Abstract

It has long been known that iron undergoes a phase transformation from body-centered cubic/ α structure to the metastable hexagonal close-packed/ ε phase under high pressure. However, the interplay of line and planar defects in the parent material with the transformation process is still not fully understood. We investigated the role of twins, dislocations, and Cottrell atmospheres in changing the crystalline iron structure during this phase transformation by using Monte Carlo methods and classical molecular dynamics simulations. Our results confirm that embryos of ε -Fe nucleate at twins under hydrostatic compression. The nucleation of the hcp phase is observed for single crystals containing an edge dislocation. We observe that the buckling of the dislocation can help to nucleate the dense phase. The crystal orientations between the initial structure α -Fe and ε -Fe in these simulations are 110 b c c | | 0001 h c p . The presence of Cottrell atmospheres surrounding an edge dislocation in bcc iron retards the development of the hcp phase.

Highlights

  • Understanding the behavior of iron under extreme conditions is important for geophysicists, astrophysicists and material scientists

  • This study aimed at clarifying the effect of 1/2h111i {110} edge dislocations, coherent twin boundaries and Cottrell atmospheres on the transition process, and the orientation relations between parent and daughter phases

  • We determined the effects of three common types of defects to the pressure-induced transformation in iron

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Summary

Introduction

Understanding the behavior of iron under extreme conditions is important for geophysicists, astrophysicists and material scientists. Shock-induced phase transformations provide insights into understanding meteoritic impacts and help to generate new materials with improved hardness properties, which are stable at ambient conditions. Under a pressure of 13 GPa [2], body-centered cubic iron (bcc/α-Fe), which is stable at room conditions with atomic packing factor (APF) of 0.68 and coordination number of 8, transforms to hexagonal close-packed iron (hcp/ε-Fe) by a diffusionless transformation process. The hcp phase in iron has a coordination number of 12 and APF of 0.74, the same as face-centered cubic iron (fcc/γ-Fe), which is a product of the austenization process. When the pressure is released, the dense phase transforms back to bcc iron exhibiting a decisive influence on the morphological properties of the material [4,9]

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