structure. This is a steel cooling control method characterized by comprising a step of comparing the cooling conditions, and a step of correcting the cooling conditions based on the comparison results. dx/dt=α(1-X) ……(1) α=A・1/Dγ・GR・(1n1/1−X) 2/3 ……(2) α=B・1/Dγ・GR P ...(3) However, α in equation (2) for ferrite transformation and bainite transformation, and (3) for pearlite transformation.
Substituting α in the formula into (1), where: X: Measured amount of transformation of the steel material during cooling α: Composition of steel material, initial austenite grain size, actual measured value of transformation amount during cooling, and actual measured value of temperature Determining function Dγ: Grain size of γ before transformation GR: Growth rate of ferrite and bainite GR P : Growth rate of pearlite A, B: Constant. As a result of repeated basic heating (austenitization)-cooling experiments and actual field experiments, the present inventors found that when a steel material is cooled, the transformation rate dX/dt due to normal diffusion generally depends on the transformation rate X at that time. We found that it is expressed as dX/dt=α(1-X)...(1). Here α is the component,
This is a function determined by the austenite structure before transformation and X. Since this equation does not include time, the transformation rate at that time can be predicted regardless of the progress of cooling or transformation up to that point. Also,
α depends on the type of transformation; specifically, it can be described as equation (2) for phallite transformation and bainite transformation, and as equation (3) for pearlite transformation. α=A・1/Dγ・GR・(1n1/1−X) 2/3 ……(2) α=B・1/Dγ・GR P ……(3) However, X is the metamorphosis rate and Dγ is the metamorphosis The particle size of the previous γ,
GR is the growth rate of ferrite and bainite;
GR P is the growth rate of pearlite. Also A, B
is a constant determined from actual measurements, and can be determined from an isothermal curve or a constant velocity cooling curve. Here, X is a value obtained from actual measurements, and Dγ is the austenite grain size before transformation. This value is determined by calculating the progress of crystallization. In addition, GR and GR P are values determined from the sample components and humidity, and here they are expressed by equations (4) and (5) (C. Zener:
Trans.AIME, 167 (1946), P.550 and M.
Hillert: Jernkonl. Ann., 141 (1957), p. 757). GR=1/r・Cγα−Cγ/Cγ−Cα・exp(−Q 0 /T)
...(4) GR P = (TA 1 −T)・(Cγα −Cγβ)・exp(−Q 0 /T) ...(5) However, Q 0 is a constant, and T is the value on the runout table. The steel temperature, TA 1 , is the A 1 transformation temperature, which is determined by the composition of the steel. Cγα, Cα, Cγβ,
r is a value determined by ordinary thermodynamic calculations based on the composition and temperature of the steel material, and the amount of carbon at the interface of each phase that determines the growth rate (varies depending on added elements other than carbon). carbon content). Furthermore, Cγ is a value calculated from the amount of added carbon in the steel material using equation (6). Cγ=(Co−X F Cα)/(1−X F ) (6) where Co is the amount of added carbon and X F is the fraction transformed to ferrite. Generally, when hypoeutectoid steel is cooled from a high-temperature austenite state, it first transforms into ferrite, and then untransformed austenite transforms into pearlite, bainite, or martensite. The state of transformation during the above cooling process is shown as an example in FIG. 3, with the horizontal axis representing the temperature of the steel material and the vertical axis representing the transformation rate of the steel material. In the figure, Bs and Ms are the bainite transformation start temperature (Bs) and martensitic transformation temperature (Ms), which will be described later. The progress of metamorphosis at this time is calculated as follows. The temperature change during cooling is divided into steps and considered as a collection of constant temperature maintenance during a minute time Δt. The start of ferrite transformation is considered to be the Ae 3 temperature determined from thermodynamic data, and the calculation of the transformation progress is started when the temperature during cooling reaches the Ae 3 temperature. The subsequent metamorphosis progress is expressed as the amount of metamorphosis in a minute time Δt as dx/dt・Δt
It is calculated using equation (1) and calculated from the accumulation from the start of metamorphosis. At this time, first of all, the ferrite metamorphosis progresses (1),
Calculations are made using equations (2) and (4), but considering the concentration of solid solute carbon in untransformed austenite as the transformation progresses, the average amount of solid solute carbon in untransformed austenite is calculated using equation (6). It is considered that pearlite transformation begins when the amount of solid solute carbon reaches a critical value determined from thermodynamic calculations based on the components and temperature. For the subsequent transformation progress, use equations (1), (3), and (5) to calculate the amount of transformation progress in a minute time Δt, as in the case of ferrite transformation.
Calculated by finding and accumulating dx/dt・Δt. Bainite transformation starts when the temperature during cooling reaches the bainite transformation start temperature Bs determined by the components determined from equation (7), and the subsequent transformation progress is determined using equations (1), (2), and (4). Calculate using the same procedure as ferrite metamorphosis. Bs (℃) = 727.5-425 [wt%C] -42.5[wt%Mn] ...(7) Here, [wt%C] is the amount of added carbon, [wt%
Mn] is the amount of added Mn. Regarding martensitic transformation, it is calculated assuming that all remaining untransformed austenite transforms into martensite when the temperature during cooling reaches the martensitic transformation temperature (Ms) determined by the components. In this method, final structure control is performed, but since the aim is to control the final steel strength (TS), it is necessary to correlate the structure and steel strength. For this purpose, the following equation is used in this method. TS=k 1 {f F・(H F +k 2-1/2 ) +f P・H P +f B・H B +f M・H M } ...(8) Here, k 1 and k 2 depend on the steel type. is a determined constant, f is the ratio of each phase and is a value obtained from the above calculation, and H is the intensity of each phase. However, F, P, B, and M represent ferrite, pearlite, bainite, and martensite, respectively. Further, Dα indicates the ferrite grain size after cooling, and this value can be found from the following equation. Dα={5.51×10 10・Dγ 1.75・exp(−21430/T 5 )・f F } 1/3 …(9) Here, Dγ is the austenite grain size before transformation, and as mentioned above, for example, iron and Steel 70 (1984),
