JPS6056210B2 - Steel transformation structure control method - Google Patents
Steel transformation structure control methodInfo
- Publication number
- JPS6056210B2 JPS6056210B2 JP2346980A JP2346980A JPS6056210B2 JP S6056210 B2 JPS6056210 B2 JP S6056210B2 JP 2346980 A JP2346980 A JP 2346980A JP 2346980 A JP2346980 A JP 2346980A JP S6056210 B2 JPS6056210 B2 JP S6056210B2
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- Prior art keywords
- transformation
- cooling
- temperature
- steel
- heat
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Classifications
-
- C—CHEMISTRY; METALLURGY
- C21—METALLURGY OF IRON
- C21D—MODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
- C21D11/00—Process control or regulation for heat treatments
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- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Thermal Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- Mechanical Engineering (AREA)
- Materials Engineering (AREA)
- Metallurgy (AREA)
- Organic Chemistry (AREA)
- Control Of Heat Treatment Processes (AREA)
- Heat Treatment Of Strip Materials And Filament Materials (AREA)
Description
【発明の詳細な説明】
周知のように一般に鋼材の材質は鋼材の化学成分と高温
(オーステナイト状態)から冷却中に生成するフェライ
ト・パーライト・ベイナイト、マルテンサイト等の変態
組織及びその生成温度に依存する。[Detailed Description of the Invention] As is well known, the quality of steel materials generally depends on the chemical composition of the steel material, the transformation structures such as ferrite, pearlite, bainite, and martensite that are generated during cooling from high temperature (austenite state), and the temperature at which they are formed. do.
このようなことから目的とする材質を鋼材に与えるため
に変態組織を制御する目的の各種の熱処理または圧延後
の直接熱処理が鋼材に対し行われる。しカルこのとき冷
却中、熱処理において鋼種によつては鋼材の温度履歴が
変態による発熱のために計画した温度パターンから大き
くずれ、目的とする材質がえられない場合がある。例え
ば第1図はO、82C−O、7Mn鋼の900℃■分加
熱オーステナイト化後のCCT図と熱処理(冷却)曲線
を示したものであるが、該鋼材をAのようにある一定冷
却速度で冷却すれば微細パーライト組織となり、強度、
靭性にすぐれた材質が得られるとする。しかし該鋼材を
ある一定の冷却条件(例えば一定の圧力、流量のガスに
よる冷却)で冷却すると変態発熱の影響で冷却パターン
はBのようになり、粗いパーライト組織となるため強度
・靭性が低下する。またより組織を微細とするためCの
ように変態中に急冷すると、一部マルテンサイト組織が
発生しやすく靭性が悪くなる。従つて例えばAのような
冷却曲線を該鋼材に与えるには、変態中の冷却条件(冷
媒の供給量等)を変化させて変態発熱を相殺するように
微妙な制御をする必要がある。このような最適な冷却制
御を行うためには、変態熱の冷却曲線への影響を定量的
に予測し、これにより時々刻々の冷却条件を決定しなけ
ればならない。さらに鋼種と得ようとする材質とによつ
ては熱履歴の冷却(あるいは昇温)速度を途中で任意に
変更する必要がある場合が多いが、このような場合にも
任意の冷却経路で変態の進行を予測しなければ冷却条件
の決定ができない。このような変態熱、冷却(昇温)速
度の変更等により温度パターンが等速冷却あるいは恒温
保持からはずれると、従来のCCT図、TTT図では変
態開始、変態の進行、変態終了の温度、時間等を予知す
ることが困難になり、適正な冷却条件を求めることが困
難となる。そこで冷却速度の変更を伴う冷却パターンで
も適用が可能であり、鋼種と冷却条件を与えることによ
り、計算で変態熱の影響も含めた冷却曲線と変態(変態
開始、その経過、終了および変態組織)とを予測する方
法を開発すれば、目的の冷却曲線を該鋼材に与えるため
の冷却の諸条件を得ることが可能となり、適正な冷却の
制御が可能になる。For this reason, in order to impart the desired material properties to the steel material, various heat treatments for the purpose of controlling the transformed structure or direct heat treatment after rolling are performed on the steel material. At this time, during cooling, depending on the type of steel during heat treatment, the temperature history of the steel material may deviate significantly from the planned temperature pattern due to heat generation due to transformation, and the desired material quality may not be obtained. For example, Figure 1 shows the CCT diagram and heat treatment (cooling) curve of O, 82C-O, 7Mn steel after heating to austenitize at 900°C for 1 minute. When cooled, it becomes a fine pearlite structure, which increases strength and
