稀土Ce对4Cr5MoSiV1钢热变形行为的影响

利用Gleeble-3800热模拟试验机对不含稀土和含稀土的4Cr5MoSiV1钢进行高温热变形模拟试验,变形温度为1 100～1 200℃,变形速率为0.1～3 s^-1,总变形程度为60%.根据得到的真应力-应变数据,对比试验钢在应变量为30%时的变形抗力值,并分析变形后的显微组织.结果表明：4Cr5MoSiV1钢在研究的试验条件下均发生了动态再结晶;相同变形条件下,含稀土4Cr5MoSiV1钢的变形抗力比不含稀土4Cr5MoSiV1钢增大12～36 MPa;稀土Ce的添加细化了再结晶晶粒,提高了试验钢变形抗力,推迟了动态再结晶的发生.稀土含量为0.012 0%的4Cr5MoSiV1钢适宜的热加工参数为变形温度1 100℃,变形速率0.1 s^-1.     

82B高碳钢热变形行为研究

采用单道次热压缩实验方法,在Thermomaster-Z型热模拟试验机上模拟高碳钢高速线材热轧变形过程动态再结晶行为,测定82B高碳钢在变形温度为800～1 100℃、变形速率为0.1～50 s-1、变形程度为0～0.60条件下的真应力-应变曲线,利用曲线特征值确定高应变速率下的变形激活能,根据实验结果分析动态再结晶变形条件,建立动态再结晶状态图。     

Al-1Mn-1Mg合金热变形过程中的动态软化行为研究

研究了Al-1Mn-1Mg合金不同变形下的流变应力曲线和微观结构特征,探讨了该铝材在热变形过程中的动态软化行为。结果表明,应变速率为0.1 s-1时,若变形温度较低,则发生了动态回复;若变形温度高于723 K,产生明显的动态再结晶;变形温度为673 K时,在低应变速率条件下,产生动态再结晶,应变速率高于0.1 s-1,软化过程具有动态回复和动态再结晶的混合特征。当应变速率高于5.0 s-1时,产生几何动态再结晶。     

铌对弹簧钢60Si2MnA动态再结晶的影响

在Gleeble-1500热模拟实验机上研究含铌弹簧钢的动态再结晶行为,用透射电镜对铌的析出物进行观察,并分析铌对弹簧钢动态再结晶的影响。结果表明,含铌弹簧钢易发生动态再结晶,在温度为850-1050℃、变形速率为0.1-20 s^-1条件下均发生动态再结晶;在变形速率为5 s^-1的条件下,60Si2MnA动态再结晶的发生推迟50℃左右;在低温情况下,铌推迟60Si2MnA动态再结晶的主要原因是Nb（C,N）的析出及其钉扎作用。     

316LN热变形行为及动态再结晶晶粒的演变规律

采用热压缩试验研究了316LN不锈钢在温度1250℃-900℃,应变速率0．005s^-1～0．5s^-1,变形程度50％条件下的变形行为和组织演变;分析了变形参数对应力-应变曲线的影响规律,计算获得了该钢热变形应力指数和激活能;并通过动态再结晶晶粒演变规律的研究,建立了该钢热变形动态再结晶图,以及动态再结晶晶粒演变规律模型。研究结果可为316LN不锈钢锻造过程晶粒细匀化的控制提供科学的依据。     

基于平面应变热模拟的3Cr2Mo钢板材动态再结晶动力学分析

采用平面应变法研究3Cr2Mo钢板材动态再结晶过程。在Gleeble-3500模拟试验机上进行平面应变热模拟试验,应变速率为0.1～50 s-1,热变形温度为950～1 100℃。用平滑处理后的流变应力数据分析热变形过程中动态再结晶的演化过程,结合平面应变实验数据回归推导得到动态再结晶的激活能为309.05 kJ/mol。引入Zener-Hollomon参数,基于流变应力曲线,分析峰值应变的模拟方程。根据不同应变速率和温度下的流变应力结果,研究3Cr2Mo钢的动态再结晶转化过程,用Avrami方程建立动态再结晶动力学方程。通过动态再结晶转化体积分数实验数据和模型计算值的对比,验证了构建的动态再结晶动力学方程可较好地预测平面应变过程中的动态再结晶过程。     