This is a value determined by the method shown in P2112. T 5 is the temperature at which the transformation rate is considered to have completed the generation of ferrite nuclei, which determines the final ferrite particle size in the calculation of the transformation progress described above, and f F is the ferrite transformation rate. It is. The transformation prediction formula that is the basis of this prediction method uses the transformation rate at a certain time as a function that does not include the time from the start of cooling, in other words, as a function of the components, temperature, and transformation rate. ) The subsequent progress of transformation can be easily predicted by actually measuring the temperature and transformation rate. The present invention is based on the above groundbreaking discovery, and by actually measuring the temperature and transformation rate during transformation, it is possible to compensate for deviations from predictions due to variations in various manufacturing conditions by adjusting subsequent cooling conditions. This makes it possible to suppress variations in the final material as much as possible. A specific example of the invention is described above with respect to a continuous hot rolling mill. Figure 1 shows the entire system. A cooling pattern to obtain a structure corresponding to the desired material quality is determined in advance from the composition of the steel material and the austenite grain size after finish rolling using the above-mentioned prediction method, and the cooling conditions are set to obtain this temperature pattern ( →→). Next, the temperature and transformation rate are measured using a thermometer and a transformation rate meter installed in the middle of the cooling zone. If the measured temperature and transformation rate are not different from the predicted temperature and transformation rate, subsequent cooling is performed according to the initially set cooling conditions. If the measured temperature and transformation rate are different from the predicted temperature and transformation rate, use formula (1) based on the measured temperature and transformation rate to obtain the structure ratio or phallite grain size corresponding to the desired material. Find the cooling conditions again and change the cooling conditions (→→). Various methods can be considered as a metamorphosis meter, but
For example, it is possible to measure the amount of transformation of a steel plate with a thickness of approximately 10 mm or more online using a transmission eddy current method. This method measures the amount of transformation by sensing changes in the magnetic properties of steel. The device consists of an oscillating coil and a receiving sensor, and is installed with a steel plate sandwiched between the two devices. The features of this device include that it is resistant to flapping when steel material is threaded, that the steel sheet can be wet with cooling water, and that the device itself is simple. With this method, measurements can only be made at temperatures below the Curie point of iron (approximately 770°C), so it is best to install the transformation meter at a location where the temperature of the steel material is below this temperature. In the case of continuous hot rolling, it is best to install it somewhere in the middle of the run-out table (ROT).
A thermometer is usually installed at this position, and a transformation meter using the transmission eddy current method is most suitable for applying the method of the present invention. (Example) An example of manufacturing a hot rolled steel plate with a tensile strength of 55 Kg/mm 2 by applying the method of the present invention to steel having the components shown in Table 1 will be explained in comparison with a case where a conventional method was applied. do. Using equations (1) to (7) to calculate the structure and material properties in various cooling patterns, the final structure preset as the conditions for obtaining the above material has a ferrite percentage of 80%, a pearlite percentage of 17%, and a bainite percentage of 3. %, and the ferrite particle size was 10 μm. In addition, the preset values of the rolling conditions are the final rolling exit temperature of 870℃,
Metamorphosis rate 70% in the middle of the runout table, temperature 670℃ in the middle of the runout table, temperature at the time of surrounding
It was 600℃. Table 2 shows the results of field experiments, and as is clear from this table, the method of the present invention reduces the variation in final material properties to a greater extent than when the conventional method is applied. FIG. 2 shows examples of changes in structure and properties according to the present method and the conventional method. FIG. 2a shows an example of a part that has been rolled and cooled under preset conditions, and the material is the same as planned. Figure b shows an example of the conventional method and corresponds to the top part of the rolling process. In this part, the rolling speed was low and the final rolling exit temperature was high, so the austenite grain size became large, and the amount of ferrite in the final structure decreased due to subsequent cooling, resulting in high strength. In contrast, in an example where this method is applied, the temperature and transformation amount are actually measured using a thermometer and transformation amount meter installed in the middle of the cooling zone, and all the actual measurements up to this point are combined.
The final structure when the subsequent cooling conditions proceed under the preset conditions is calculated using equations (1) to (7) and compared with the preset structure. In this case, the predicted final structure of the Top part is 61% ferrite, 0% pearlite, 39% bainite, and 8 μm ferrite grain size.
, which is significantly different from the preset value,
In order to correct the difference, cooling conditions (cooling rate, coiling temperature) from the time when the temperature and transformation amount were actually measured.
We calculated the final structure when cooling with different conditions using equations (1) to (7), selected cooling conditions that gave a final structure close to the preset final structure, and adjusted the amount of water to give this cooling condition ( (decrease in cooling rate and increase in coiling temperature), the desired structure as shown in Fig. 2c was obtained at the top part of the rolling process, and as a result, the material had the desired steel strength.

