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粉末冶金Ti-22Al-25Nb合金动态再结晶临界表征模型
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作者 马雄 赵帅元 +2 位作者 张建伟 梁晓波 程云君 《热加工工艺》 CSCD 北大核心 2017年第18期95-99,103,共6页
对粉末冶金Ti-22Al-25Nb合金进行变形温度995~1075℃、应变速率0.001~1 s-1条件下的热模拟压缩试验。研究了该合金在热加工过程中的流动应力与变形机制,根据Poliak和Jonas提出的临界动力学条件和温度补偿应变速率因子Z,构建了粉末冶金Ti... 对粉末冶金Ti-22Al-25Nb合金进行变形温度995~1075℃、应变速率0.001~1 s-1条件下的热模拟压缩试验。研究了该合金在热加工过程中的流动应力与变形机制,根据Poliak和Jonas提出的临界动力学条件和温度补偿应变速率因子Z,构建了粉末冶金Ti-22Al-25Nb合金的动态再结晶临界表征模型。结果表明,确定了发生动态再结晶所需激活能为410.172 k J/mol。此外,ε_p可通过Z参数的指数函数形式表示,即:ε_p=0.00011Z^(0.15)。ε_c与临界应力(σ_c)随着变形温度的升高和应变速率的降低而减小,这说明较小的Z参数能促进粉末冶金Ti-22Al-25Nb合金动态再结晶行为的发生。 展开更多
关键词 TI-22AL-25NB合金 流变力学行为 动态再结晶 临界模型
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Dynamic recrystallization kinetics of as-cast AZ91D alloy 被引量:18
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作者 徐岩 胡连喜 孙宇 《Transactions of Nonferrous Metals Society of China》 SCIE EI CAS CSCD 2014年第6期1683-1689,共7页
The flow behavior and dynamic recrystallization(DRX) behavior of an as-cast AZ91 D alloy were investigated systematically by applying the isothermal compression tests in temperature range of 220-380 ℃ and strain ra... The flow behavior and dynamic recrystallization(DRX) behavior of an as-cast AZ91 D alloy were investigated systematically by applying the isothermal compression tests in temperature range of 220-380 ℃ and strain rate range of 0.001-1 s^-1.The effect of temperature and strain rate on the DRX behavior was discussed.The results indicate that the nucleation and growth of dynamic recrystallized grains easily occur at higher temperatures and lower strain rates.To evaluate the evolution of dynamic recrystallization,the DRX kinetics model was proposed based on the experimental data of true stress-true strain curves.It was revealed that the volume fraction of dynamic recrystallized grains increased with increasing strain in terms of S-curves.A good agreement between the proposed DRX kinetics model and microstructure observation results validates the accuracy of DRX kinetics model for AZ91 D alloy. 展开更多
关键词 AZ91D magnesium alloy compression flow behavior dynamic recrystallization behavior kinetics model
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铸态超级双相不锈钢S32750热变形过程的动态软化行为研究
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作者 武敏 郝文慧 +1 位作者 李建春 裴海祥 《太钢科技》 2013年第3期32-39,共8页
运用Gleeble-3800热模拟实验机在变形温度为950~1200℃、应变速率为0.1~25/s、真应变为0.1、0.5和1的条件下对S32750进行热压缩实验。结果表明,在950,1050℃、0.1/s变形时,流变曲线表现出不同于单相不锈钢的“类屈服平台”... 运用Gleeble-3800热模拟实验机在变形温度为950~1200℃、应变速率为0.1~25/s、真应变为0.1、0.5和1的条件下对S32750进行热压缩实验。结果表明,在950,1050℃、0.1/s变形时,流变曲线表现出不同于单相不锈钢的“类屈服平台”特征;当变形温度为1100~1200℃或应变速率为10/s、25/s时,流变曲线为典型的动态再结晶特征。微观组织演变显示,铁素体在各变形条件下均发生动态再结晶;奥氏体在低温区950℃变形时,发生动态回复;中温区1050℃变形时,小应变速率下(0.I/s)发生动态回复,大应变速率下(10/s)发生动态再结晶;高温区1200℃变形时,奥氏体发生动态再结晶。应变分配对S32750热变形过程中的组织演变影响显著。提高变形温度,增大应变量,可促进动态再结晶发生。 展开更多
关键词 超级双相不锈钢S32750流变力学行为 动态回复 动态再结晶
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Creep characteristic simulation of deep soft rock roadway and long-term mechanical analysis of lining support 被引量:3
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作者 ZHAO Tong-bin MA Yan-hua +1 位作者 TAN Yun-liang CHEN Yun-juan 《Journal of Coal Science & Engineering(China)》 2009年第2期193-196,共4页
By the generalized Kelvin creep model,rheological characteristics of deep softrock and long-term mechanical behaviors of support structures were simulated.Mechanicaldeformation characteristics of support structures un... By the generalized Kelvin creep model,rheological characteristics of deep softrock and long-term mechanical behaviors of support structures were simulated.Mechanicaldeformation characteristics of support structures under different lining circumstanceswere also analyzed on the basis of deducing the relationship between the generalizedKelvin creep model and implicit creep equations in ANSYS FEM software.The resultsshow that high stress of deep tunnels is the main factor in creep damage;the surroundingrock's deformation binding effect due to lining increases as the thickness increases but theeffect becomes very weak when it increases to a certain value;contact pressure on thelining decreases as its thickness decreases. 展开更多
关键词 deep soft rock generalized Kelvin model creep simulation lining structure
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Microstructure, morphology, crystallization and rheological behavior of impact polypropylene copolymer 被引量:4
