钒微合金化非调质钢48MnVS的奥氏体动态再结晶行为

实验用非调质钢48MnVS（/%:0.48C,0.60Si,1.50Mn,0.35Cr,0.14V,0.05S,0.020Al,0.0150N）由100t EAF冶炼,连铸成280 mm×360 mm坯,轧成Φ100 mm棒材。通过Gleeble-3800热模拟实验机研究了变形温度950~1150℃,变形速率0.1~10 s^-1,变形量60%的单道次压缩钒微合金非调质钢48MnVS的奥氏体再结晶过程得出真应力-应变曲线,计算得出实验钢的动态再结晶晶粒尺寸模型和动态再结晶状态图。结果表明,钒微合金化非调质钢48MnVS变形温度越高,变形速率越低,则发生动态再结晶的形变储能越小,越容易发生动态再结晶。实验钢48MnVS的动态再结晶激活能为Q_d=343.202 kJ/mol。     

微合金化非调质钢C38N2动态再结晶行为

针对微合金化非调质钢热轧过程的变形特征,通过Gleeble-3800热模拟试验机研究了Nb-Ti-V非调质钢C38N2(/%:0.40C、0.52Si、1.42Mn、0.010P、0.047S、0.028V、0.025 Ti、0.022Nb)在950～1 150℃,变形速率0.1～10 s-1变形量60%,单道次压缩时的奥氏体动态再结晶过程,计算得出C38N2钢的动态再结晶晶粒尺寸模型和动态再结晶状态图。结果表明,C38N2钢变形温度越高,变形速率越低,则发生动态再结晶的储蓄能越小,动态再结晶越易发生。C38N2钢的动态再结晶激活能Q_d=294.905 kJ/mol。     

HGH3126镍基合金热变形行为及组织演变

通过热压缩实验研究了HGH3126镍基合金（/%:≤0.005C,17.20Cr,4.21W,16.25Mo,5.49Fe,0.46Mn,0.20V）在变形温度为950～1200℃、应变速率为0.01～10 s^-1的热变形行为。基于Arrhenius方程和Zener-Hollomon参数模型,建立了HGH3126合金高温热变形的流变应力本构方程。通过对高温热变形后的HGH3126合金显微组织进行观察,分析了变形温度和应变速率对HGH3126合金动态再结晶行为的影响。结果表明,变形温度越高,合金动态再结晶越容易形核;应变速率越小,合金动态再结晶过程进行得越充分。当应变速率0.1 s^-1,变形温度1100℃时,该合金基本发生完全动态再结晶。     

Nb-V-Ti微合金化0.37C-1.45Mn非调质钢动态再结晶行为

借助Gleeble-3800热模拟实验机研究了真空感应炉熔炼,并锻成φ25 mm棒材的Nb-V-Ti微合金化0.37C-1.45Mn非调质钢(/%:0.37C,0.60Si,1.45Mn,0.025Nb,0.078V,0.017Ti)在950~1150℃,形变速率0.1~10 s^-1,形变量60%的单道次压缩的奥氏体动态再结晶过程。结果表明,Nb-V-Ti微合金化0.37C-1.45Mn钢形变温度越高,形变速率越低,则发生动态再结晶的形变储能越小,越容易发生动态再结晶。试验用钢因含有Nb而动态再结晶激活能较高,为Q_d=353.80 kJ/mol。     

钒对直接切削用非调质钢动态再结晶的影响

 在Gleeble-3800热模拟试验机上进行热变形试验,研究不同钒质量分数的直接切削用非调质钢在变形温度为950～1 150 ℃,应变速率为0.1～10 s-1,变形量为60%的单道次压缩的奥氏体再结晶过程,计算得出V1钢的动态再结晶激活能[Qd]比V2钢提高了79.617 kJ/mol,增加钒质量分数具有抑制奥氏体动态再结晶发生的作用。根据试验模拟结果并结合实际生产情况,确定V1钢和V2钢最佳的热加工工艺参数。     

CSP热轧TRIP钢动态再结晶行为研究

摘要：采用Gleeble-3500热模拟试验机,在温度为950~1150℃、应变速率为0.1~10s-1和变形量为65%的条件下研究了CSP热轧TRIP钢的动态再结晶行为,探讨了初始奥氏体晶粒尺寸对TRIP钢动态再结晶行为的影响。研究结果表明,初始奥氏体晶粒尺寸越小,变形温度越高,应变速率越慢时,TRIP钢中奥氏体越易发生动态再结晶。其中,粗晶试样（初始奥氏体晶粒尺寸为767.54μm）在1050~1150℃内变形时,将发生动态再结晶。其热变形激活能为361539.17J/mol,确定了Zener-Holloman参数与应变速率和温度的关系式,建立了动态再结晶临界应变模型、高温奥氏体流动应力模型和动态再结晶晶粒尺寸模型,理论模拟结果与试验结果吻合较好。     

