应用ProcessingMap研究D2钢高温变形的动态应变时效

应用以动态材料模型为基础的ＰｒｏｃｅｓｓｉｎｇＭａｐ研究了Ｄ２钢在变形温度９００～１１６０℃、变形速率０．０１～１０．００ｓ－１区间的动态应变时效规律。结果表明，Ｄ２钢在变形温度为１１２０～１１５０℃、变形速率为０．０１ｓ－１条件下发生动态应变时效，并表现出强烈的硬化效应。同时，应变速率敏感系数小于零可以作为发生动态应变时效的一个标志。     

60Si2MnA弹簧钢的热变形行为

通过热模拟压缩试验，研究了60Si2MnA弹簧钢高温变形时的力学行为和动态再结晶行为。由实验数据求得了60Si2MnA弹簧钢的热变形激活能，峰值应力，峰值应变以及动态再结晶晶粒尺寸与Zener-Hollomon参数之间的关系。结果表明，通过动态再结晶能获得细小的晶粒。     

Q235钢的热变形特性

通过热模拟压缩试验,研究了Q235钢热变形时的动态再结晶行为,确定了其热变形激活能,建立了峰值应力、峰值应变、晶粒尺寸与Zener-Hollomon参数之间的关系模型.结果表明:Q235钢的动态再结晶主要发生在形变温度≥900℃、应变速率≤5 s-1(即lnZ≤37.77)的条件下.     

热变形对中铬半钢热疲劳裂纹扩展动力学的影响

研究了热变形对中铬半钢热疲劳裂纹扩展动力学的影响。结果表明 :中铬半钢的热疲劳裂纹扩展符合 L =b Na(a<1)的关系。变形量小于 4 0 %时 ,随变形量的增加 ,裂纹扩展速率减小 ,其激活能随之增大。这些变化是由于碳化物形状的改变和粒状碳化物的析出所致。     

Hot Deformation Behaviors of $31042 Austenitic Heat-Resistant Steel

The hot deformation behavior of S31042 austenitic heat-resistant steel was investigated over the tempera- ture range of 900--1 200 ℃ and strain rate range of 0.01--10 s- 1 using hot compression tests a...     

Hot Deformation Characteristics of 34CrMo4 Steel

The 34CrMo4(AISI 4130)steel is extensively utilized in the compressed natural gas cylinders.Due to the importance of thermomechanical processing in the production of these cylinders,the dynamic recrystallization(DRX)characteristics of 34CrMo4 steel were investigated.The effect of hot deformation parameters such as temperature and strain rate on the dynamic restoration processes of a 34CrMo4 alloy was studied.Hot compression tests were performed in the temperature range of 900 to 1100 ℃ and the strain rate r...     

一种曲轴用中碳非调质钢的热变形行为

用Gleeble-3500热力模拟试验机对一种中碳曲轴用非调质钢进行1 223~1 473 K和0.2~10 s-1的热压缩变形,获得了其流变曲线,并给出了试验用钢的热变形方程式、动态组织状态图、动态再结晶晶粒尺寸与Z参数之间以及动态再结晶分数与应变量之间的定量关系式。结果表明,试验用钢的流变应力和峰值应变均随变形温度的降低和应变速率的提高而增大,动态再结晶晶粒平均尺寸随着变形Z参数的增大而减小,Z参数越大,发生动态再结晶和完全动态再结晶所需的应变也越大。     

中碳钢形变及冷却过程中的组织演变

热模拟单向压缩下,中碳钢形变温度低于Ad3（786℃）点时,析出形变诱导铁素体（DIF）,DIF量随形变温度降低而提高;在低于750℃形变时,DIF量远高于平衡态铁素体含量54％。DIF析出时碳原子高度富集在铁素体晶界和铁素体／奥氏体界面。形变后在低于A1（719℃）温度等温或控冷过程中。过冷奥氏体将发生不同类型的转变：高于Ad3形变试样中,奥氏体转变为铁素体＋片层状珠光体;低于Ad3点但高于Ar3（645℃）点形变时,未转变奥氏体转变为铁素体＋片层状珠光体＋晶界渗碳体;稍高于Ar3点形变时,将获得铁素体＋弥散渗碳体的球化组织。     

Modeling of Mechanical Characteristics in Hot Deformation of 4130 Steel

In this investigation, hot compression tests were performed at 900 °C ? 1100 °C and strain rate of 0.001 ? 0.1 s^?1 to study hot deformation behavior and flow stress model of 4130 steel. Based on the classical stress–dislocation relations and the kinematics of the dynamic recrystallization, the flow stress constitutive equations of the work hardening‐dynamical recovery period and dynamical recrystallization period were established for 4130 steel, respectively. The validity of the model was demonstrated by comparing the experimental data with the numerical results. The agreement of this comparison is quite reasonable.     

