LITHOSPHERIC plate motions at the Earth's surface result from thermal
convection in the mantle(1). Understanding mantle convection is made d
ifficult by variations in the material properties of rocks as pressure
and temperature increase from the surface to the core. The plates the
mselves result from high rock strength and brittle failure at low temp
erature near the surface. In the deeper mantle, elevated pressure may
increase the effective viscosity by orders of magnitude(2-5). The infl
uence of depth-dependent viscosity on convection has been explored in
two-dimensional numerical experiments(6-8), but planforms must be stud
ied in three dimensions. Although three-dimensional planforms can be e
lucidated by laboratory fluid dynamic experiments(9,10), such experime
nts cannot simulate depth-dependent rheology. Here we use a three-dime
nsional spherical convection model(11,12) to show that a modest increa
se in mantle viscosity dth depth has a marked effect on the planform o
f convection, resulting in long, linear downwellings from the upper su
rface boundary layer and a surprisingly 'red' thermal heterogeneity sp
ectrum, as observed for the Earth's mantle(13). These effects of depth
-dependent viscosity may be comparable to the effects of the plates th
emselves.