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

机译:等原子CoCrFeMnNi高熵合金的高温变形机理及加工图

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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:研究了等原子FCC CoCrFeMnNi高熵合金(HEA)在1023和1323 K之间的温度范围以及10(-3)和10 s(-1)之间的应变率范围内的热压缩变形机理和加工图。 。在高于1 s(-1)的高应变速率下,即使在0.84T(m)的非常高的温度下,应变硬化仍占主导地位,这可能归因于CoCrFeMnNi HEA的扩散系数低和堆垛层错能低,导致抑制动态恢复。根据加工图,在1323 K时,热加工的最佳条件是在10(-3)s(-1)附近。在低温和高应变速率下,发生明显的应变硬化时,发生了幂律分解和不稳定的流动。考虑到弹性模量对温度的依赖性,在幂律蠕变状态下测得的塑性流动的活化能为312.2 kJ / mol;该值接近于通过加权CoCrFeMnNi HEA中每种元素的贡献而计算出的加权扩散系数的活化能(284 kJ / mol)。与传统金属一样,随着应变速率的降低和温度的升高,动态再结晶晶粒的尺寸和分数也随之增加。发生了不连续动态重结晶和连续动态重结晶(CDRX)。随着温度升高,CDRX变得更加独特。就应力指数以及堆垛层错能和扩散率对蠕变速率的影响而言,CoCrFeMnNi HEA的变形机理和行为与FCC纯金属非常相似。

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