38MnSiVS非调质钢奥氏体晶粒长大模型

 细化奥氏体晶粒是控制钢的组织与力学性能的重要方法。为了控制38MnSiVS非调质钢在轧制待温时间内的晶粒尺寸,利用热变形与定量金相方法,研究了38MnSiVS非调质钢变形后在不同待温温度、不同待温时间的再结晶奥氏体晶粒长大规律。结果表明,38MnSiVS非调质钢再结晶奥氏体晶粒长大过程与时间满足幂指数关系。基于试验数据,通过数值解析和非线性回归分析求得Anelli、Sellars与Sellars修正模型3种晶粒长大模型,其中Sellars修正模型预测误差最小为0.73%,能够更加精确地预测38MnSiVS非调质钢晶粒长大规律。由于形变储能等因素的影响,变形后再结晶奥氏体晶粒长大激活能为161 737.65 J/mol,远小于再加热过程奥氏体晶粒长大激活能。     

GH4169合金高温变形显微组织演变及热加工图

在Gleeble-3500D热模拟机上采用单道次等温压缩试验,系统研究了GH4169合金在变形温度为900～1 150℃、应变速率为0.01～10 s~(-1)、变形量为10%～70%条件下的动态再结晶行为,确定了合金在不同变形条件下的完全再结晶条件,绘制了再结晶图,给出了该合金变形的热加工图。研究结果表明:GH4169合金随变形过程温度的升高而再结晶程度增大,变形量越大、应变速率越慢,发生完全动态再结晶的温度区间越宽;在应变速率为0.01 s~(-1)时变形过程中经历了变形-回复-再结晶-晶粒长大的完整过程;而应变速率为10 s~(-1)条件时,仅发生了变形-回复-(完全/部分)再结晶的过程,晶粒还未有充分长大的动力学条件;随着变形量增加,GH4169合金的易加工区间(η)和稳定加工区间(■)越宽,在变形量为70%时温度为965～1 134℃,应变速率0.02～10 s~(-1)范围内,(■)大于0,处于加工稳定区。     

变形条件对GH625合金高温变形动态再结晶的影响

采用Gleeble高温压缩实验研究了变形条件对GH625合金高温变形动态再结晶的影响,结果表明:当变形程度较小时,原始晶粒内部出现大量孪晶,晶界呈现锯齿状凸出;随变形程度的增加,在晶界弓出部位开始形核,形成大量再结晶晶粒,随变形程度进一步增加,GH625合金动态再结晶体积分数增大,但是再结晶晶粒尺寸无明显变化;GH625合金动态再结晶是一个受变形温度和应变速率控制的过程,变形温度越高,动态再结晶越容易形核,应变速率越小,动态再结晶过程进行得越充分。在低应变速率条件下,GH625合金获得完全动态再结晶组织的温度随变形速率的升高而升高,而在高应变速率条件下必须考虑变形热效应对合金变形组织的影响。     

利用热模拟技术探讨微Ti对低碳钢热变形特性的影响

利用热模拟技术就微Ｔｉ在低碳钢热变形过程中的作用进行了初步探讨。结果表明，奥氏体的动态再结晶行为主要受变形温度的影响（变形速率、变形量不变时），在较高温度变形时，微Ｔｉ几乎没有推迟奥氏体发生动态再结晶的作用。在变形温度稍低时，微Ｔｉ对含碳较低的钢的作用大于含碳较高的钢。Ｔｉ的啬对高温变形抗力影响不大。     

New Type Austenite Dynamic Recrystallization of Microalloyed Forging Steels 38MnVS During Forging Process

 Hot compression tests of microalloyed forging steels 38MnVS were carried out on the Gleeble-3800 thermo-mechanical simulator at the deformation temperatures from 950 to 1150 ℃ with the strain rates ranging from 0. 1 to 10 s-1. The effects of the deformation temperature and strain rate on the austenite dynamic recrystallization and microstructural changes were researched. The experimental results show that the dynamic recrystallization accelerated with the increase of the deformation temperatures and the decrease of the strain rate. The activation energy of dynamic recrystallization was calculated, which was about 275. 453 kJ/mol. The relation between the dynamic recrystallization and the Z-parameter was investigated, and the state chart of the dynamic recrystallization of the microalloyed forging steel 38MnVS was made according to the experimental data and the deformation parameters.     

