Global time-dependent simulations provide a means to investigate time-depen
dent dynamic evolution in accretion disks. This paper seeks to extend previ
ous local simulations by beginning a systematic effort to develop fully glo
bal three-dimensional simulations. The nonlinear development of the magneto
rotational instability is investigated using a time-explicit finite differe
nce code written in cylindrical coordinates. The equations of ideal magneto
hydrodynamics are solved with the assumption of an adiabatic equation of st
ate. Both a Newtonian potential and a pseudo-Newtonian potential are used.
Two simplifications are also explored: a cylindrical gravitational potentia
l (the "cylindrical disk") and axisymmetry. The results from those simulati
ons are compared with fully three-dimensional global simulations. The globa
l simulations begin with equilibrium pressure-supported accretion tori. Two
different initial held geometries are investigated: poloidal fields that a
re constant along initial equidensity surfaces and toroidal fields with a c
onstant ratio of gas to magnetic pressure. In both cases the magnetorotatio
nal instability rapidly develops and the torus becomes turbulent. The resul
ting turbulence transports angular momentum, and the torus develops an angu
lar momentum distribution that is near Keplerian. A comparison with axisymm
etric simulations shows that in three dimensions the magnetorotational inst
ability can act as a dynamo and regenerate poloidal field, thereby sustaini
ng the turbulence. As previously observed in local simulations, the stress
is dominated by the Maxwell component. The total stress in the interior of
the disk is approximate to 0.1-0.2 times the thermal pressure. At late time
the disks are characterized by relatively thick configurations, with rapid
time dependence and tightly wrapped, low-ill spiral structures.