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1.
目前关于变形温度、应变速率等因素对流变应力的影响有大量的研究报道,而对温变形条件下碳含量的增加对流变应力的影响规律还缺乏系统研究.基于此开展起始组织为马氏体的不同淬火碳钢温变形流变行为研究.结果表明,在较低温度和较高应变速率(600℃,0.1~1s-1)下,流变应力随碳含量的增加而增大;在较高温度和较低应变速率下(700℃,0.01~0.001 s-1),流变应力在高碳范围内呈下降趋势.碳的质量分数低于0.78%时,淬火碳钢温变形激活能随碳含量的增加而降低;碳的质量分数高于0.78%时,淬火碳钢温变形激活能随碳含量的增加而增加.在相同变形条件下,能量耗散效率最大值随着碳含量的增加呈增大趋势.  相似文献   

2.
采用Gleeble-1500热模拟机高温压缩试验,研究5A01铝合金在应变速牢为0.01~1s-1、变形温度为350~450℃条件下的流变行为,并利用光学显微镜分析合金在不同压缩条件下的组织形貌特征.结果表明:应变速率和变形温度的变化强烈影响合金流变应力的大小,流变应力随变形温度升高而降低,随应变速率提高而增大.采用双曲正弦形式ARRHENIUS的关系来描述5A01铝合金高温压缩变形时的流变应力行为,获得的材料常数A、α、n和Q分别为0.068 31 s-1、0.009 4 MPa-1、2.708 9和161.14 kJ/mol:在应变速率为0.01 s-1及变形温度低于400℃条件下变形时,5A01铝合金组织为纤维组织,而当变形温度升高到450℃时,再结晶程度很高,出现大量等轴晶.  相似文献   

3.
采用Gleeble-1500D热模拟机进行热压缩变性试验,研究7N01铝合金在变形温度为340 ~460℃、应变速率为0.01~ 10.00 s-1条件下的流变应力行为.结果表明:变形温度和应变速率对合金流变应力有显著影响,流变应力随变形温度的升高而降低,随应变速率的增加而升高;合金在低应变速率(0.01,0.10,1.00s-1)时主要为动态回复软化机制,而在高应变速率(10.00 s-1)时出现动态再结晶软化;7N01铝合金的高温流变行为可用Zener-Hollomon参数描述.  相似文献   

4.
文章研究工业纯铝在等温压缩过程中流变应力特征和微观组织的演变。结果表明:在同一应变速率0.01/s下,变形温度为220℃和300℃时,真应力-真应变曲线呈稳态特征,材料只发生了动态回复,当T≥380℃时,发生了动态再结晶;任同一变形温度460℃,不同应变速率(1/s,0.1/s,0.01/s,0.001/s)下变形时发生了动态再结晶;动态再结晶机制是连续动态再结晶和几何动态再结晶,其真应力-真应变曲线呈单峰特征?  相似文献   

5.
 在Gleeble 3500热模拟试验机上,用热压缩方法研究了原始组织为层片状珠光体的高碳钢在温度为913~973 K、应变速率为001~10 s-1范围内的温变形行为。结果表明:实验条件下,流变应力及峰值应变随变形温度的降低和应变速率的提高而增大。另外,回归出了高碳钢的峰值应力及峰值应变与变形温度、应变速率之间的关系,得到了相应的形变激活能和温变形方程式,为高碳钢的温变形工艺优化提供了理论依据。  相似文献   

6.
采用真空感应熔炼法制备了医用Ti-50. 7%Ni合金(原子数分数), 测试了铸态合金的成分、相变点、微观组织和硬度, 并采用Gleeble-3800热模拟实验机在变形温度750~950℃、应变速率0. 001~1 s-1, 应变量为0. 5的条件下对Ni-Ti合金进行高温压缩变形, 分析其流动应力变化规律, 建立了高温塑性变形本构关系和热加工图.结果表明: 当变形温度减小或应变速率增大时, Ni-Ti合金的流动应力会随之增大.应变速率为1 s-1时, 合金的真应力-真应变曲线呈现出锯齿状特征.根据热加工图, 获得了Ni-Ti合金的加工安全区和流变失稳区, 进而确定其合理的热变形温度范围为820~880℃, 真应变速率低于0. 1 s-1.从而为制定镍钛合金的锻造工艺参数提供理论和数据基础.   相似文献   

7.
采用Gleeble-3500热模拟试验机进行热压缩试验,研究了Cu-3.6Ni-1.0Si合金在变形温度为500~950℃、变形速率为0.01~10s。状态下的热塑性变形行为。根据应力.应变数据,构建了cu.3.6Ni-1.0Si合金热塑性变形过程中流变应力与变形温度、变形速率等加工参数之间的本构关系方程。经过参数拟合与优化,得到Cu-3.6Ni-1.0Si合金在650~950℃之间、热变形过程的应力.应变速率关系方程。试验结果及分析表明,Cu-3.6Ni-1.0Si合金加热保温及开轧温度应以950℃为上限,终轧温度以高于7000C为宜,不能低于650℃,热轧加工变形速率范围在0.1~10s-1之间。  相似文献   

