We use three-dimensional (3D) numerical magnetohydrodynamic simulations to
follow the evolution of cold, turbulent, gaseous systems with parameters ch
osen to represent conditions in giant molecular clouds (GMCs). We present r
esults of three model cloud simulations in which the mean magnetic field st
rength is varied (B-0 = 1.4-14 muG for GMC parameters), but an identical in
itial turbulent velocity field is introduced. We describe the energy evolut
ion, showing that (1) turbulence decays rapidly, with the turbulent energy
reduced by a factor 2 after 0.4-0.8 flow crossing times (similar to2-4 Myr
for GMC parameters), and (2) the magnetically supercritical cloud models gr
avitationally collapse after time approximate to6 Myr, while the magnetical
ly subcritical cloud does not collapse. We compare density, velocity, and m
agnetic field structure in three sets of model "snapshots" with matched val
ues of the Mach number M approximate to 9,7,5. We show that the distributio
ns of volume density and column density are both approximately log-normal,
with mean mass-weighted volume density a factor 3-6 times the unperturbed v
alue, but mean mass-weighted column density only a factor 1.1-1.4 times the
unperturbed value. We introduce a spatial binning algorithm to investigate
the dependence of kinetic quantities on spatial scale for regions of colum
n density contrast (ROCs) on the plane of the sky. We show that the average
velocity dispersion for the distribution of ROCs is only weakly correlated
with scale, similar to mean size-line width distributions for clumps withi
n GMCs. We find that ROCs are often superpositions of spatially unconnected
regions that cannot easily be separated using velocity information; we arg
ue that the same difficulty may affect observed GMC clumps. We suggest that
it may be possible to deduce the mean 3D size-line width relation using th
e lower envelope of the 2D size-line width distribution. We analyze magneti
c field structure and show that in the high-density regime n(H2) greater th
an or similar to 10(3) cm(-3), total magnetic field strengths increase with
density with logarithmic slope similar to1/3-2/3. We find that mean line-o
f-sight magnetic field strengths may vary widely across a projected cloud a
nd are not positively correlated with column density. We compute simulated
interstellar polarization maps at varying observer orientations and determi
ne that the Chandrasekhar-Fermi formula multiplied by a factor similar to0.
5 yields a good estimate of the plane-of sky magnetic field strength, provi
ded the dispersion in polarization angles is less than or similar to 25 deg
rees.