A three-dimensional time-dependent convection model is used to describ
e circulation and property fields in rotating, stratified, and moving
fluids near a point source of heat. The study context and, consequentl
y, model scales are those of chronically discharging hydrothermal vent
fields found at submarine ridge crests. Hydrothermal plumes having di
stinctive thermal and chemical anomalies have been observed to rise se
veral hundreds of meters above the deep-sea floor before being advecte
d away by background cross flows typically of magnitude 1-4 cm s(-1).
The model is used to study effects of rotation and indicate difference
s in plumes with respect to variation of subgrid-scale turbulence inte
nsity and cross-flow strength. Counterrotating vorticity (zeta) couple
ts in all three coordinate directions develop in the lower plume stem
at startup and follow the plume to the level of neutral buoyancy; for
a nonrotational case (Omega = 0), zeta patterns resemble those previou
sly found for jets injected into homogenous cross flow. Ambient fluid
entrainment into the convecting column is primarily from the upstream
side, but deflection of background flow around both sides of the risin
g column is the root of the relative vorticity (zeta(z)) couplet in th
e lower plume. Turbulence intensity within the buoyant region of the p
lume and/or globally controls smoothness and temporal variability of d
istal nonbuoyant plume distributions, allowing or preventing oscillati
ons of potential temperature, theta, for example, at background buoyan
cy frequency, N. Over the range of turbulent mixing studied, rise heig
ht of plumes did not change appreciably, but breadth of plumes, counte
rintuitively, increased for decreasing turbulent mixing strength. Incr
easing cross-flow strength, U-0, bends model plumes such that rise hei
ght proportional to U-0(-0.4). For the two largest values of cross flo
w, for which R, the ratio of maximum vertical velocity to U-0, took va
lues of 2.8 and 1.0, plumes showed evidence of bifurcation.