材料科学
空隙(复合材料)
极限抗拉强度
复合材料
合金
应变率
冶金
作者
Dinh-Quan Doan,Te-Hua Fang,Tao-Hsing Chen,Thi-Xuyen Bui
标识
DOI:10.1016/j.engfracmech.2021.107848
摘要
The figure shows the atomistic configurations of mono-crystal AlCrCuFeNi 2 high-entropy alloy samples with a pre-void (a1) and a pre-inclusion (b1) at the strain value of 0.2: von Mises shear strain (a2 and b2), atomic phase (a3 and b3). • The mechanical parameters are decreased under increasing the void size and reducing the strain rate. • There exists a critical value of the mechanical parameters at the tension of sample with an inclusion size of 15 Å. • The deformation behavior reveals that the void and inclusion are the main cause of initial strain. • The HCP phase of inclusion exhibits relatively unstable, demonstrated by a rapid phase transformation of inclusion. The effects of various void sizes, inclusion sizes, and strain rates on the mechanical response, deformation behavior, and failure mechanism of AlCrCuFeNi 2 high-entropy alloy samples with a pre-void/inclusion under the tension are investigated via the molecular dynamics. The results reveal that there exists a critical value of mechanical parameters such as the tensile strength and Young’s modulus in the tension of sample with an inclusion size of 15 Å, where the mechanistic parameters are changed. Meanwhile, the mechanical parameters decrease under increasing the void size and reducing the strain rate. The deformation behavior discloses that the void and inclusion are the principal cause of initial strain, and the shear bands are propagated inside the workpiece along the direction of an angle of 45° related to the tensile axis. The transformation from the FCC phase to other structures such as HCP and amorphous has occurred during deformation. Also, the HCP phase of inclusion shows relatively unstable, which is demonstrated by a rapid phase transformation of inclusion under a small strain. Finally, the dislocation evolution mechanism exhibits that it begins to nucleate around the void and inclusion, and the dislocations are then moved to free surfaces with increased strain.
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