汽车用高品质非调质钢YF45MnVS的热变形行为

用Gleeble-1500热模拟实验机对YF45MnVS钢(%:0.48C、0.45Si、1.36Mn、0.009P、0.043S、0.086V)200 mm×200 mm铸坯上切取的Φ8mm试样进行950～1 200℃,变形速率10^-2～10¹s^-1变形量10%～50%的单道次等温压缩试验。结果表明,低应变速率和大变形量有利于实验用钢动态再结晶的发生。通过计算得到YF45MnVS钢在950～1 200℃的动态再结晶激活能为299.55 kJ/mol。     

高速列车车轴钢30NiCrMoV12的热变形行为

通过Φ250 mm锻件切取的试样在Gleeble-3500热模拟机于850~1150℃以应变速率0.01~10s^-1对高速列车车轴钢30NiCrMoV12(/%:0.26C,0.33Si,0.62Mn,3.01Ni,0.82Cr,0.56Mo,0.10V)进行了热压缩试验。研究了车轴钢在热变形过程中奥氏体变形行为及再结晶规律,确定了车轴钢的热变形方程,建立应变量ε为0.5和0.9的热加工图。结果表明,在应变速率一定时,温度越高,变形量越大,则越有利于动态再结晶的发生;随着温度升高以及应变速率降低,能量耗散效率η逐渐升高;当真应变0.5,温度1100℃,应变速率0.01 s^-1时,变形能量耗散效率达到最大值0.41。该车轴钢在1000~1150℃,应变速率0.01~1.0s^-1时,具有较好的可锻性。     

Dynamic and Static Recrystallization Behaviour of Coarse-grained Austenite in a Nb-V-Ti Microalloyed Steel简

The dynamic recrystallization （DRX） and static recrystallization （SRX） behaviour of coarse-grained aus- tenite in a Nb-V-Ti microalloyed steel were studied by using a Gleeble thermomechanical simulator. Continuous and interrupted compression tests of coarse-grained austenite were performed in the temperature range of 1000-1 150 ℃ at a strain rate of 0. 1- 5 s 1. The peak and critical strains for the onset of DRX were identified with strain hardening rate analysis, and the ratio of critical strain to peak strain was found to be consistent with the one reported for fine- grained austenite. An equation of the time for 50% softening was proposed by considering the activation energy of steel without microalloying elements and the solute drag effect of microalloying elements. Strain-induced precipitation may not take place at the deformation temperature above 1000 ℃, which indicates that SRX of coarse-grained aus- tenite is mainly retarded by coarse grain size and Nb in solution during rough rolling.     

Recrystallization behavior of twin roll cast low carbon steel strip

The dynamic and static recrystallization behaviors of twin roll cast low carbon steel strip were investigated with an attempt to provide guiding deformation parameters for the on line hot rolling.In order to investigate dynamic recrystallization behavior,as cast strip was reheated and soaked with austenite grain size similar to the width level of the as cast columnar structure.Tensile test was used and the deformation temperature is in the range of 900℃to 1 100℃and strain rates are 0.01 s^-1,0.1 s^-1,1 s^-1.The activation energy and stress exponent were determined as 306kJ/mol and 4.69 respectively.The ratio of critical strain to the peak strain is 0.65,and that of critical stress to the peak stress is 0.92.The dependence of the peak strain on the initial grain size and Zener - Hollomon parameters Z isε_p =9.1×10^-4×D₀^0.48Z^0.13.The kinetics of the dynamic recrystallization and recrystallized grain size was predicted using models published.The as cast coarse austenite were dramatically refined after complete dynamic recrystallization.For static recrystallization,the tensile test was carried out on Gleeble -3500 thermo - mechanical simulator.The deformation temperature is in the range of 800℃to 1 200℃with strain rate 0.01 s^-1 to 1s^-1.The pre strain is fixed at 0.04 to 0.12 and the inter-hit delay time varies from 1 s to 3 000 s.The activation energy and Avrami exponent of static recrystallization were determined as 241 kJ/mol and 0.54 respectively.A kinetics model was proposed to describe the static recrystallization kinetics.The predicted results were in good agreement with the experimental results.     

0.03Nb-0.15Ti微合金化低碳高强度钢的动态再结晶

通过Gleeble 1500热模拟试验机试验研究了Nb-Ti微合金化低碳钢（/%:0.06C,0.22Si,1.80Mn,0.03Nb,0.15Ti,≤0.007N,≤0.002S）10mm带钢在850~1100℃,以应变速率0.1~20.0 s^-1,总变形量75%单道次压缩变形时动态再结晶,由真应力-真应变曲线,结合加工硬化率曲线,得出动态再结晶临界应变0.4~0.7和完全再结晶应变量1.1~1.4。该钢的热变形激活能为618.225 kJ/mol。根据试验结果得到Zener-Hollomon方程和动态再结晶状态图,利用Johnson-Mehl-Avrami（JMA）方程法得到再结晶体积分数实际值,采用Epsilon-P模型对实验数据进行回归,得到试验钢的再结晶动力学模型。     

40Mn2V非调质钢热变形再结晶的研究

采用Gleeble-1500热模拟机测得40Mn2V微合金化非调质钢(%:0.38C、1.48Mn、0.12V)Φ90 mm管坯在800～1 000℃、变形速率0.5～2.0 s^-1时的真应力-应变曲线,并研究了该钢的动态再结晶行为。结果表明,40Mn2V钢的动态再结晶激活能Q_d为382.21 kJ/mol,通过动态再结晶图得出,因子Z＞2.621×10¹⁵时,40Mn2V钢动态再结晶难以完成,当因子Z＞2.014×10¹⁷时,该钢动态再结晶难以发生。