Anton-Schmidt equation of state
The Anton-Schmidt equation is an empirical equation of state for crystalline solids, e.g. for pure metals or intermetallic compounds.[1] Quantum mechanical investigations of intermetallic compounds show that the dependency of the pressure under isotropic deformation can be described empirically by
- .
Integration of leads to equation of the state for the total energy. The energy required to compress a solid to volume is
which gives
- .
The fitting parameters and are related to material properties, where
- is the bulk modulus at equilibrium volume .
- correlates with the Grüneisen parameter .[2][3]
However, the fitting parameter does not reproduce the total energy of the free atoms.[4]
The total energy equation is used to determine elastic and thermal material constants in quantum chemical simulation packages.[4][5]
See also
References
- ↑ Mayer, B.; Anton, H.; Bott, E.; Methfessel, M.; Sticht, J.; Harris, J.; Schmidt, P.C. (2003). "Ab-initio calculation of the elastic constants and thermal expansion coefficients of Laves phases". Intermetallics 11 (1): 23–32. doi:10.1016/S0966-9795(02)00127-9. ISSN 0966-9795.
- ↑ Otero-de-la-Roza, et al., Gibbs2: A new version of the quasi-harmonic model code. Computer Physics Communications 182.8 (2011): 1708-1720. DOI: 10.1016/j.cpc.2011.04.016
- ↑ Jund, Philippe, et al., Physical properties of thermoelectric zinc antimonide using first-principles calculations., Physical Review B 85.22 (2012) .
- 1 2 Atomic Simulation Environment documentation of the Technical University of Denmark, Department of Physics
- ↑ Gilgamesh chemical software documentation of the Department of Chemical Engineering of Carnegie Mellon University
This article is issued from Wikipedia - version of the Wednesday, March 09, 2016. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.