Abstract

For ductile metals, the process of dynamic fracture occurs through nucleation, growth and coalescence of voids. The stress required to nucleate these voids is inferred from the velocimetry data (using the acoustic approach) and termed as the spall strength. This is a key parameter that is used to evaluate a material’s susceptibility to damage and failure. However, it is also well recognized that the dynamic parameters used to generate the shock state such as pulse duration, tensile strain-rate and peak stress coupled with material microstructure itself affect the material response in a complex manner. Yet, it is impossible to capture all this information by assessing only the spall strength measured from simple one-dimensional Photon Doppler Velocimetry measurements. Although, there exist widely used corrections proposed by Kanel et. al. that allow for the inclusion of some of these complexities into the measured spall strength but still does not take the microstructure into account. In this work, we propose another scheme for normalization of spall strength with a damage area to capture the complexities included in the damage and failure process especially pertaining to microstructure. We will also demonstrate the application of this scheme by applying to examples of materials such as Copper, Copper-24 wt%Ag, Copper-15 wt% Nb and additively manufactured 316L SS.

Highlights

  • Multiple notions of strength may be applied to a given material depending on the loading conditions

  • The development of microstructurally-aware predictive models for spallation is predicated on quantification of both the damage mechanism as well as the kinetics and volume within the sample over which this energy is dissipated

  • Work by Escobedo et al investigated four different grain size ranging from 30-200 μm in copper to study the effect of grain size on the spall strength and total nucleated damage within the samples [17]

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Summary

Introduction

Multiple notions of strength may be applied to a given material depending on the loading conditions. The simplest way to generate dynamic loading conditions in a material involves high velocity impact with a flyer This gives rise to a compression or shock wave, of a given amplitude, in the material and the flyer. The material is driven into tension in the specific region of intersection leading to the creation of damage in the form of voids in ductile materials, which grow and coalesce leading to failure under sufficiently large tension Parameters such as the peak stress, pulse duration, pulse shape, tensile strain-rate associated with the shock wave can all be controlled to some extent by altering either the flyer thickness and material or using high explosives or lasers to generate shock in the material [2, 3]. These loading parameters have complex interactions with the microstructure of a material

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