8.
Fe16Mn0.6C TWIP钢流变应力和临界动态再结晶行为   总被引:1,自引:1,他引:0  
 利用Thermecmastor-Z热模拟实验机,得到了Fe16Mn0.6C TWIP钢在变形温度850~1150℃,应变速率0.03~30s-1条件下热压缩变形的真应力应变曲线。进而研究了变形温度、应变速率对Fe16Mn0.6C流变应力和临界动态再结晶行为的影响规律。结果表明,850~1150℃范围内Fe16Mn0.6C热变形的峰值应力随温度的升高而降低,随着应变速率的增大而升高;且在应变速率为0.03 s-1和30 s-1出现明显的应力峰值,材料发生了动态再结晶。最后采用线性回归方法计算出Fe16Mn0.6C的高温变形流变应力本构方程,得出热变形激活能为469kJ/mol;并通过应变硬化速率与流变应力曲线求出了该钢种动态再结晶临界条件与Z参数之间的关系。  相似文献   

9.
以氢化钛粉为原料,采用粉末冶金法-热等静压法制备高温钛合金Ti-1100,并进行了等温压缩试验,通过压缩样品应力应变曲线进行压缩变形行为分析,再结合Arrhenius双曲正弦本构模型建立热压缩本构方程.通过应力应变曲线分析,发现应变速率在0.01 s-1时,所有样品在加工硬化后均表现出稳态流变行为;而应变速率为1 s-1、温度在900℃或1000℃时,流变应力随着变形达到稳态流变状态后,呈增加趋势.应变速率为0.01、0.1、1 s-1时的热压缩变形激活能分别为96、165、232 kJ/mol.硬度测试结果表明显微硬度随温度和应变速率增加稍有降低趋势,当温度为950℃,应变速率为0.1 s-1时,合金的硬度普遍较小,热加工性能最佳.  相似文献   

10.
摘要:为了探究Custom 450钢的动态再结晶行为,采用Gleeble 3800热模拟试验机,在变形温度为1050~1200℃和应变速率为0.01~10s-1的变形条件下开展了单道次等温压缩试验。研究结果显示,在变形温度为1050~1200℃和应变速率为1.0~10s-1的变形范围内,钢虽发生了完全的动态再结晶,但应力应变曲线未表现出明显的应力峰值;钢的动态再结晶的晶粒尺寸随着变形温度的升高和应变速率的降低逐渐增大,当应变速率为001s-1时,动态再结晶晶粒发生长大。采用双曲正弦函数构建了Cutom 450钢的热变形方程,并建立了钢的动态再结晶动力学、临界应变、峰值应变及动态再结晶晶粒尺寸与Zener Holloman参数的定量关系。  相似文献   

11.
 In order to investigate the effect of initial microstructure on warm deformation behavior, some specimens of 45 steel were annealed and some quenched. Then the specimens were isothermally compressed on a Gleeble 3500 machine. The deformation temperature range was 550 to 700 ℃ and the strain rate range was 0.001 to 0.1 s-1. An optical microscope (OM) and a transmission electron microscope (TEM) were used to study the microstructures. The results show that the microstructure of annealed specimens is ferrite and pearlite and that of quenched specimens is martensite. The flow stress of quenched specimens is higher than that of annealed ones at 550 ℃ when strain rates are greater than 0.001 s-1. However, at 600 to 700 ℃ and strain rate of 0.001 s-1, the whole flow curves of quenched specimens are below that of annealed ones. Under the rest conditions, the flow stress of quenched specimens is higher at the beginning of compression and then the opposite is true after the strain is greater than a critical value. The microstructure examination proves that the tempering and dynamic recrystallization easily occur in the specimens with martensite during warm compression, which results in the above phenomena.  相似文献   

12.
关键词:双相不锈钢; 流变曲线; 本构方程; 热加工图  相似文献   

13.
在Gleeble-3500热模拟试验机上对Ti-25Al-14Nb-2Mo-1Fe合金进行了等温恒应变速率压缩试验,研究了在变形温度为950~1 100℃,应变速率为0.001~1 s-1,最大变形程度为50%的条件下合金的热压缩变形流变应力行为与微观组织演变。结果表明:Ti-25Al-14Nb-2Mo-1Fe合金的流变应力对变形温度和应变速率均较为敏感,其流变应力曲线具有应力峰值、流变软化和稳态流变的特征。在变形温度为950℃,应变速率为0.001~0.1 s-1的条件下,Ti-25Al-14Nb-2Mo-1Fe合金的热变形特性为片层组织球化,其热变形机制可用晶界分离球化模型进行解释说明;在变形温度为1 000~1 100℃,应变速率为1 s-1的条件下,材料只发生了动态回复现象;在变形温度为1 050~1 100℃,应变速率为0.001~0.1 s-1的条件下,材料发生了动态再结晶现象。  相似文献   

