The static color-Coulomb potential is calculated as the solution of a
non-linear integral equation. This equation has been derived recently
as a self-consistency condition which arises in the Coulomb Hamiltonia
n formulation of lattice gauge theory when the restriction to the inte
rior of the Gribov horizon is implemented. The potential obtained is i
n qualitative agreement with expectations, being Coulombic with logari
thmic corrections at short range and confining at long range. The valu
es obtained for the string tension and <lambda((MS))over bar> are in s
emi-quantitative agreement with lattice Monte Carlo and phenomenologic
al determinations.