含硼、钴9%Cr耐热钢的热变形行为

热机械模拟试验是研究新型含硼、钴9%Cr耐热钢材料的有效方法,试验在温度T为900～1050℃、应变速率ε·为0.001～10s-1条件下进行,确定材料的热变形参数。利用相关试验数据建立基于峰值应力的新型含硼、钴9%Cr耐热钢本构方程,并以动态材料模型和Murthy失稳准则为理论基础,绘制材料的热加工图。试验结果表明:含硼、钴9%Cr耐热钢在高温下有较好的塑性,变形温度和变形速率对其高温塑性影响不大,但对动态再结晶的影响比较明显。将试验后的试样进行抛光腐蚀,并利用光学显微镜对含硼、钴9%Cr耐热钢在不同变形条件下的组织演变进行观察,进而研究动态再结晶生成及变化规律。     

SPCC钢塑性变形中动态再结晶的数学模型与模拟分析

利用热模拟设备Gleeble-1500D,对SPCC钢在不同变形量下的真应力-应变曲线进行了测定,并结合微观组织观察,确定了SPCC钢动态再结晶的数学模型,研究并分析了变形参数对动态再结晶晶粒的影响.通过DEFORM有限元软件对SPCC钢的热压缩过程进行模拟计算.分析了不同变形条件对晶粒尺寸的影响.模拟计算结果很好地与实验结果相吻合,为进一步研究这种钢的动态再结晶提供了一定的参考依据.     

热轧镁合金AZ31B板材的超塑性变形行为与机制

研究工业态热轧 AZ31B镁合金板材的超塑性及变形机制,在应变温度为 723K,应变速率为 1× 10-3s-1的实验条件下,其最大断裂延伸率达到 216%,应变速率敏感指数达 0.36;研究结果表明:晶界滑动( GBS)是工业态热轧 AZ31B镁合金超塑性的主要变形机制,变形初期有动态再结晶发生,断裂是由晶界处形成的空洞不断长大、连接而引起的.     

挤压态MB15镁合金的显微组织与力学性能研究

针对MB15镁合金在挤压温度为648 K,应变速率0.001s-1,挤压比9∶1的条件下进行挤压变形研究,通过对其变形后的组织特征分析和拉伸性能测试,光学显微组织研究表明MB15镁合金在挤压过程中发生动态再结晶;透射电镜组织研究表明机械孪晶、位错滑移和动态再结晶是材料变形的典型特征;扫描电镜组织研究表明挤压后的材料塑性明显增强.挤压变形后的MB15镁合金沿挤压方向的抗拉强度提高39.5％,屈服强度提高89.4％,延伸率提高25％,弹性模量提高6.7％.     

Deformation Behavior of 6063 Aluminum Alloy During High-Speed Compression

The deformation behavior characteristics of 6063 aluminum alloy were studied experimentally by isothermal compression tests on a Gleeble- 1500 thermal-mechanical simulator. Cylindrical specimens of 14mm in height and 10mm in diameter were compressed dynamically at temperatures ranging from 473 to 723K and at higher strain rntes from 5 to 30s^-1. It is fouud that the flow curves not only depend on the strain rate and temperature but nlso on the dynamic recovery aud recrystallization behavior. The results show that the flow stress decreased with the increase of temperature, while increased with the increase of strain rate. The discontinuous dynamic recrystallization （DDRX） may take place at a high strain rate of 20s^-1 under the tested conditions. At 30s^-1 , the flow curve can exhibit,flow softening due to the effect of temperature rise that raised the temperature by aboat 32K in less than 0.05s.     

Hot deformation behavior and flow stress model of F40MnV steel

Single hit compression tests were performed at 1 223-1 473 K and strain rate of 0.1-10 s-1 to study hot deformation behavior and flow stress model of F40MnV steel. The dependence of the peak stress, initial stress, saturation stress, steady state stress and peak stain on Zener-Hollomon parameter were obtained. The mathematical models of dynamic recrystallization fraction and grain size were also obtained. Based on the tested data, the flow stress model of F40MnV steel was established in dynamic recovery region and dynamic recrystallization region, respectively. The results show that the activation energy for dynamic recrystallization is 278.6 kJ/mol by regression analysis. The flow stress model of F40MnV steel is proved to approximate the tested data and suitable for numerical simulation of hot forging.     

