Abstract
The mechanism of formation of a cellular dislocation structure in face-centered cubic (fcc) metal crystals subjected to shock compression at strain rates \(\dot \varepsilon \) > 106 s−1 has been considered theoretically within the dislocation kinetic approach based on the kinetic equation for the dislocation density (dislocation constitutive equation). A dislocation structure of the cellular type is formed in the case of a two-wave structure of the compression wave behind its shock front (elastic precursor). It has been found that, at pressures σ > 10 GPa, the dislocation cell size Λ c depends on the pressure σ and the density ρ G of geometrically necessary dislocations generated at the shock front according to the relationship Λ c ∼ ρ −n G ∼ σ−m, where n = 1/4–1/2, m = 3/4–3/2, and m = 1, for different pressures and orientations of the crystal. It has been shown that, in copper and nickel crystals with the shock loading axis oriented along the [001] direction, the cellular structure is not formed after reaching the critical pressures σ c equal to 31 and 45 GPa, respectively.
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References
L. E. Murr, Scr. Metall. 12, 201 (1978).
M. A. Meyers, F. Gregory, B. K. Kad, M. S. Schneider, D. H. Kalantar, B. A. Remington, G. Ravichandran, T. Boehly, and J. S. Wark, Acta Mater. 51, 1211 (2003).
M. S. Schneider, B. K. Kad, F. Gregory, D. H. Kalantar, B. A. Remington, and M. A. Meyers, Metall. Mater. Trans. A 35, 2633 (2004).
M. A. Meyers, H. Jarmakani, E. M. Bringa, and B. A. Remington, Dislocations in Solids, Ed. by J. P. Hirth and L. Kubin (Elsevier, Amsterdam, The Netherlands, 2009), Vol. 15, Chap. 89, pp. 96–197.
J. C. Crowhurst, M. R. Armstrong, K. B. Knight, J. M. Zaug, and E. M. Behymer, Phys. Rev. Lett. 107, 144302 (2011).
M. A. Shehadeh, H. M. Zbib, and T. Diaz De La Rubia, Philos. Mag. 85, 1667 (2005).
M. A. Shehadeh, E. M. Bringa, H. M. Zbib, J. M. McNaney, and B. A. Remington, Appl. Phys. Lett. 89, 171918 (2006).
F. R. N. Nabarro, Z. S. Basinski, and D. B. Holt, The Plasticity of Pure Single Crystals (Adv. Phys. 13, 192 (1964); Metallurgiya, Moscow, 1967).
Z. P. Luo, H. W. Zhang, N. Hansen, and K. Lu, Acta Mater. 60, 1322 (2012).
G. A. Malygin, S. L. Ogarkov, and A. V. Andriyash, Phys. Solid State 55(4), 780 (2013).
G. A. Malygin, S. L. Ogarkov, and A. V. Andriyash, Phys. Solid State 55(11), 2280 (2013).
C. S. Smith, Trans. AIME 212, 574 (1958).
M. A. Meyers, Scr. Metall. 12, 21 (1978).
G. A. Malygin, Phys.-Usp. 42(9), 917 (1999).
G. A. Malygin, Phys. Solid State 37(1), 1 (1995).
G. A. Malygin, S. L. Ogarkov, and A. V. Andriyash, Phys. Solid State 55(4), 787 (2013).
L. E. Murr, in Shock Waves and High-Strain-Rate Phenomena in Metals, Ed. by M. A. Meyers and L. E. Murr (Plenum, New York, 1981).
G. A. Malygin, Phys. Solid State 48(4), 693 (2006).
Y. Kawasaki, J. Phys. Soc. Jpn. 27, 142 (1974).
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Original Russian Text © G.A. Malygin, S.L. Ogarkov, A.V. Andriyash, 2014, published in Fizika Tverdogo Tela, 2014, Vol. 56, No. 6, pp. 1123–1130.
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Malygin, G.A., Ogarkov, S.L. & Andriyash, A.V. Mechanism of formation of cellular dislocation structures during propagation of intense shock waves in crystals. Phys. Solid State 56, 1168–1176 (2014). https://doi.org/10.1134/S1063783414060237
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DOI: https://doi.org/10.1134/S1063783414060237