Estimation of Metal Strength at Very High Rates Using Free-Surface Richtmyer–Meshkov Instabilities

Recently, Richtmyer–Meshkov Instabilities (RMI) have been proposed for studying the average strength at strain rates up to at least 10 7 /s. RMI experiments involve shocking a metal interface that has initial sinusoidal perturbations. The perturbations invert and grow subsequent to shock and may arr...

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Veröffentlicht in:Journal of Dynamic Behavior of Materials 2017-06, Vol.3 (2), p.189-202
Hauptverfasser: Prime, Michael B., Buttler, William T., Buechler, Miles A., Denissen, Nicholas A., Kenamond, Mark A., Mariam, Fesseha G., Martinez, John I., Oró, David M., Schmidt, Derek W., Stone, Joseph B., Tupa, Dale, Vogan-McNeil, Wendy
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Sprache:eng
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Zusammenfassung:Recently, Richtmyer–Meshkov Instabilities (RMI) have been proposed for studying the average strength at strain rates up to at least 10 7 /s. RMI experiments involve shocking a metal interface that has initial sinusoidal perturbations. The perturbations invert and grow subsequent to shock and may arrest because of strength effects. In this work we present new RMI experiments and data on a copper target that had five regions with different perturbation amplitudes on the free surface opposite the shock. We estimate the high-rate, low-pressure copper strength by comparing experimental data with Lagrangian numerical simulations. From a detailed computational study we find that mesh convergence must be carefully addressed to accurately compare with experiments, and numerical viscosity has a strong influence on convergence. We also find that modeling the as-built perturbation geometry rather than the nominal makes a significant difference. Because of the confounding effect of tensile damage on total spike growth, which has previously been used as the metric for estimating strength, we instead use a new strength metric: the peak velocity during spike growth. This new metric also allows us to analyze a broader set of experimental results that are sensitive to strength because some larger initial perturbations grow unstably to failure and so do not have a finite total spike growth.
ISSN:2199-7446
2199-7454
DOI:10.1007/s40870-017-0103-9