Multiscale Richtmyer-Meshkov instability experiments to isolate the strain rate dependence of strength

Abstract

Theoretical analysis of Richtmyer-Meshkov instability (RMI) experiments for solid strength shows that the strain rate for a given shock should be inversely proportional to the length scale of the sine wave perturbations when η0k, the nondimensional amplitude to wavelength ratio, is held fixed. To isolate the effect of strain rate on strength, free-surface RMI specimens of annealed copper were prepared with three perturbation regions with the same η0k but different length scales, characterized by the wavelength λ varying by a factor of 4.9 from 65 to 130 to 320µm. Three such targets with different fixed η0k′s were impacted to a shock pressure of 25 GPa, and the instability evolution was measured with photon Doppler velocimetry. Strengths estimated by comparing hydrocode simulation to the data increased from 700 to 1200 MPa as λ decreased. The different η0k targets exercised increasing amounts of plastic strain yet showed no evidence of strain hardening. Physical regime sensitivity analysis determined that for 320−65µm wavelength perturbations, the effective strain rates increased from 8.7×106 to 3.3×107s−1, a factor of 3.8. Thus, the predicted strain rate scaling was mostly achieved but slightly suppressed by increased strength at higher rates. The RMI strength estimates were plotted against constitutive testing data on copper from the literature to show striking evidence of the strength upturn at higher strain rates. Published by the American Physical Society 2024

Metals strengthen with increasing temperature at extreme strain rates

“…For comparison, under quasistatic conditions, annealed copper would have a typical strength on the order of 70 MPa (ref. 37 ) and under extreme conditions involving shock (such as Richtmyer–Meshkov instability tests 38 ), strengths up to 1,000 MPa have been inferred. The present value between these limits represents substantial rate-hardening, but no superimposed effect of shock or high pressure.…”