14.
Various isothermal compression tests are carried out on an ultrahigh carbon steel(1.2% C in mass percent), initially quenched or spheroidized,using a Gleeble-3500system.The true stress is observed to decrease with increasing temperature and decreasing strain rate.The true stress of the initially quenched steel is lower than that of the initially spheroidized steel at high deformation temperature(700℃)and low deformation strain rate(0.001s-1).The value of the deformation activation energy(Q)of the initially quenched steel(331.56kJ/mol)is higher than that of the initially spheroidized steel(297.94kJ/mol).The initially quenched steel has lower efficiency of power dissipation and better processability than the initially spheroidized steel.The warm compression promotes the fragmentation and the spheroidization of lamellar cementites in the initially quenched steel.The fragmentation of lamellar cementites is the spheroidizing mechanism of the cementites in the initially quenched steel.Results of transmission electron microscope investigation showed that fine grains with high angle boundaries are obtained by deformation of the initially quenched steel.  相似文献   

15.
 The hot deformation characteristics of GH4720Li alloy were studied at the temperature of 1100-1170 ℃ and strain rate of 001-1 s-1 using Gleeble hot compression tests. True stress-true strain curves and deformation microstructures were investigated. Constitutive equation was established using the hyperbolic law. Processing map for hot working was also developed on the basis of the variations of efficiency of power dissipation with temperature and strain rate. The results show that dynamic recrystallization is the dominant softening mechanism during hot deformation. Fully recrystallized grain is obtained at strain of 07 above 1130 ℃, and coarsening occurs above 1150 ℃. The mean deformation activation energy is determined to be 512 kJ/mol. According to the low activation energy value, high dissipation efficiency parameter and fine recrystallized microstructure, 1130 ℃ is chosen as the hot working temperature for GH4720Li alloy.  相似文献   

16.
The hot deformation behavior of as-cast AISI M2high-speed steel containing mischmetal(RE)has been investigated on a Gleeble-3500simulator in the temperature range of 1 000-1 150℃and strain rate range of 0.01-10 s-1 at true strain of 1.0.The mechanical behavior has been characterized using stress-strain curve analysis,kinetic analysis,processing maps,etc.Metallographic investigation was performed to evaluate the mechanism of flow instability.The results show that the deformation activation energy decreases with increasing deformation temperature; the efficiency of power dissipation increases with decreasing strain rate and increasing temperature;flow instability is observed at low-to-medium temperature and higher strain rate region when the strain is smaller,but extends to lower strain rate and high temperature regions with the increment of strain,in which it is manifested as flow localization near the grain boundary.Hot deformation equations and processing maps are obtained.The optimal processing window is suggested and the deformation mechanism is dynamic recrystallization(DRX).  相似文献   

17.
为制定中温中压容器用钢13MnNiMoR的热加工工艺提供理论依据并实现其工业化生产,利用单道次热压缩模拟实验研究了变形温度(900~1150℃)和应变速率(0.01~1s~(-1))对其热变形行为的影响.结果表明:当应变速率低于0.1s~(-1)时,新晶粒有足够的时间进行形核和长大,奥氏体容易发生动态再结晶;当变形温度降低或应变速率增加时,实验钢在变形过程中主要发生动态回复,流变应力也随之提高.基于测定的流变应力曲线,通过拟合得到实验钢在热变形时的应力指数为4.29,动态再结晶激活能为319kJ/mol,据此建立了13MnNiMoR钢在高温变形时的热加工方程.  相似文献   

18.
 通过Nb V Ti和Nb V Ti Mo两种微合金钢在高温(td=900~1 100 ℃)和不同应变速率(=001~10 s-1)下的单道次压缩模拟试验,研究了热变形参数对两种微合金钢的动态再结晶过程的影响,求出动态再结晶形变激活能及相关参数,建立了热变形方程,并通过对比,分析了钼对微合金钢动态再结晶的影响。结果表明:含钼钢的动态再结晶更困难。这是因为钼的自扩散系数大,致使钢具有更高的动态再结晶激活能。  相似文献   

19.
为了获得C HRA 5钢轧制生产的最佳工艺参数,采用Gleeble 3800热力模拟试验机对C HRA 5钢进行了双道次热压缩实验。实验在变形温度范围为900~1100℃,应变速率范围为001~1s-1,道次间隙时间分别为1、5、15、30s的条件下获得C-HRA -5钢的真应力 应变曲线。采用0.2%补偿法计算得到了软化分数,且软化分数随变形温度的升高和应变速率的增大而增加。通过线性回归分析得到了MDRX的动力学方程。建立的C-HRA-5钢热加工图表明材料在1000~1100℃的范围内变形稳定。此外,道次间隙时间为5s时,C-HRA-5钢在较低温度下进行第2道次压缩的过程中不会出现失稳。  相似文献   

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