The Local Supercluster kinematic properties (the Local Group infall to
ward the Virgo Cluster and galaxy density distribution about the Virgo
Cluster) in various cosmological models are examined utilizing large-
scale N-body (PM) simulations (500(3) cells, 250(3) particles, and box
size of 400 h-1 Mpc) and are compared to observations. Five models ar
e investigated: (1) the standard, COBE-normalized CDM model with OMEGA
= 1, h = 0.5, and sigma8, = 1.05; (2) the standard HDM model with OME
GA = 1, h = 0.75, and sigma8 = 1; (3) the tilted CDM model with OMEGA
= 1, h = 0.5, n = 0.7, and sigma8 = 0.5; (4) a CDM + lambda model with
OMEGA = 0.3, lambda = 0.7, h = 2/3, and sigma8 = 2/3; (5) the PBI mod
el with OMEGA = 0.2, h = 0.8, x = 0.1, m = -0.5, and sigma8 = 0.9. Com
parison of the five models with the presently available observational
measurements (v(LG) = 85 - 305 km s-1 [with mean of 250 km s-1], DELTA
n(g)/n(g)BAR = 1.40 +/- 0.35) suggests that an open universe with OMEG
A approximately 0.5 (with or without lambda) and sigma8 approximately
0.8 is preferred, with OMEGA = 0.3-1.0 (with or without lambda) and si
gma8, = 0.7-1.0 being the acceptable range. At variance with some prev
ious claims based on either direct N-body or spherical nonlinear appro
aches, we find that a flat model with sigma8 approximately 0.7-1.0 see
ms to be reasonably consistent with observations. However, if one favo
rs the low limit of v(LG) = 85 km s-1, then an OMEGA approximately 0.2
-0.3 universe seems to provide a better fit, and flat (OMEGA = 1) mode
ls are ruled out at approximately 95% confidence level. On the other h
and, if the high limit of v(LG) = 350 km s-1 is closer to the truth, t
hen it appears that OMEGA approximately 0.7-0.8 is more consistent. Th
is test is insensitive to the shape of the power spectrum, but rather
sensitive to the normalization of the perturbation amplitude on the re
levant scale (e.g., sigma8) and OMEGA. We find that neither linear nor
nonlinear relations (with spherical symmetry) are good approximations
for the relation between radial peculiar velocity and density perturb
ation, i.e., nonspherical effects and gravitational tidal field are im
portant. The derived OMEGA using either of the two relations is undere
stimated. In some cases, this error is as large as a factor of 2-4.