It is assumed that a material with excellent toughness can be obtained. However, when the steel material is cooled under certain cooling conditions (for example, cooling with gas at a certain pressure and flow rate), the cooling pattern becomes as shown in B due to the effect of transformation heat generation, resulting in a coarse pearlite structure that reduces strength and toughness. . Furthermore, if the material is rapidly cooled during transformation as in C to make the structure finer, a martensitic structure tends to occur in some parts and the toughness deteriorates. Therefore, in order to provide the steel material with a cooling curve such as A, it is necessary to perform delicate control to offset the transformation heat generation by changing the cooling conditions (coolant supply amount, etc.) during the transformation. In order to perform such optimal cooling control, it is necessary to quantitatively predict the effect of transformation heat on the cooling curve, and to determine the cooling conditions from time to time based on this. Furthermore, depending on the type of steel and the material to be obtained, it is often necessary to arbitrarily change the cooling (or heating) rate of the thermal history, but even in such cases, transformation can occur through any cooling path. Cooling conditions cannot be determined unless the progress of the process is predicted. When the temperature pattern deviates from constant cooling or constant temperature maintenance due to changes in the heat of transformation, cooling (temperature rise) rate, etc., conventional CCT and TTT diagrams show the temperature and time at which transformation begins, progresses, and ends. It becomes difficult to predict such factors, and it becomes difficult to find appropriate cooling conditions. Therefore, it is possible to apply a cooling pattern that involves changing the cooling rate, and by giving the steel type and cooling conditions, it is possible to calculate the cooling curve and transformation (transformation start, process, end, and transformed structure) including the effect of transformation heat. If a method for predicting this is developed, it will be possible to obtain cooling conditions for giving the steel material the desired cooling curve, and appropriate cooling control will be possible.
変態の開始温度を計算により求める方法はこれまでの研
究でもなされいくつかの方法が紹介されているが、変態
熱の影響も定量的に把握して変態終了まで計算で予測す
る方法はいまだ提案されていない。Several methods have been introduced in previous studies to calculate the start temperature of transformation, but no method has yet been proposed to quantitatively grasp the influence of transformation heat and predict the end of transformation by calculation. Not yet.
本発明は、変態熱の定量的な影響も定式化し、変態開始
から終了までの変態と冷却曲線とを計算により求める画
期的ないかなる温度パターンにも適用可能な変態予測方
法に基づく熱処理の制御方式を提案するものである。The present invention also formulates the quantitative influence of transformation heat, and controls heat treatment based on a transformation prediction method that can be applied to any innovative temperature pattern that calculates transformation and cooling curves from the start to the end of transformation. This paper proposes a method.
本発明者等は、基礎的な高温冷却実験および実際の線材
等の現場実験を重ねた結果、一般に鋼材の冷却過程にお
いて、以下のような方法により、冷却条件を与えれば鋼
材の変態挙動(変態開始、進行、終了および変態熱によ
る温度パターンの変化、)を予測できることを見出した
。As a result of repeated basic high-temperature cooling experiments and field experiments using actual wire rods, etc., the present inventors have found that, in general, during the cooling process of steel materials, the transformation behavior of steel materials (transformation We found that it is possible to predict the onset, progression, termination, and changes in temperature patterns due to heat of transformation.
即ち変態の開始から終了までの経過がいわゆるTOhn
sOn−Mehlの式でほぼ近似的に表現されることを
多くの基礎実験から明らかにした。In other words, the progress from the start to the end of metamorphosis is the so-called TOhn
It has been clarified through many basic experiments that it can be approximately expressed by the sOn-Mehl equation.