Constitutive Modeling and Dynamic Recrystallization Mechanisms of an Ultralow-carbon Microalloyed Steel During Hot Compression Tests

The hot deformation behavior of an ultralow-carbon microalloyed steel was investigated using an MMS-200 thermal simulation test machine in a temperature range of 1 073-1 373 K and strain rate range of 0.01-10 s~(-1).The results show that the flow stress decreases with increasing deformation temperature or decreasing strain rate.The strain-compensated constitutive model based on the Arrhenius equation for this steel was established using the true stress-strain data obtained from a hot compression test.Furthermore,a new constitutive model based on the Z-parameter was proposed for this steel.The predictive ability of two constitutive models was compared with statistical measures.The results indicate the new constitutive model based on the Z-parameter can more accurately predict the flow stress of an ultralow-carbon microalloyed steel during hot deformation.The dynamic recrystallization (DRX) nucleation mechanism at different deformation temperatures was observed and analyzed by transmission electron microscopy (TEM),and strain-induced grain boundary migration was observed at 1 373 K/0.01 s~(-1).     

Flow stress behavior and processing map of Al-Cu-Mg-Ag alloy during hot compression

The hot deformation behavior of Al-Cu-Mg-Ag was studied by isothermal hot compression tests in the temperature range of 573-773 K and strain rate range of 0.001-1 s^-1 on a Gleeble 1500 D thermal mechanical simulator. The results show the flow stress of Al-Cu-Mg-Ag alloy increases with strain rate and decreases after a peak value, indicating dynamic recovery and recrystallization. A hyperbolic sine relationship is found to correlate well the flow stress with the strain rate and temperature, the flow stress equation is estimated to illustrate the relation of strain rate and stress and temperature during high temperature deformation process. The processing maps exhibit two domains as optimum fields for hot deformation at different strains, including the high strain rate domain in 623-773 K and the low strain rate domain in 573-673 K.     

Hot deformation behavior of FGH96 superalloys

1. Introduction Precipitation-hardened nickel-based superalloys have been widely used as high-temperature structural materials in gas turbine engine applications for more than 50 years. Because powder metallurgy (P/M) process produces a fine, homogenous a…     

形变和热处理温度对纯铌管材组织和性能的影响

通过对纯铌挤压管坯和冷变形管材的显微组织及力学性能的分析,研究了形变程度和热处理温度对材料的组织和性能的影响.试验结果表明,经800～850℃挤压的纯铌管坯,完全再结晶退火温度约为1 150℃,挤压管坯经87%冷变形后,完全再结晶退火温度约为1 100℃;纯铌管材完全再结晶退火温度随着形变总加工率的增加,基本呈下降趋势,且影响比较明显.     

Plastic deformation behavior of ZK60 magnesium alloy with addition of neodymium

The hot deformation simulation of a ZK60 magnesiuln alloy at different temperatures from 373 to 673 K and different strain rates of 0.1, 0.01 and 0.002 s^-1 was studied by using the Gleebe-1500 simulator. The plastic deformation behavior was measured and the deformation activation energy was calculated. The microstructures of ZK60 magnesium alloy with an addition of neodymium during the deformation process were observed by using Polyvar-MET optical microscope and Tecnai G^2 20 TEM. The results show that the working hardening, the dynamic recovery and the dynamic recrystallization occur during the plastic deformation process at different temperatures and strain rates. The dynamic recrystallization starts when the temperature is over 473 K and the DRX grain size after hot deformation is only 5-10 μm. So the refined grains improve both the tensile strength and the elongation of alloys at room temperature. Neodymium is added into the alloy and a precipitate phase Mg12Nd that impedes the movement of dislocations is formed, which benefits to increasing mechanical properties of ZK60 magnesium alloy.     

Dynamic recrystallization behavior of 35CrMo structural steel

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Static recrystallization behavior of Inconel 718 alloy during thermal deformation

The softening behavior of Inconel 718 alloy at different temperatures was studied using twostage interrupted compression method on Gleeble1500D thermal stimulator, and the 2% offset method was applied to analyze the experimental dates. Finally, the static recrystallization fraction was obtained. At the same times, optical microscope(OM) and transmission electron microscopy(TEM) were employed to investigate the microstructure characteristic. The experimental results showed that the recrystallization was more sensitive to temperature than holding time. The recrystallization process finished quickly above 1 050 ℃, and significantly prolonged below 1 025 ℃. Additionally, the dynamical model of static recrystallization follows the Avrami equation. The nucleating mechanism was characterized by bulging at grain boundary and merging of sub-grain.