Dynamic Recrystallization Behavior of Medium Carbon Cr-Ni-Mo-Nb Steel during Hot Deformation

Hot compression deformation behaviors of medium carbon Cr-Ni-Mo-Nb steel were investigated at deformation temperatures ranging from 1223 to 1423 Kand strain rates of 0.1,1and 5s^-1.Dynamic recovery（DRV）and dynamic recrystallization（DRX）were observed during the hot compression deformation.For all of the samples,DRX occurred at deformation temperatures above 1323 Kat different strain rates,while below 1223 K,no DRX was observed.The activation energy of the tested steel was determined as 386.06kJ/mol.The ratio of critical stress to peak stress and the ratio of critical strain to peak strain were 0.835 and 0.37,respectively.Kinetic equations interpreting the DRX behavior of the tested steel were proposed,and the corresponding parameters including the volume fraction and the average grain size were determined.Moreover,the microstructures induced under different deformation conditions were analyzed.     

Hot Deformation Behavior of GCr15 Steel

 Hot deformation behavior of GCr15 (ASTM 52100) steel was investigated using single-hit compression tests on Gleeble-1500 simulator at the temperature range of 850-1100 ℃ and strain rate range of 0. 1-10 s-1. The flow stress constitutive equation of GCr15 steel during hot deformation was determined by stress-strain curves analysis on the basis of the hyperbolic sine equation. And the models of dynamic recrystallization fraction and dynamic recrystallization grain size of GCr15 steel were established by the measured curves and microstructure observation in different experimental conditions. The mean activation energy and the time exponent of dynamic recrystallization kinetics equation in the range of experimental conditions were determined to be 356. 2 kJ/mol and 2. 12, respectively. Meanwhile, the flow stress model was also established by the method of allocating flow stress curve with three main stress values, the saturation stress, the steady state stress and the stress when strain is 0. 1. The flow stress curves predicted by the developed models under different deformation conditions are in good agreements with the measured ones.     

超低碳13Cr-5Ni-2Mo马氏体不锈钢热变形行为及本构关系

 利用Gleeble-3800热模拟试验机对超低碳13Cr-5Ni-2Mo马氏体不锈钢进行单道次高温压缩试验,研究其在900～1 200 ℃、0.1～50 s-1条件下的热变形行为,并讨论了不同变形条件下的微观组织演变规律;基于Sellars双曲正弦模型构建了超低碳13Cr-5Ni-2Mo 马氏体不锈钢的高温流变应力本构方程。研究结果表明,变形温度越高、应变速率越低,则流变应力越小,峰值应变也越小,微观组织由动态回复型向动态再结晶型转变,并且晶粒逐渐长大、粗化。在高温区变形,随着应变速率的升高,动态再结晶晶粒明显细化。所建立的本构方程具有较高的精确度,能反映超低碳13Cr-5Ni-2Mo 马氏体不锈钢的高温变形力学行为,可为热加工数值模拟研究提供参考。     

钒对低硅含磷系TRIP钢热变形行为的影响

通过分析不同变形温度及应变速率下低硅含磷系TRIP钢高温流变曲线的变化规律,建立了本构关系,并分析了合金元素钒对其影响。结果表明,添加0.19%钒,由于固溶钒原子的拖曳作用,使动态再结晶激活能提高~6%,同时推迟了动态再结晶的发生,使σc/σp和εc/εp值均有所提高。通过回归得到无钒钢和含钒钢的峰值应力和临界应力、峰值应变和临界应变与lnZ的关系。     

双相不锈钢2205铸态组织的热变形研究

研究了工业连铸双相不锈钢2205在不同温度和应变速率下的热变形过程。通过单道次热模拟压缩试验分析了铸态2205流变应力与温度和应变速率的关系,计算出铸态2205的热变形激活能Q=599 kJ/mol,说明铸态2205热加工性能较差。组织分析显示,两相之间变形不协调是相界微裂纹产生的根本原因。     

热变形和加速冷却对低碳微合金钢组织的影响

利用Gleeble-1500热模拟实验机研究了热变形和加速冷却工艺对3种低碳微合金钢组织演变的影响,结果表明,在再结晶或未再结晶温区实施1道次变形的晶粒细化效果不如2道次形次的效果明显,在再结晶和再结晶温区实施4道次变形可以得到更细的组织,配合较高的冷却速度可以形成部分针状铁素体组织。随着冷却速度的提高,组织变得更细,并且针状铁素体的数量增加。在相近的变形和冷却条件下,碳、锰含量较高的试样具有更细的组织。     

含铌微合金化热轧多相钢的控轧控冷工艺

通过热轧试验研究了两阶段轧制+层流冷却、空冷、超快冷的TMCP工艺对高硅铌钢、高硅Nb-Ti钢、低硅Nb-Ti钢显微组织和力学性能的影响。结果表明,控轧控冷后的试验钢含有铁素体、贝氏体、马氏体以及少量残余奥氏体的混合组织。在控轧控冷工艺参数相近的情况下,高硅铌钢、高硅Nb-Ti钢、低硅Nb-Ti钢的抗拉强度依次减小,其伸长率和强塑积依次增大。低硅Nb-Ti钢的伸长率和强塑积分别达到了41%、25 256 MPa.%的最大值。