ここでB,Kは定数であるが、とくにBは成分、および
変態前の熱処理時の加熱条件で変化するので、後述のよ
うに一般にはその鋼のある熱処理条件でのTTT曲線を
求め、その一定量変態する時間の温度から求める方法が
とられる。この式を用いると温度TlCC)、変態率Y
1であつた鋼が次の段階で温度T2(℃)になり、この
温度で微小時間Δt保持されるとすればΔt後の変態率
Y2はで表わされる。Here, B and K are constants, but B in particular changes depending on the composition and the heating conditions during heat treatment before transformation. A method is used to determine the temperature at a certain amount of time for transformation. Using this formula, temperature TlCC), transformation rate Y
If the steel at temperature 1 reaches a temperature T2 (° C.) in the next stage and is maintained at this temperature for a minute time Δt, the transformation rate Y2 after Δt is expressed as follows.
この式により温度パターンにそつて変態率の変化を計算
し変態率の累積を求める。次に変態に伴う変態熱の発生
とこれに伴う冷却曲線の変化の計算の手順を第2図に示
す。ある微少時間Δtの間について考えると、変態がな
いと仮定した場合の冷却速度(これを区別して冷却強度
と呼ぶことにする)をVとして鋼材はこの間にΔTc=
Vdt温度降下するはずであるが、実際には変態がこの
間にΔY=Y2−Y1進行するので、これに比例した変
態発熱がある。これをΔnとするとHを全変態潜熱(C
al/f)、この間の平均比熱をC(Deg/y)とし
てH・ΔY=C・ΔThの関係があるので、実際の温度
低下ΔT(Deg)は、として計算される。Using this formula, the change in transformation rate is calculated along the temperature pattern, and the cumulative transformation rate is determined. Next, FIG. 2 shows the procedure for calculating the generation of transformation heat accompanying transformation and the accompanying change in the cooling curve. Considering a certain minute time Δt, assuming that there is no transformation, the cooling rate (this will be distinguished and referred to as cooling intensity) is V, and the steel material will be ΔTc=
Although the Vdt temperature is supposed to drop, the transformation actually progresses by ΔY=Y2-Y1 during this time, so there is heat generated by the transformation in proportion to this. Letting this be Δn, H is the total transformation latent heat (C
al/f), and the average specific heat during this period is C (Deg/y), and there is a relationship of H·ΔY=C·ΔTh, so the actual temperature drop ΔT (Deg) is calculated as follows.
このようにして計算されたT2=T1+ΔTの温度から
また同様の計算を行うことを計算機によりつづけて行く
と変態熱を考慮した刻々の鋼材の温度変化が計算される
ことになる。If the computer continues to perform similar calculations from the temperature T2=T1+ΔT calculated in this way, the momentary temperature change of the steel material taking into account the heat of transformation will be calculated.
なお1の計算を行う際に冷却開始からの時間に対して変
態を原理的に計算できるのであるが、このときB,Rの
値の簡略な決定法として次のような手順を採用すること
ができる。In addition, when performing calculation 1, the transformation can be calculated in principle with respect to the time from the start of cooling, but at this time, the following procedure can be adopted as a simple method for determining the values of B and R. can.
1 ある鋼の恒温変態曲線区匡TTを実験または計算に
より求める。1. Determine the isothermal transformation curve section TT of a certain steel by experiment or calculation.
このとき変態開始線をt=Z(T)と置く。(第3図は
0.62C−0.7Mn鋼を900℃10分間加熱した
ときのTTT曲線を示す。)2連続冷却の変態開始温度
Tsを次のScheilの式に従つて求める。At this time, the metamorphosis start line is set as t=Z(T). (Figure 3 shows a TTT curve when 0.62C-0.7Mn steel is heated at 900°C for 10 minutes.) The transformation start temperature Ts of two consecutive coolings is determined according to the following Scheil equation.
(E.Schecl;Kch.Eiserlhutte
nW.,乎(1935)、P565) ここでΔ×(T
)は温度Tでの恒温保持時間
TOは計算を始める起点の温度
U(T)は温度Tでの時間に対する温度勾配このTsか
ら1式に従つて変態の進行を計算するが、通常同じ種類
の鋼ではRが一定(2〜3程度)であることが基礎研究
かられかつているので、Z(T)からBをB=BOln
Z(T)(BOは定数)として求めることができる。(E. Schecl; Kch. Eiserlhutte
nW. (1935), P565) where Δ×(T
) is the constant temperature holding time TO at temperature T is the starting point temperature U (T) is the temperature gradient versus time at temperature T. From this Ts, the progress of transformation is calculated according to equation 1, but usually the same Basic research has shown that R is constant (approximately 2 to 3) in steel, so we can calculate B from Z(T) by B=BOln
It can be determined as Z(T) (BO is a constant).
