In a simulation, the potential energy of an atom, i {\displaystyle i} , is given by3
where r i j {\displaystyle r_{ij}} is the distance between atoms i {\displaystyle i} and j {\displaystyle j} , ϕ α β {\displaystyle \phi _{\alpha \beta }} is a pair-wise potential function, ρ β {\displaystyle \rho _{\beta }} is the contribution to the electron charge density from atom j {\displaystyle j} of type β {\displaystyle \beta } at the location of atom i {\displaystyle i} , and F {\displaystyle F} is an embedding function that represents the energy required to place atom i {\displaystyle i} of type α {\displaystyle \alpha } into the electron cloud.
Since the electron cloud density is a summation over many atoms, usually limited by a cutoff radius, the EAM potential is a multibody potential. For a single element system of atoms, three scalar functions must be specified: the embedding function, a pair-wise interaction, and an electron cloud contribution function. For a binary alloy, the EAM potential requires seven functions: three pair-wise interactions (A-A, A-B, B-B), two embedding functions, and two electron cloud contribution functions. Generally these functions are provided in a tabularized format and interpolated by cubic splines.
Daw, Murray S.; Mike Baskes (1984). "Embedded-atom method: Derivation and application to impurities, surfaces, and other defects in metals". Physical Review B. 29 (12). American Physical Society: 6443–6453. Bibcode:1984PhRvB..29.6443D. doi:10.1103/PhysRevB.29.6443. /wiki/Murray_S._Daw ↩
Daw, Murray S.; Foiles, Stephen M.; Baskes, Michael I. (1993). "The embedded-atom method: a review of theory and applications". Mat. Sci. Eng. Rep. 9 (7–8): 251. doi:10.1016/0920-2307(93)90001-U. /w/index.php?title=Stephen_M._Foiles&action=edit&redlink=1 ↩
"Pair - EAM". LAMMPS Molecular Dynamics Simulator. Retrieved 2008-10-01. http://lammps.sandia.gov/doc/pair_eam.html ↩