Shear Modulus and Yield Stress Change with Pressure and Temperature
DOI:
https://doi.org/10.14738/aivp.105.13102Abstract
It is well known that the shear modulus (G) and the yield stress (Y) of metals increase with pressure (P) and decrease with temperature (T). Steinberg [1], in his popular compendium of dynamic material properties, assumes for Y/Y0(P,T)=G/G0(P,T) linear relations based on tests at ambient conditions. But recent tests of high-pressure dynamic loading of certain metals yielded results that generally deviate from Steinberg’s equations. Here we use a different approach to estimate G/G0(P,T). As a first approximation we let G/G0 follow from the assumption of constant Poisson ratio (n). This leads to G/G0=K/K0, where K is the isentropic bulk modulus. With this assumption we compute the longitudinal sound speed of tantalum along its principal Hugoniot curve, and compare the result to recent measurements. There is a slight disagreement which we correct by assuming (second approximation) that Poisson’s ratio decreases slightly with pressure, and increases slightly with temperature. As K is always available in a hydrocode run from the equation of state, so are therefore also G/G0 and Y/Y0.
References
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H.S. Park et al. (17 authors), Experimental results of tantalum material strength at high pressure and high strain rate, shock compression of condensed matter 2011, AIP conf. proc. 1426, 1371-1374 (2012).
S.D. Rothman, R.J. Edwards, T.J. Vogler and M.D. Furnish, Inferring the high-pressure strength of copper by measurement of longitudinal sound speed in a symmetric impact and release experiment, Shock compression of condensed matter 2011, AID conf. proc. 1426, 104-107 (2012).
P.A. Rigg, R.J. Scharff and R.S. Hixon, Sound speed measurements in tantalum using the front surface impact th th technique, 18 APS-SCCM and 24 AIRAPT, J. of Phys. Conf. series 500 (2014).
J. Hu et al. (9 authors), Sound velocity measurements of tantalum under shock compression in the 10-110GPa range, J. Appl. Phys. 111, 033511 (2012).
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