本予測法により、変態開始点のみならず変態中の温度、
変態率等も予測可能であるので、目的とする材質の鋼材
を得るための合理的温度パターンを与えるための熱処理
条件を予知することができる。With this prediction method, it is possible to determine not only the temperature at the start of transformation, but also the temperature during transformation.
Since the transformation rate and the like can be predicted, it is possible to predict the heat treatment conditions to provide a reasonable temperature pattern to obtain the desired steel material.
本発明は以上の方法を利用した熱処理制御法を提供する
ものである。制御の手順について第4図を用いて以下説
明する。The present invention provides a heat treatment control method using the above method. The control procedure will be explained below using FIG. 4.
この図は圧延後鋼材の潜熱を利用して直接熱処理を行う
場合の説明であるが、鋼材を冷間の状態から出発して熱
処理を行う場合でも全く同様である。鋼材の成分がわか
つていると熱処理条件からTTTを特定することがでぎ
)る。圧延後の直接熱処理の場合は、圧延条件を指定す
れば熱処理のどのような条件(オーステナイト粒度)に
相当するかを一般に予言できる。Although this figure describes the case where heat treatment is performed directly using the latent heat of the rolled steel material, the same applies even when the steel material is heat treated starting from a cold state. If the composition of the steel material is known, it is possible to specify TTT from the heat treatment conditions. In the case of direct heat treatment after rolling, it is generally possible to predict what conditions (austenite grain size) correspond to the heat treatment conditions by specifying the rolling conditions.
これは圧延方式によつて異なるのでここでは一律に示す
ことができないが、たとえば1製鉄研究JNO.289
(1976)43〜61頁の54頁13図に示すように
予測される。このような手順で、Z(T),B,Rが決
定されるので任意の冷却条件(冷却強度の時間的経過)
に対して1〜4式を用いて変態の開始・経過・終了の温
度と時間を計算することができる。This varies depending on the rolling method, so it cannot be shown uniformly here, but for example, 1 Steel Research JNO. 289
(1976), pages 43-61, page 54, Figure 13. With this procedure, Z(T), B, and R are determined, so any cooling conditions (time course of cooling intensity) can be determined.
The temperature and time at which transformation starts, progresses, and ends can be calculated using Equations 1 to 4.
たとえば高炭素鋼の線材て最適組織とされるのは550
〜600℃て変態したパーライト組織であるが、ある冷
却条件、たとえば第1図のAのようなある一定速度で冷
却する場合上述のような組織が得られるとすると、変態
開始まては一定の冷却強度(たとえば一定の小量による
水冷)で冷却して行き変態開始後計算される刻々の変態
量に応じその変態熱を相殺するように変態終了まで水量
を増加させれば第1図Aのような冷却曲線に沿つて冷却
させることができるのである。次に第1図の点線で示し
たように冷却中(または冷却後)に温度が実測できる場
合は(第4図aの点線)、さらに次のような精密な制御
が可能になる。For example, the optimum structure for high carbon steel wire is 550.
The pearlite structure is transformed at ~600°C, but if the above-mentioned structure is obtained under certain cooling conditions, for example, at a certain constant rate like A in Figure 1, then the transformation starts at a certain level. If you cool with a cooling intensity (for example, water cooling with a fixed small amount) and increase the amount of water until the end of the transformation to cancel out the heat of transformation according to the amount of transformation calculated every moment after the start of transformation, the result shown in Figure 1A is obtained. It is possible to perform cooling along such a cooling curve. Next, if the temperature can be actually measured during cooling (or after cooling) as shown by the dotted line in FIG. 1 (dotted line in FIG. 4a), the following more precise control becomes possible.
