Within the local-density approximation, the interlayer binding and the elec
tronic properties of graphite and ''graphitic'' Si have been determined. Fo
r graphite, the optimized equilibrium lattice constant agrees well with the
experimental value. The role of 2p(z) orbitals (pi states) turned out to b
e twofold: contributing a major part to the binding of C atoms within basal
planes, and giving a minor contribution in the form of the overlay of 2p(z
) orbitals, which leads to weaker interlayer binding. The interlayer bindin
g attributed to the interaction of C-C atoms in different layers yields the
calculated binding energy as a function of the lattice constants and is ap
plied to fit an additional Lennard-Jones-type empirical potential to be inc
luded in classical molecular-dynamics simulations. In contrast to that, the
calculated energy pathways for "graphitic" Si show an extended region of m
inima within the range of a = 3.84 Angstrom and for c varying from 5.50 to
6.68 Angstrom having two lower levels, which indicates chemisorption and ph
ysical absorption. The obtained electronic density distribution demonstrate
s that the atoms in "graphitic" Si tend to form a structure with metal-like
electron distributions. Nevertheless, a Lennard-Jones potential with restr
icted validity may be fitted to describe the weak long-range behavior, too.