Compositional effects in the liquid Fe–Ni–C system at high pressure

We performed molecular dynamics simulations based on density functional theory to systematically investigate the Fe–Ni–C system including (1) pure Fe and Ni; (2) binary Fe–Ni, Fe–C, and Ni–C; and (3) ternary Fe–Ni–C liquid compositions at 3000 K and three simulation volumes corresponding to pressure ( P ) up to 83 GPa. Liquid structural properties, including coordination numbers, are analyzed using partial radial distribution functions. Self-diffusion coefficients are determined based on the atomic trajectories and the asymptotic slope of the time-dependent mean-square displacement. The results indicate that the average interatomic distance between two Fe atoms ( r Fe–Fe ) decreases with P and is sensitive to Ni ( X Ni ) and C ( X C ) concentration, although the effects are opposite: r Fe–Fe decreases with increasing X Ni , but increases with increasing X C . Average r Fe–C and r Ni–C values also decrease with increasing X Ni and generally remain constant between the two lowest P points, corresponding to a coordination change of carbon from ~ 6.8 to ~ 8.0, and then decrease with additional P once the coordination change is complete. Carbon clustering occurs in both binary (especially Ni–C) and ternary compositions with short-range r C-C values (~ 1.29 to ~ 1.57 Å), typical for r C-C in diamond and graphite. The self-diffusion results are generally consistent with high- P diffusion data extrapolated from experiments conducted at lower temperature ( T ). A subset of additional simulations was conducted at 1675 and 2350 K to estimate the effect of T on diffusion, yielding an activation enthalpy of ~ 53 kJ/mol and activation volume of ~ 0.5 cm 3 /mol.