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利用本钢Gleeble-2000热/力模拟试验机结合本钢薄板坯连铸连轧生产线生产低碳含Nb钢X46的生产工艺,对不同Nb含量的低碳钢进行单道次压缩实验.考虑了钢中Mn和Nb的影响,回归了变形抗力模型.现场数据和热模拟实验结果表明:管线钢X46的再结晶终止温度为981.3 ℃.薄板坯连铸连轧粗轧阶段的动态软化率接近于1.考虑动态再结晶以及未再结晶区的应变累计,计算的变形抗力与现场实测的变形抗力吻合良好.表明该模型能够预测薄板坯连铸连轧生产线生产低碳含Nb钢的变形抗力. 相似文献
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利用Gleeble-2000热模拟试验机对Q345GJC钢(/%:0.16C,0.36Si,1.37Mn,0.026Nb)进行了单道次压缩试验,实测了试验钢900~1 150℃、真应变0.8~1.2、应变速率0.1~1 s-1的变形抗力,分析了各工艺变形参数对试验钢动态再结晶和变形抗力的影响。确定了试验钢的动态再结晶激活能为245.448 kJ/mol(峰态时)和166.994 kJ/mol(稳态时),并建立了试验钢高温变形抗力的数学模型。该模型具有良好的曲线拟合特性,用该模型计算的结果与实测值吻合较好。 相似文献
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利用热模拟试验机,在850~1 150℃、应变量为0.1~0.7和应变速率为1~50 s~(-1)的条件下对耐热钢P91进行高温单道次压缩试验,分析压缩变形温度、压缩变形量和变形速率对材料变形抗力的影响。结果表明,压缩变形温度对材料变形抗力的影响最大,变形温度与变形抗力对数间呈近似线性关系,变形速率和变形量对材料变形抗力也产生较大影响,材料压缩变形抗力受三者共同作用的影响。且在较高变形速率和较低应变速率时,动态再结晶过程都会受到抑制,低应变速率下金属畸变能较低,而高应变速率下金属来不及发生动态再结晶过程。利用多元非线性拟合回归建立了P91变形抗力模型,拟合结果与实测结果吻合程度较好。 相似文献
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设计了不同间隔时间的双道次压缩实验,模拟热轧条件下5%Ni低温压力容器钢07Ni5DR的变形过程,实测了实验钢的应力-应变曲线。根据应力-应变曲线计算软化率,绘制出软化率-时间曲线,确定实验钢在不同变形温度变形后不同保持时间内的静态软化率。此外,分析静态再结晶动力学过程,为制定合理的轧制工艺提供了实验和理论依据。研究表明,5%Ni低温钢的静态再结晶软化率随变形温度的升高和道次间隔时间的延长而增大,其静态再结晶激活能为233.97 kJ/mol。此外,建立了5%Ni低温钢的静态再结晶动力学方程。 相似文献
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设计了不同间隔时间的双道次压缩实验,模拟热轧条件下5%Ni低温压力容器钢07Ni5DR的变形过程,实测了实验钢的应力-应变曲线。根据应力-应变曲线计算软化率,绘制出软化率-时间曲线,确定实验钢在不同变形温度变形后不同保持时间内的静态软化率。此外,分析静态再结晶动力学过程,为制定合理的轧制工艺提供了实验和理论依据。研究表明,5%Ni低温钢的静态再结晶软化率随变形温度的升高和道次间隔时间的延长而增大,其静态再结晶激活能为233.97 kJ/mol。此外,建立了5%Ni低温钢的静态再结晶动力学方程。 相似文献
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利用Gleeble-3500热模拟试验机在变形温度900~1 200℃和应变速率0.01~10 s-1范围内,对40Cr钢试样进行压缩实验。研究了40Cr钢真应力-应变曲线特征,建立了峰值应力、应变速率和变形温度间的本构方程,并确定了40Cr钢热变形激活能为310.625 kJ/mol。研究结果显示:40Cr钢热变形时的流变软化机制为动态回复和动态再结晶;随着变形温度增加和应变速率减小,流变应力减小;试样的变形温度越高,应变速率越低,显微组织中的动态再结晶越完全,并且动态再结晶晶粒越容易长大。 相似文献
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Prediction of Rolling Load, Recrystallization Kinetics, and Microstructure During Hot Strip Rolling 总被引:1,自引:0,他引:1
The recrystallization kinetics and grain size models were developed for the C Mn and niobium containing steels to describe the metallurgical phenomenon such as softening, grain growth, and strain accumulation. Based on the recrystallization kinetics equations, the mean flow stress and the rolling load of each pass were predicted and the optimum rolling schedule was proposed for hot strip rolling. The austenite grain refinement is associated with the addition of niobium, the decrease of starting temperature of finish rolling, and the reduction of finished thickness. The mean flow stress curve with a continuous rising characteristic can be usually observed in the finish rolling of niobium containing steel, which is formed as a result of the heavy incomplete softening and strain accumulation. The predicted rolling loads are in good agreement with the measured ones. 相似文献
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40Cr10Si2Mo钢的热变形模型及动态再结晶行为 总被引:1,自引:0,他引:1
为了优化马氏体耐热钢40Cr10Si2Mo的热轧生产工艺参数,建立线棒材轧制数字化设计及智能化系统数据库,在Gleeble-3500热模拟机上对马氏体耐热钢40Cr10Si2Mo进行单道次热压缩试验,研究了该钢在温度为900~1 100 ℃、应变速率为0.1~20 s-1条件下的应变补偿本构方程及动态再结晶行为,为探索塑性变形行为和组织优化提供理论依据。结果表明,应力随变形温度的升高而减小,随应变速率的增加而增加。温度和应变速率对热变形抗力(真应力)的影响主要取决于在塑性变形过程中,金属内部发生的加工硬化与动态回复、再结晶等软化机制交互作用的结果。建立了双曲正弦(Arrhenius)本构模型。对比发现所建立的本构模型预测值与试验值相关系数R2为0.983 97,平均相对误差(AARE)为4.531%。采用对σ-ε曲线进行4次多项式拟合并求导的方法,分析了40Cr10Si2Mo钢的软化过程以及不同温度和应变速率下动态再结晶的临界条件。阐述了动态再结晶的临界条件与lnZ(Zener-Hollomon参数)值的关系。发现40Cr10Si2Mo钢在lnZ值小于63时,动态再结晶的临界应变随lnZ值的增大而增大。在lnZ值大于63时,动态再结晶的临界应变随lnZ值的增大变化不明显。对比了40Cr10Si2Mo钢的微观组织,发现在1 100 ℃/0.1 s-1条件下晶粒发生了相互吞食合并,部分再结晶晶粒没有长大,最终导致混晶组织出现。然而增加应变速率有助于动态再结晶晶粒的细化。 相似文献