上記最適冷却強度に設定して冷却を開始したとき冷却ラ
イン上での刻々の変態量の増加と、これによる変態熱発
生に伴う冷却曲線が特許請求の範囲に示した式で計算で
きるので、冷却ライン上に設置した温度計でこの計算し
た温度との差が検出された場合は冷却条件あるいは圧延
条件が実際には計算に用いた条件から変動しているため
に差異を生じたと考えられる。(圧延条件が変態前のオ
ーステナイト粒度の変化を通じ拡散変態に影響を与える
ことは上述の通りである)。従つてここで実測温度が予
測温度より高い場合は最終的な平均変態温度を低下させ
目的とする微細組織が得られるように冷却強度を増すな
どの手段で冷却を強化する。またこれ以降の時間では当
初設定した冷却強度を大きくする等の変更を加え目標の
材質が中間で冷却条件の修正を行わなくても得られるよ
うにすることができる。このようにして材質を目標に合
致するよう正確に制御することが可能である。また、冷
却制御のみでは最適な変態組織を得ることができない場
合には第4図−bのように加熱又は保温装置を用いて、
必要によりその操業条件(在炉時間、燃料供給量等)を
制御することを付加することにより温度を制御すること
も可能である。When cooling is started with the above optimum cooling intensity set, the cooling curve associated with the momentary increase in the amount of transformation on the cooling line and the generation of transformation heat due to this can be calculated using the formula shown in the claims. If a thermometer installed on the line detects a difference between the calculated temperature and the calculated temperature, it is considered that the difference is caused by the cooling conditions or rolling conditions actually varying from the conditions used in the calculation. (As mentioned above, rolling conditions affect diffusion transformation through changes in austenite grain size before transformation). Therefore, if the measured temperature is higher than the predicted temperature, the cooling is strengthened by means such as increasing the cooling intensity so that the final average transformation temperature is lowered and the desired microstructure is obtained. Further, after this time, it is possible to make changes such as increasing the initially set cooling intensity so that the target material quality can be obtained without intermediately modifying the cooling conditions. In this way it is possible to precisely control the material to meet the target. In addition, if it is not possible to obtain the optimal transformed structure by cooling control alone, heating or heat retention equipment may be used as shown in Figure 4-b.
If necessary, it is also possible to control the temperature by controlling the operating conditions (furnace time, fuel supply amount, etc.).
以下に実施例を示す。Examples are shown below.
第1表に示す成分の5.5Tnφの鋼線について、本発
明を適用して熱処理を行なつた。A 5.5Tnφ steel wire having the components shown in Table 1 was heat treated by applying the present invention.
第1表に示す成分の鋼は、鉛パテンテイング等により、
約550〜60CfCの温度域で変態させると、微細な
パーライト組織となり、強度、靭性にすぐれた材質が得
られることが知られている。この実施例では、鉛パテン
テイング処理等を行なうことなく、簡単な水スプレーの
適用によつて同等のすぐれた強度、靭性を有する微細な
パーライト組織を得ることがてきる。The steel with the composition shown in Table 1 is made by lead patenting etc.
It is known that when it is transformed in a temperature range of about 550 to 60 CfC, it becomes a fine pearlite structure and a material with excellent strength and toughness can be obtained. In this example, a fine pearlite structure having the same excellent strength and toughness can be obtained by simple application of water spray without conducting lead patenting treatment or the like.
第1表に示す鋼62Bを、水スプレーの適用により連続
冷却するときの冷却曲線を、スプレーの水量水準毎に、
変態率(Y2)および鋼62Bの真の温度変化ΔTを求
める(3)式から算出し、スプレーの水量水準毎に第5
図aに示す冷却曲線A,B,Cを得た。The cooling curve when steel 62B shown in Table 1 is continuously cooled by applying water spray is shown for each spray water level.
The transformation rate (Y2) and the true temperature change ΔT of steel 62B are calculated from equation (3), and the fifth
Cooling curves A, B, and C shown in Figure a were obtained.
強度、靭性にすぐれた微細パーライト組織を得るために
は、約550〜600℃の温度域で変態させる必要があ
るが、冷却用スプレーの水量水準毎に求めた冷却曲線A
で、鋼62Bを冷却して行つた場合、変態温度域が60
0℃以上となることが、第5図aに示す予測結果から明
らかであり、従つて変態組織はフェライト+粗いパーラ
イトとなることが予測される。In order to obtain a fine pearlite structure with excellent strength and toughness, it is necessary to undergo transformation in a temperature range of approximately 550 to 600°C.
