Using density-functional theory, we investigate fluctuations of the ground-
state energy of spin-polarized, disordered quantum dots in the metallic reg
ime. To compare to experiment, we evaluate the distribution of addition ene
rgies and find a convolution of the Wigner-Dyson distribution, expected for
noninteracting electrons, with a narrower Gaussian distribution. The width
of the Gaussian is accurately given by the fluctuations in the screened Co
ulomb interaction between a pair of electrons at the Fermi energy.