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Molecular dynamics (MD) simulation of uniaxial tension of some single-crystal cubic metals at nanolevel

机译:某些单晶立方金属在纳米水平单轴拉伸的分子动力学(MD)模拟

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Molecular Dynamics (MD) simulations of uniaxial tension at nanolevel have been carried out at a constant rate of loading (500 ms{sup}(-1)) on some single-crystal cubic metals, both FCC (Al, Cu, and Ni) and BCC (Fe, Cr, and W) to investigate the nature of deformation and fracture. Failure of the workmaterials due to void formation, their coalescence into nanocracks, and subsequent fracture or separation were observed similar to their behavior at macroscale. The engineering stress-strain diagrams obtained by the MD simulations of the tensile specimens of various materials show a rapid increase in stress up to a maximum followed by a gradual drop to zero when the specimen fails by ductile fracture. The radius of the neck is found to increase with an increase in the deformation of the specimen and to decrease as the ductility of the material decreases. In this investigation, the strain to fracture is observed to be lower with the BCC materials than FCC materials. In the case of BCC crystals, no distinct linear trend in the engineering stress-strain characteristics is observed. Instead, rapid fluctuations in the force values were observed. If the drop in the force curves can be attributed to the rearrangement of atoms to a new or modified crystalline structure, it appears that BCC materials undergo a significant change in their structure and subsequent realignment relative to the FCC materials, as previously reported in the literature. While good correlation is found between the D- and α-parameters of the Morse potential with the ultimate strength and the strain to failure for the FCC metals, no such correlation is found for the BCC metals. From this, it appears that Morse potentials may not represent the deformation behavior of BCC metals as accurately as FCC metals and alternate potentials may need to be considered. 2001 Elsevier Science Ltd. All rights reserved.
机译:在某些单晶立方金属(FCC(Al,Cu和Ni))上以恒定加载速率(500 ms {sup}(-1))进行了纳米级单轴张力的分子动力学(MD)模拟。和BCC(铁,铬和钨)来研究变形和断裂的性质。观察到工作材料由于空隙形成,它们聚结成纳米裂纹以及随后的破裂或分离而失效,这与它们的宏观行为相似。通过各种材料的拉伸试样的MD模拟获得的工程应力-应变图显示,应力迅速增加直至最大值,然后在试样因延性断裂而破裂时逐渐下降至零。发现颈部的半径随着样品变形的增加而增加,并且随着材料的延展性降低而减小。在这项研究中,观察到BCC材料的断裂应变低于FCC材料。对于BCC晶体,在工程应力-应变特性中没有观察到明显的线性趋势。相反,观察到力值的快速波动。如果力曲线的下降可归因于原子重新排列为新的或修饰的晶体结构,则BCC材料似乎在结构上发生了重大变化,并相对于FCC材料发生了随后的重新排列,如先前在文献中报道的那样。尽管在FCC金属的摩尔斯电势的D参数和α参数与极限强度和破坏应变之间发现了良好的相关性,但对于BCC金属却没有发现这种相关性。由此看来,莫尔斯电势可能不能像FCC金属那样准确地代表BCC金属的变形行为,因此可能需要考虑替代电势。 2001 Elsevier ScienceLtd。保留所有权利。

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