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作者 SHANG-GUAN YongGang CHEN Feng ZHENG Qiang 《Science China Chemistry》 SCIE EI CAS 2012年第5期698-712,共15页
Impact polypropylene copolymer (IPC), named polypropylene catalloy, not only possesses excellent impact property, but also presents good rigidity. Its superior performances result from the complicated composition and ... Impact polypropylene copolymer (IPC), named polypropylene catalloy, not only possesses excellent impact property, but also presents good rigidity. Its superior performances result from the complicated composition and microstructure. In the present article, recent progress in the studies on microstructure, morphology, crystallization and rheological behavior of IPC is summarized, and findings of the authors and their collaborators are reported. In general, IPC is divided into three components, i.e., ethylene-propylene random copolymer (EPR), a series of different segment lengths ethylene-propylene copolymer (EbP) and propylene homopolymer. The reasonable macromolecular structures of EbP and a multilayered core-shell model of dispersed phase structure in IPC were proposed, in which the dispersed phase consists of an outer EbP shell, an inner EPR layer and an EbP core. It is found that the annealing at melt-state may lead to an abnormal phase inversion, and the phase inversion disappears when temperature cools down to room temperature. The cause of phase inversion is ascribed to the existence of EbP component, which results in the stronger activity of the dispersed phase. The crystalline structure and morphologic results confirm the formation of β-iPP in IPC. Furthermore, it is found that the ethylene content in IPC and cooling rate of the samples have an important influence on the formation of β-iPP. Based on the crystallization kinetics analyzed by Lauritzen-Hoffman theory, crystallization behavior of different IPC samples is discussed and it is proposed that the dilution effect of ethylene propylene copolymer has a more remarkable influence on surface nucleation than on crystal growth. In addition, annealing at high temperature can result in the changes of chain structure for IPC, and this instability is ascribed to the oxidative degradation and crosslink reaction mainly in iPP component. 展开更多
关键词 MICROSTRUCTURE MORPHOLOGY crystallization behavior rheological property impact polypropylene copolymer
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Mechanical behavior of pathological and normal red blood cells in microvascular flow based on modified level-set method
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作者 XiWen Zhang FangChao Ma +1 位作者 PengFei Hao ZhaoHui Yao 《Science China(Physics,Mechanics & Astronomy)》 SCIE EI CAS CSCD 2016年第1期66-74,共9页
The research of the motion and deformation of the RBCs is important to reveal the mechanism of blood diseases. A numerical method has been developed with level set formulation for elastic membrane immersed in incompre... The research of the motion and deformation of the RBCs is important to reveal the mechanism of blood diseases. A numerical method has been developed with level set formulation for elastic membrane immersed in incompressible fluid. The numerical model satisfies mass and energy conservation without the leaking problems in classical Immersed Boundary Method(IBM), at the same time, computing grid we used can be much smaller than the general literatures. The motion and deformation of a red blood cell(including pathological & normal status) in microvascular flow are simulated. It is found that the Reynolds number and membrane's stiffness play an important role in the transmutation and oscillation of the elastic membrane. The normal biconcave shape of the RBC is propitious to create high deformation than other pathological shapes. With reduced viscosity of the interior fluid both the velocity of the blood and the deformability of the cell reduced. With increased viscosity of the plasma both the velocity of the blood and the deformability of the cell reduced. The tank treading of the RBC membrane is observed at low enough viscosity contrast in shear flow. The tank tread fixed inclination angle of the cell depends on the shear ratio and viscosity contrast, which can be compared with the experimental observation well. 展开更多
关键词 red blood cell microvascular flow shear flow fluid-structure interaction level set
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