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�����࣬�λ�ƽ�������������𣬴����� 《钢铁研究学报》2013,25(8):46-50
By using the thermal simulation technology, the effect of RE on the recrystallization behavior of low-carbon micro-alloyed steel was investigated in the laboratory. The results show that, effect of RE composition on dynamic recrystallization critical strain ??D is more obvious, the critical strain of RE content to 100??10-6 and RE content to 60??10-6 samples are higher than the without RE samples, and with the amount of RE increase, the recrystallization is no longer to occur when the deformation temperature reached 910??, so dynamic recrystallization is delayed to occur by adding of RE, and the delayed effect was more obvious with the addition of rare earth increased. Effect of RE on double-pass static recrystallization softening rate at high-temperature is more obvious than that of low temperature rolling. And compared without RE samples, additting the appropriate amount of RE deformation resistance is improved obviously. So recrystallization easily occurs in the pass-interval times, while less rare earth content has no significant effect. 相似文献
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为了探索材料热塑性变形工艺理论,针对热轧态17Cr2Ni2Mo齿轮用钢进行热力模拟试验,研究材料在应变速率=0.01~10 s-1、热变形温度t=1 050~1 150 ℃条件下的动态再结晶行为。结果表明,在较高应变速率下,应力在峰值后,出现动态回复或持续性动态再结晶软化,在较低应变速率下,应力呈现波浪多峰值状,出现多次动态再结晶软化。通过加工硬化率随应变变化曲线(θ ε),确定了动态再结晶临界特征应变量εc,结合峰值应变量εp统计得到εc/εp比值为0.629~0.854,并可知当应变速率一定时,εc随着温度升高而减小,当温度一定时,εc随应变速率的增大而增大。同时建立了流变应力本构方程,数据验证平均相对误差为1.705%。最后建立了动态再结晶动力学模型。 相似文献
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Static Recrystallization Kinetics Model After Hot Deformation of Low-Alloy Steel Q345B 总被引:2,自引:0,他引:2
The static recrystallization behavior of low-alloy steel Q345B during double-pass hot compression deformation tests was investigated in the temperature range of 900-1000 ℃,the true strain range of 0.15-0.25 and the interpass time range of 0.5-50 s on Gleeble-3500 thermo-simulation machine.The results show that static recrystallization during the interpass time is observed.As the deformation temperature and strain increase,softening caused by static recrystallization is obvious.According to the analysis and calculation of thermo-simulation data,the static recrystallization activation energy was obtained and static recrystallization kinetics model was built.Finally,the error analysis of static recrystallization kinetics model proved that the model had good accuracy.Therefore,this model provides a theoretical basis for static recrystallization(SRX)and will contribute to the development of multipass hot rolling process,in order to control the rolling process more accurately. 相似文献
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通过现场实际数据利用数学回归的方法建立了310S热轧变形抗力模型,模型计算的轧制力与实测值符合良好。利用所建立的模型对比分析了310S和304热轧变形抗力的影响因素,结果表明,随着温度的降低,310S变形抗力的增加速度较304快。 相似文献
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Microstructure Evolution and Dynamic Softening Mechanism of 00Cr22Ni5Mo3N DSS During Hot Compression
Through plane strain compression, hot ductility of 00Cr22Ni5Mo3N DSS is studied under plane strain condition, and the dynamic softening mechanism is investigated through microstructure observation under TEM. The results show that the deformation temperature can markedly influence the peak stress of 00Cr22Ni5Mo3N specimens. And being different from DSS softening mechanism generally reported, ferrite can be softened through dynamic recovery and recrystallization, but austenite can be softened only through dynamic recovery during hot deformation. The unfavourable effect of N on softening capacity of austenite is greater than that of Ni. 相似文献