Abstract

High-purity Zr has been observed to undergo a phase transformation from the α-phase to the hexagonal ω-phase under high pressure generated either statically or by shock loading. The transition pressure from α-Zr to ω-Zr at 300 K is 2.10 GPa. The main aim of this research was to determine the conditions of α-Zr in ω-Zr transformation and the state of stresses after the high-pressure pressing and sintering of zirconium powders. Commercially acquired zirconium powders of 99.9% and 98.8% purity were used in this study. Qualitative and quantitative phase analysis of the materials was carried out using X-ray diffraction. The materials were statically pressed and sintered using a Bridgman-type toroidal apparatus at under 4.0 and 7.8 GPa. After pressing, the transformation proceeded for the zirconium powder containing 98.8% purity (with hydrides admixture) but did not occur for the high-purity zirconium powders with 99.9% purity. The zirconium powders were sintered using the HPHT (High Pressure—High Temperature) method at temperatures of 1273 K and 1473 K. The transformation proceeded for both powders. The highest contribution of the ω-Zr phase was obtained in the zirconium (98.8% purity with the hydrides contents) sintered for 1 min at a temperature of 1473 K and a pressure of 7.8. The ω-phase content was 87 wt.%. The stress measurement was performed for the pressed and sintered materials using the sin2ψ X-ray diffraction method. The higher sintering temperature resulted in a decrease of the residual stresses in the ω-Zr phase for the sintered zirconium. The higher levels of stress limited the transformation of the α-Zr phase into the ω-Zr phase. Investigated materials characterized by higher compressive macrostresses were also typical of the greater stability of the ω-Zr phase at high temperatures.

Highlights

  • Zirconium crystallises in a hexagonal close-packed structure known as the α phase

  • The main aim of the current research was to determine the conditions of α-Zr to ω-Zr transformation and the state of stress after high-pressure pressing and sintering of zirconium powders

  • Produced high-purity zirconium powders from two different sources were used in this study

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Summary

Introduction

Zirconium crystallises in a hexagonal close-packed (hcp) structure known as the α phase. At atmospheric pressure with temperature up to 1135 K, it transforms into a body-centred cubic (bcc) structure commonly referred to as the β phase. With the increase of pressure, α-Zr (P63/mmc) transforms into another hexagonal structure, not close-packed and named the ω phase (P6/mmm), which has three atoms per unit cell. The ω-Zr can be considered as a metastable phase in ambient conditions when pressure is released. It undergoes the reverse transformation to the α phase at temperatures above 470 K [1,2]. The phase transition from α-Zr to β-Zr at atmospheric

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