A three-dimensional finite-element method is used to investigate thermal convection in the earth's mantle. The equations of motion are solved implicitly by means of a fast multigrid technique. The computational mesh for the spherical problem is derived from the regular icosahedron. The calculations described use a mesh with 43,554 nodes and 81,920 elements and were run on a Cray X. The earth's mantly is modeled as a thick spherical shell with isothermal, free-slip boundaries. The infinite Prandtl number problem is formulated in terms of pressure, density, absolute temperature, and velocity and assumes an isotropic Newtonian rheology. Solutions are obtained for Rayleigh numbers up to approximately 106 for a variety of modes of heating. Cases initialized with a temperature distribution with warmer temperatures beneath spreading ridges and cooler temperatures beneath present subduction zones yield whole-mantle convection solutions with surface velocities that correlate well with currently observed plate velocities.
[1]
F. Busse,et al.
Patterns of convection in spherical shells. Part 2
,
1982,
Journal of Fluid Mechanics.
[2]
John H. Woodhouse,et al.
Mapping the upper mantle: Three‐dimensional modeling of earth structure by inversion of seismic waveforms
,
1984
.
[3]
Adam M. Dziewonski,et al.
Mapping the lower mantle: Determination of lateral heterogeneity in P velocity up to degree and order 6
,
1984
.
[4]
A. Boss.
Convection (earth interior).
,
1983
.
[5]
G. Schubert,et al.
Character and stability of axisymmetric thermal convection in spheres and spherical shells. [model for heat transfer in planetary interiors
,
1983
.
[6]
G. Schubert.
Subsolidus Convection in the Mantles of Terrestrial Planets
,
1979
.