2014
DOI: 10.1134/s1028335814060056
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Phase transition behind a shock front in polycrystalline copper

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Cited by 5 publications
(12 citation statements)
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“…As we had showed earlier [5,6] the average grain size in nanocrystalline copper exerts a minor effect on the dependences of the shock wave velocity on the piston velocity and of the pressure on the density behind the front. For the material with the grain size of about 2 nm, the temperature behind the front is 10% higher than for the materials with greater grain sizes.…”
Section: Structural State Of Copper Under Shock Conditionsmentioning
confidence: 95%
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“…As we had showed earlier [5,6] the average grain size in nanocrystalline copper exerts a minor effect on the dependences of the shock wave velocity on the piston velocity and of the pressure on the density behind the front. For the material with the grain size of about 2 nm, the temperature behind the front is 10% higher than for the materials with greater grain sizes.…”
Section: Structural State Of Copper Under Shock Conditionsmentioning
confidence: 95%
“…In this case we observe the effect which was called virtual melting in [8]. The mechanism of this crystal structure damage is related to the fact that, due to the nonhydrostatic character of loading in bulk behind the shock front, high tangential stresses arise, which are related to the deviator part of the stress tensor [5,6,8]. During compression, the tangential stresses achieve the maximum about 0.2 GPa for a calculation presented on Fig.…”
Section: Structure Of Shock Front In Titaniummentioning
confidence: 99%
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