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High-temperature deformation mechanisms and processing maps of equiatomic CoCrFeMnNi high-entropy alloy

机译:高温变形机制和赤素COCRFEMNI高熵合金的处理地图

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The hot compressive deformation mechanism and processing maps of the equiatomic FCC CoCrFeMnNi high-entropy alloy (HEA) were studied in the temperature range between 1023 and 1323 K and in the strain rate range between 10(-3) and 10 s(-1). At high strain rates above 1 s(-1), strain hardening was dominant even at the very high temperature of 0.84T(m) which may be attributed to the sluggish diffusion coefficient and low stacking fault energy of the CoCrFeMnNi HEA, leading to suppression of dynamic recovery. According to the processing maps, the best condition for hot working was near 10(-3)s(-1) at 1323 K. Power-law breakdown and unstable flow occurred at low temperatures and high strain rates where the strain hardening was pronounced. The activation energy for plastic flow measured in the power-law creep regime when considering the dependence of elastic modulus on temperature was 312.2 kJ/mol; this value is close to the activation energy for the weighted diffusion coefficient calculated by weighting the contribution of each element in the CoCrFeMnNi HEA (284 kJ/mol). The size and fraction of the dynamically recrystallized grains increased as the strain rate decreased and the temperature increased, as in conventional metals. Both discontinuous dynamic recrystallization and continuous dynamic recrystallization (CDRX) occurred. CDRX became more distinct as the temperature increased. The deformation mechanism and behavior of the CoCrFeMnNi HEA were very similar to those of FCC pure metals in terms of the stress exponent and the effect of the stacking fault energy and diffusivity on the creep rates.
机译:在1023和1323k的温度范围内研究了赤脂FCC COCRFEMENNI高熵合金(HEA)的热压缩变形机制和加工图,在10(-3)和10s(-1)之间的应变速率范围内。在高于1 s(-1)的高应变率下,即使在0.84t(m)的高温下,菌株硬化也占主导地位,这可能归因于COCRFEMNI HEA的缓慢扩散系数和低堆叠故障能量,导致抑制动态恢复。根据处理图,在1323k的高温下,热工作的最佳条件在10(-3)℃(-1)接近10(-3),在低温下发生功率 - 律衰弱和不稳定流动,并且在菌株硬化发音的高应变速率下发生。在考虑弹性模量对温度的依赖性时,在动力法蠕变制度中测量的塑性流动的激活能量为312.2kJ / mol;该值接近通过加权COCRFEMNI HEA(284kJ / mol)中每个元素的贡献来计算加权扩散系数的激活能量。随着应变速率降低并且温度增加,动态再结晶晶粒的尺寸和分数增加,如常规金属。发生不连续的动态再结晶和连续的动态再结晶(CDRX)。随着温度的增加,CDRX变得更加明显。 COCRFEMNNI HEA的变形机制和行为与压力指数的纯净金属的变形机制和行为与堆叠故障能量和蠕变率扩散率的效果非常相似。

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