Zp. Sun et G. Schubert, NUMERICAL-SIMULATION OF THERMAL-CONVECTION IN A ROTATING SPHERICAL FLUID SHELL AT HIGH TAYLOR AND RAYLEIGH NUMBERS, Physics of fluids, 7(11), 1995, pp. 2686-2699
In this study, we carry out numerical simulations of thermal convectio
n in a rapidly rotating spherical fluid shell at high Taylor number Ta
and Rayleigh number R with a nonlinear; three-dimensional time-depend
ent, spectral-transform code. The parameters used in the simulations a
re chosen to be in a range which allows us to study two different type
s of convection, i.e., single column and multi-layered types, and the
transition between them. Numerical solutions feature highly time-depen
dent north-south open columnar convective cells. The cells occur irreg
ularly in longitude, are quasi-layered in cylindrical radius, and main
tain alternating bands of mean zonal flow. The complex convective stru
cture and the banded mean zonal flow are results of the high Taylor an
d Rayleigh numbers. The transition between the two types of convection
appears to occur gradually with increasing Rayleigh and Taylor number
s. At a Taylor number of 10(7) the differential rotation pattern consi
sts of an inner cylindrical region of subrotation and an outer cylindr
ical shell of superrotation manifest at the outer boundary as an equat
orial superrotation and a high latitude subrotation. The differential
rotation pattern is similar at Ta = 10(8) and low Rayleigh number, Cyl
indrical shells of alternately directed mean zonal how begin to develo
p at Ta = 10(8) and R = 50R(c) and at Ta = 10(9) and R = 25R(c). This
pattern is seen pn the outer surface as a latitudinally-banded zonal f
low consisting of an equatorial superrotation, a-middle and high latit
ude subrotation, and a polar superrotation. At Ta = 10(9) and R = 50R(
c) the differential rotation appears at the surface as a broad eastwar
d how in the equatorial region with alternating bands of westward and
eastward how at high latitudes. (C) 1995 American Institute of Physics
.