So, when steel 62B is cooled, the transformation temperature range is 60
It is clear from the prediction results shown in FIG. 5a that the temperature will be 0° C. or higher, and it is therefore predicted that the transformed structure will be ferrite + coarse pearlite.
フェライト+粗いパーライトの組織は強度が低い。同様
に、予測された冷却曲線Bで鋼62Bを冷却して行つた
場合、パーライト変態は終了せず、一部未変態部が残り
、この部分が冷却によつてマルテンサイト組織となるの
で、最終的にパーライト+マルテンサイト組織となるこ
とが予測される。The structure of ferrite + coarse pearlite has low strength. Similarly, when steel 62B is cooled according to the predicted cooling curve B, the pearlite transformation does not complete, and some untransformed parts remain, which become martensitic structures upon cooling, so that the final It is predicted that the structure will be pearlite + martensite.
このような組織は靭性が劣る。同様に、予測された冷却
曲線Cで鋼62Bを冷却して行つた場合、570〜60
0℃の温度域で変態することになるからフェライト+微
細パーライト組織が得られることが予測される。このよ
うな組織は、強度、靭性にすぐれた所期の特性を示す。
そこで、この実施例では、予測の前提となつた、スプレ
ー冷却における水量水準別に鋼6?を、800℃の温度
から冷却を開始し進めて行つた。Such a structure has poor toughness. Similarly, when steel 62B is cooled using the predicted cooling curve C, 570 to 60
Since the transformation occurs in the temperature range of 0°C, it is predicted that a ferrite + fine pearlite structure will be obtained. Such a structure exhibits the desired properties of excellent strength and toughness.
Therefore, in this example, steel 6? The cooling was started from a temperature of 800°C and proceeded.
その結果を第2表に示す。第2表から明らかなように、
予測された結果、(最終的に得られる組織)と、実際の
結果は一致している。The results are shown in Table 2. As is clear from Table 2,
The predicted results (finally obtained tissue) match the actual results.
このことは、この発明になる鋼の変態、組織制御法の適
用により所望の材質を得ることができることを示してい
る。次の実施例として、第1表に示す鋼77Bを対象一
として、熱処理を行なつた。鋼77Bにおいても、微細
パーライト組織にするためには、約550〜600℃の
温度域で変態させねばならないけれども、この鋼種は、
C量が多く、焼き入り易い。この実施例においても冷却
速度35きC/Sとなる冷却水量水準で第5図bに示す
冷却曲線を求めた。冷却曲線Dがそれであるが、この冷
却曲線で冷却が行なわれた場合はパーライト+マルテン
サイトの組織が得られることが予測される。このような
組織は靭性に欠ける。This shows that a desired material quality can be obtained by applying the steel transformation and structure control method according to the present invention. In the next example, steel 77B shown in Table 1 was subjected to heat treatment. Steel 77B also needs to be transformed in a temperature range of about 550 to 600°C in order to form a fine pearlite structure, but this steel type
It has a large amount of C and is easily hardened. In this example as well, the cooling curve shown in FIG. 5b was determined at a cooling water flow level that resulted in a cooling rate of 35 C/S. This is cooling curve D, and if cooling is performed using this cooling curve, it is predicted that a pearlite + martensite structure will be obtained. Such a structure lacks toughness.
そこで、この実施例では、変態の途中で冷却を停止し、
温度パターンを緩冷或は、僅かに昇温或は、恒温にする
ために保熱炉に装入した。そのときの冷却曲線を既に述
べた手段により求め、冷却曲線Eを得た。冷却曲線Eに
沿つて、800℃から冷却を開始し、上に述べたように
変態の途中で冷却を停止し、保熱したその結果を第2表
に示す。第2表から明らかなように、予測された結果(
最終的に得られる組織)と、実際の結果は一致している
。Therefore, in this example, cooling was stopped in the middle of the transformation,
The material was placed in a heat retention furnace in order to have a temperature pattern of slow cooling, slight increase in temperature, or constant temperature. The cooling curve at that time was determined by the method described above, and a cooling curve E was obtained. Along cooling curve E, cooling was started from 800° C., cooling was stopped in the middle of transformation as described above, and heat retention was performed. The results are shown in Table 2. As is clear from Table 2, the predicted results (
The final tissue obtained) is consistent with the actual results.