【表】【table】

【表】 (発明の効果) 本発明は冷却途中の変態組織を制御しつつ冷却
を行うことができるので、目的とする材質の鋼材
が適格に得られ、その工業的効果は甚大である。
[Table] (Effects of the Invention) Since the present invention can perform cooling while controlling the transformed structure during cooling, a steel material of the desired quality can be properly obtained, and its industrial effects are enormous.

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

第1図は本発明法の全体のシステム例を示す
図、第2図は本発明法および従来法による組織を
示す写真、第3図は冷却過程での鋼材の変態の様
子の一例を示すグラフである。
Figure 1 is a diagram showing an example of the entire system of the method of the present invention, Figure 2 is a photograph showing the structures of the method of the present invention and the conventional method, and Figure 3 is a graph showing an example of the transformation of steel during the cooling process. It is.

【特許請求の範囲】[Claims]

1 鉄鉱石、副原料、雑原料および燃料からなる
粉状の焼結原料に水を添加して混合造粒し、これ
を焼結機に装填して焼結鉱を製造するにさいし、 各粉状物質のそれぞれの飽和水分値Wiを予め
求めておき、この各飽和水分値Wiと各粉状物質
の配合割合Miとから焼結原料の飽和水分値の加
重平均(ΣWi×Mi)を算出し、この算出された
加重平均飽和水分値の50±2%の量の水を該焼結
原料に含有させて造粒することを特徴とする焼結
鉱の製造法。
1. When producing sintered ore by adding water to powdered sintering raw materials consisting of iron ore, auxiliary raw materials, miscellaneous raw materials, and fuel, and loading this into a sintering machine to produce sintered ore, each powder The saturated moisture value Wi of each powdery substance is determined in advance, and the weighted average (ΣWi×Mi) of the saturated moisture value of the sintering raw material is calculated from each saturated moisture value Wi and the blending ratio Mi of each powdery substance. A method for producing sintered ore, characterized in that the sintered raw material contains water in an amount of 50±2% of the calculated weighted average saturated moisture value and is granulated.

Claims (1)

ただし、フエライト変態、ベイナイト変態に対
しては(2)式のαを、パーライト変態に対しては(3)
式のαを(1)に代入し、式中、 X:冷却途中での鋼材の変態量実測値 α:鋼材の成分、初期オーステナイト粒径、冷却
途中での変態量実測値および温度実測値で決ま
る関数 Dγ:変態前のγの粒径 GR:フエライトおよびベイナイトの成長速度 GRP:パーライトの成長速度 A、B:定数 である。
However, α in equation (2) is used for ferrite transformation and bainite transformation, and (3) is used for pearlite transformation.
Substituting α in the formula into (1), where Determining function Dγ: Grain size of γ before transformation GR: Growth rate of ferrite and bainite GR P : Growth rate of pearlite A, B: Constant.
JP8198985A 1985-04-17 1985-04-17 Cooling method for steel products Granted JPS61243125A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8198985A JPS61243125A (en) 1985-04-17 1985-04-17 Cooling method for steel products

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8198985A JPS61243125A (en) 1985-04-17 1985-04-17 Cooling method for steel products

Publications (2)

Publication Number Publication Date
JPS61243125A JPS61243125A (en) 1986-10-29
JPH0380848B2 true JPH0380848B2 (en) 1991-12-26

Family

ID=13761881

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8198985A Granted JPS61243125A (en) 1985-04-17 1985-04-17 Cooling method for steel products

Country Status (1)

Country Link
JP (1) JPS61243125A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE19943403A1 (en) * 1999-09-10 2001-03-22 Siemens Ag Method and device for cooling a hot-rolled steel strip emerging from a roll stand
JP4529517B2 (en) * 2003-06-27 2010-08-25 Jfeスチール株式会社 High carbon steel plate manufacturing method and manufacturing equipment
JP4402502B2 (en) * 2004-04-13 2010-01-20 東芝三菱電機産業システム株式会社 Winding temperature controller
JP2015205331A (en) * 2014-04-23 2015-11-19 株式会社日立製作所 Control device and control method for hot rolling mill

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