New PDF release: Guida a Hegel

By A cura di Claudio Cesa

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Dislocations 2004, special issue of Mater. Sci. Eng. A, vols. 400–401, 2005. [7] Z. ), Multiscale Materials Modeling, Woodhead Publishing, Abington, 2007. [8] P. ), Third International Conference on Multiscale Materials Modelling, MMM 2006, J. Comput. Aided Mater. , vol. 14 (Suppl. 1) 2007. [9] W. A. Moriarty, Phys. Rev. B 54 (1996) 6941; Comput. Mater. Sci. 9 (1998) 348. [10] S. A. Arias, Phys. Rev. Lett. 84 (2000) 1499. [11] C. I. Rao, Philos. Mag. A 81 (2001) 1305. I. Rao, C. Woodward, Philos.

As previously demonstrated in the case of Ta [13], 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 [21]. 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. [18] 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. [20] L. Kubin, G. Canova, M. Condat, B. Devincre, V. Pointikis, Y. Brechet, Solid State Phenom. 23–24 (1992) 455. [21] M. P. R. Canova, Acta Mater. 46 (1998) 3221. [22] M. Tang, in: S. ), Handbook of Materials Modeling, vol.

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Guida a Hegel by A cura di Claudio Cesa


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