このことは、先に述べたように、本発明の変態熱の影響
を織込んだ冷却曲線の予測に基づく、鋼材の温度・時間
関係の、保熱或は加熱をも含めた制御によつて、種々の
鋼について、所望の材質を得ることができることを示し
ている。As mentioned earlier, this can be achieved by controlling the temperature/time relationship of the steel material, including heat retention or heating, based on the prediction of the cooling curve that incorporates the effects of transformation heat according to the present invention. , it has been shown that desired materials can be obtained for various steels.
第1図は変態曲線及び冷却曲線を示す例、第2図は変態
熱の考え方を示す図、第3図は恒温変態曲線TTTにお
ける変態開始線を示す図、第4図A,bは本発明の具体
的方式例のフロー、第5図A,bは本発明による熱処理
パターンの例をそれぞれ示す。Figure 1 is an example showing a transformation curve and cooling curve, Figure 2 is a diagram showing the concept of transformation heat, Figure 3 is a diagram showing the transformation start line in the isothermal transformation curve TTT, Figure 4 A and b are according to the present invention. 5A and 5B respectively show examples of heat treatment patterns according to the present invention.
Claims (1)
える熱処理において、温度T_1(℃)、変態率Y_1
の鋼が次の段階で温度T_2(℃)で微小時間Δt保持
された後の変態率Y_2を、▲数式、化学式、表等があ
ります▼ また、変態熱のない場合の冷却速度をV(deg/秒)
全変態熱をH(cal/g)、比熱をc(cal/de
gg)としてこの時間Δt間の変態発熱と冷却とによる
鋼の正味の温度変化ΔT=T_2−T_1(deg)を
、ΔT=VΔt−(Y_2−Y_1)(H/C)なる式
で任意の冷却条件下での刻々の変態の進行を計算より求
め、これにより変態温度域を予測し、これを希望の変態
温度域と比較して差異があれば冷却条件を修正して、さ
らに必要であれば、冷却停止、保温、昇温の手段を附加
することにより、変態温度域で希望の変態をさせ所期の
材質を得ることを特徴とする鋼の変態組織制御法。[Claims] 1. In heat treatment to achieve the desired material quality by causing diffusion transformation of steel at a desired temperature, temperature T_1 (°C), transformation rate Y_1
The transformation rate Y_2 after the steel is held at temperature T_2 (℃) for a short time Δt in the next stage is expressed as ▲There are mathematical formulas, chemical formulas, tables, etc.▼ Also, the cooling rate in the absence of transformation heat is expressed as V (deg / second)
The total heat of transformation is H (cal/g), and the specific heat is c (cal/de).
gg), the net temperature change of the steel due to the transformation heat generation and cooling during this time Δt, ΔT=T_2−T_1 (deg), can be expressed as an arbitrary cooling value using the formula ΔT=VΔt−(Y_2−Y_1)(H/C). Calculate the progress of transformation moment by moment under the conditions, predict the transformation temperature range from this, compare this with the desired transformation temperature range, and if there is a difference, modify the cooling conditions, and if necessary, A method for controlling the transformed structure of steel, which is characterized in that by adding means for stopping cooling, retaining heat, and increasing the temperature, the desired transformation is carried out in the transformation temperature range and the desired material quality is obtained.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2346980A JPS6056210B2 (en) | 1980-02-28 | 1980-02-28 | Steel transformation structure control method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2346980A JPS6056210B2 (en) | 1980-02-28 | 1980-02-28 | Steel transformation structure control method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56119741A JPS56119741A (en) | 1981-09-19 |
| JPS6056210B2 true JPS6056210B2 (en) | 1985-12-09 |
Family
ID=12111381
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2346980A Expired JPS6056210B2 (en) | 1980-02-28 | 1980-02-28 | Steel transformation structure control method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6056210B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6399211U (en) * | 1986-12-18 | 1988-06-27 |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2020138294A1 (en) * | 2018-12-27 | 2020-07-02 | 日本製鉄株式会社 | Heat treatment analysis method and device, program, and recording medium |
-
1980
- 1980-02-28 JP JP2346980A patent/JPS6056210B2/en not_active Expired
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6399211U (en) * | 1986-12-18 | 1988-06-27 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56119741A (en) | 1981-09-19 |
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