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首页> 外文期刊>Journal of Materials Engineering and Performance >High-Temperature Deformation and Ductility of a Modified 5083 Al Alloy
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High-Temperature Deformation and Ductility of a Modified 5083 Al Alloy

机译:改性5083铝合金的高温变形和延展性

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The high-temperature deformation of a 5.5% Mg and 0.6% Ca modified 5083 aluminum alloy was investigated in the temperature range from 573 to 723 K at strain rates in the range of 10?5-10?1 s?1. Ca was added to form an insoluble second phase in the range of temperatures tested to improve the high-temperature characteristics of this alloy. It was shown that the deformation behavior of the alloy could be divided into two regions with stress exponent, n of 3.5 and 13 at low and high strain rates, respectively. The apparent activation energy determined in both regions suggested that the deformation process is diffusion controlled in both regions. The slightly high value of n at the low-strain rate region (viscous glide) was attributed to the presence of threshold stress. The values of threshold stress showed an exponential increase with decreasing temperature and a dependence with an energy term Qo = 16.5 kJ mol?1. Analysis of creep data in terms of threshold stress and using diffusivity of Mg in normalizing the strain rates, revealed two types of deformation behavior. At high values of normalized strain rate $ ({ifmmodeexpandafterdotelseexpandafter.fi{upvarepsilon }kT} mathord{left/ {vphantom {{ifmmodeexpandafterdotelseexpandafter.fi{varepsilon }kT} {DGb}}} right. kern-0em} {DGb} > 10^{{ - 9}} ), $ a high value of stress exponent of n = 10 is observed, and the exponential law creep takes place. At low normalized strain rates ≤10?9, the n value is 3 and the true activation energy, Q, is equal to 123 kJ mol?1 suggesting viscous glide of dislocations as rate-controlling mechanism. Enhanced ductility has been observed in the region of viscous-glide controlled deformation as a result of high strain-rate sensitivity.
机译:研究了5.5%Mg和0.6%Ca改性的5083铝合金在573至723 K温度范围内,应变速率为10?5 -10?1 s?1 。添加钙以形成在测试温度范围内的不溶性第二相,以改善该合金的高温特性。结果表明,在低应变速率和高应变速率下,合金的变形行为可以分为应力指数为n的两个区域,n分别为3.5和13。在两个区域中确定的表观活化能表明,变形过程在两个区域中均受扩散控制。在低应变率区域(粘性滑移)处的n值稍高归因于阈值应力的存在。阈值应力值随温度降低呈指数增加,并且与能量项Qo = 16.5 kJ mol?1 呈依赖性。根据阈值应力和使用Mg扩散率归一化应变率进行的蠕变数据分析显示出两种类型的变形行为。在高归一化应变率下,$({ifmmodeexpandafterdotelseexpandafter.fi {upvarepsilon} kT} mathord {left / {vphantom {{ifmmodeexpandafterdotelseexpandafter.fi {varepsilon} kT} {DGb}}} right。kern-0em} {DGb}> 10 ^ {{-9}}),观察到高应力指数n = 10,并且发生了指数规律蠕变。在低归一化应变率≤10?9 时,n值为3,真实活化能Q等于123 kJ mol?1 ,表明位错的粘性滑移是速率控制的机制。由于高应变率敏感性,在粘性滑行控制的变形区域观察到了增强的延展性。

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