L. Cserepes et al., Effect of the mid-mantle viscosity and phase-transition structure on 3D mantle convection, PHYS E PLAN, 118(1-2), 2000, pp. 135-148
Recent geophysical evidence shows some sort of layering in the lower part o
f the mantle transition zone down to a depth of 1000 km, Seismic observatio
ns have revealed a sharp reflector surface at around 900 or 1000 km depth f
or which a possible explanation can be given in terms of a new phase transi
tion of the lower-mantle constituent minerals, Furthermore, new results fro
m the inversion of the oceanic geoid show the existence of a second low vis
cosity zone (LVZ) somewhere between 660 and 1000 Bm depth. The existence of
the second LVZ may be linked to the mid-mantle phase transitions. The phas
e and viscosity stratification of the transition zone have been included in
a series of 3D convection simulations in a 4 X 4 X 1 rectangular box with
a surface Rayleigh number of 2 x 10(7). Beneath the well-known 400 and 660
km phase changes, we assumed a hypothetical weak endothermic transition at
1000 km in some of our models. The principal controlling factor of the styl
e of mantle convection is still the 660 km endothermic transition, which se
ts up a partial or full barrier to flow, causing stratified circulation. We
used various viscosity profiles with emphasis on the model containing the
second LVZ, The main consequence of this zone is to enhance flow layering,
Many plumes can emanate from the transition zone and small-scale instabilit
ies develop in the second LVZ. When the 1000 km endothermic phase transitio
n is included, these instabilities can grow only at a few places but then t
hey form strong downwellings. Two distinct types of penetrative, deep downw
ellings can be present at the same time: one which crosses the whole transi
tion zone, and another one which crosses only the 660 km discontinuity and
stops at 1000 km at least temporarily. This can explain seismological obser
vations which suggest that subducted slabs can be retarded not only by the
660 km boundary but also by some deeper obstacle near 1000 km depth. (C) 20
00 Elsevier Science B.V. All rights reserved.