By A cura di Claudio Cesa
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Additional resources for Guida a Hegel
Dislocations 2004, special issue of Mater. Sci. Eng. A, vols. 400–401, 2005.  Z. ), Multiscale Materials Modeling, Woodhead Publishing, Abington, 2007.  P. ), Third International Conference on Multiscale Materials Modelling, MMM 2006, J. Comput. Aided Mater. , vol. 14 (Suppl. 1) 2007.  W. A. Moriarty, Phys. Rev. B 54 (1996) 6941; Comput. Mater. Sci. 9 (1998) 348.  S. A. Arias, Phys. Rev. Lett. 84 (2000) 1499.  C. I. Rao, Philos. Mag. A 81 (2001) 1305. I. Rao, C. Woodward, Philos.
As previously demonstrated in the case of Ta , the lowest energy kink pair in the absence of a preexisting APD has the character pln–nrp. In Ta at 28 Lin H. Yang et al. Ch. 02 eV used in microscale DD simulations to account for the observed yield stress . For this reason, we have adopted the pln–nrp kink pair as the appropriate model for kink-pair formation in bcc transition metals, and used it here for Ta, Mo, and V at both ambient and high pressures. To model an isolated pln or nrp kink accurately, we work at constant volume and set up the GFBC simulation cell in the form of a long compliant cylinder made up of unit disks of width b and radius 20b (for the atomistic region), and a total length 60–80b centered on the dislocation line.
Bulatov, S. Yip, J. Comput. Aided Mater. Des. 9 (2002) 99 and references therein. L. W. Jacobsen, Philos. Mag. 83 (2003) 365.  M. Mrovec, D. G. Pettifor, V. Vitek, Phys. Rev. B 69 (2004) 94115. A. X. N. H. Streitz, M. H. Yang, J. Mater. Res. 21 (2006) 563 and references therein.  L. Kubin, G. Canova, M. Condat, B. Devincre, V. Pointikis, Y. Brechet, Solid State Phenom. 23–24 (1992) 455.  M. P. R. Canova, Acta Mater. 46 (1998) 3221.  M. Tang, in: S. ), Handbook of Materials Modeling, vol.
Guida a Hegel by A cura di Claudio Cesa