The average mass density profile measured in the Canadian Network for
Observational Cosmology cluster survey is well described with the anal
ytic form rho(r) = Ar-1(r + a(rho))(-2), as advocated on the basis of
n-body simulations by Navarro, Frenk, & White. The predicted core radi
i are a(rho) = 0.20 (in units of the radius where the mean interior de
nsity is 200 times the critical density) for an Omega = 0.2 open cold
dark matter model and a(rho) = 0.26 for a flat Omega = 0.2 model, with
little dependence on other cosmological parameters for simulations no
rmalized to the observed cluster abundance. The dynamically derived lo
cal mass-to-light ratio, which has little radial variation, converts t
he observed light profile to a mass profile. We find that the scale ra
dius of the mass distribution, 0.20 less than or equal to a(rho) less
than or equal to 0.30 (depending on modeling details, with a 95% confi
dence range of 0.12-0.50), is completely consistent with the predicted
values. Moreover, the profiles and total masses of the clusters as in
dividuals can be acceptably predicted from the cluster rms line-of-sig
ht velocity dispersion alone. This is strong support for the hierarchi
cal clustering theory for the formation of galaxy clusters in a cool,
collisionless, dark-matter-dominated universe.