Abstract

Spalling in tantalum has been observed in an experiment aiming at testing an antiproton production target prototype at CERN’s HiRadMat Facility. The experiment consisted in impacting 47 intense and high-energy proton beams onto a target equipped with ten cylindrical cores made of tantalum of Ø8 mm by 16 mm. Each of these proton beam impacts induced a sudden rise of temperature in the bulk of the Ta cores around 1800 °C in 0.9 μs leading to the excitation of a vibration mode which exposed their material to compressive-to-tensile pressures ranging from 2 GPa to 9 GPa, with pressure rates up to 20 GPa/μs. Post-irradiation analyses such as neutron tomography and metallographic examination of the cores, revealed the creation of voids in the bulk of the tantalum cores ranging from to 2 μm to 1 mm in diameter. These voids present a non-uniform size and density distribution within the cores, with limited growth and coalescence in areas subjected to higher temperatures and tensile pressures. Grain-growth due to a fast, thermally-induced, recrystallization has been also observed in some zones. In this work, we present a detailed characterization of the unique thermal and mechanical load that has induced this spall process by means of Finite Element and hydrocode simulations, together with post-experiment microscope and EBSD observations of the Ta rods. This analysis suggests that spall-induced void growth and coalescence is enhanced in the temperature and pressure window of 1300-1800 °C and 3-6.5 GPa, whereas is restrained at temperatures and tensile pressures above 2000 °C and 6.5 GPa. In addition, the analysis suggests that full thermal-recrystallization in tantalum can take place when exposed to temperatures above 2000 °C for less than 2 s. Four different hypotheses to explain the observed void size distribution trends are presented.

Highlights

  • The present study deals with the appearance of voids observed in the bulk of tantalum rods after exposing them to high dynamic stresses induced by high-energy proton beam impacts

  • Window regime in which growth and coalescence of voids is limited: areas exposed to the temperatures above 2000 ◦C and tensile pressures above 6.5 GPa. This corresponds to radial zones 1–2 for cores no. 4–6, where average voids diameter observed are within 18–40 μm. These depicted temperature and pressure windows associated to each regime have to be considered as tendency estimates since the analysis presents some features that shall be taken into account: there is a limited number of sliced samples to provide extended statistics of void distribution, in addition to uncertainties in their exact cutting position as well as in the potential influence of the discretization in steps of 0.5 mm, which is arbitrary

  • The HRMT-42 experiment exposed ten tantalum rods to 47 high energy (440 GeV/c momentum) proton pulse impacts. Each of these proton impacts induced a sudden rise of temperature in the bulk of such rods, with the subsequent excitation of a mode of vibration that exposed them to oscillating compressive-totensile pressures of several gigapascals

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Summary

Introduction

The present study deals with the appearance of voids observed in the bulk of tantalum rods after exposing them to high dynamic stresses induced by high-energy proton beam impacts. As presented in the current study, this is not the case of the HRMT-42 target core for several reasons: (i) The load comes from the bulk material, being highly hydrostatic, (ii) the strain state is mostly triaxial, (iii) tensile stresses are due to a mode excitation, that subjects the core to a series of hundreds of compression–tension oscillations, and (iv) these dynamic processes take place at temperatures well above 1000 ◦C The observation of these voids by the neutron tomography led to the target opening, core extraction and subsequent tantalum slicing for metallographic inspection combining optical microscope (OM) and Electron backscatter diffraction (EBSD) measurements (Fornasiere, 2020).

Conditions experienced by the tantalum cores
Thermal-transient analysis of the target progressive heating
Dynamic response of the cores
Post-experiment examinations of the Ta cores
OM images of the voids
Presence of recrystallization and comparison with pristine material
Findings
Discussion of the results and conclusions
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