A. Lenardic et Wm. Kaula, MORE THOUGHTS ON CONVERGENT CRUSTAL PLATEAU FORMATION AND MANTLE DYNAMICS WITH REGARD TO TIBET, J GEO R-SOL, 100(B8), 1995, pp. 15193-15203
Evidence suggests that some 10 m.y. ago a large portion of thickened m
antle lithosphere below the Tibetan Plateau was rapidly removed. Remov
al appears to have been abrupt and delayed from the time of substantia
l thickening. Fluid dynamical models of convective thermal boundary la
yer instability have had difficulties explaining abrupt lithospheric r
emoval long after initial thickening. Such models have implied that ei
ther removal should be synchronous with thickening or should not occur
at all, due to boundary layer stabilization resulting from high litho
spheric viscosity. We present simple thermal/chemical boundary layer c
onvection models that suggest a compromise between previous end-member
results. The models allow for delayed instability of a thickened ther
mal boundary layer under geologically reasonable parameter conditions.
Instability delay relies on high viscosity of thickened mantle lithos
phere stabilizing it against free convective removal and on lateral ex
tent of thickened crust exceeding that of mantle lithosphere. The latt
er condition leads to a peripheral region of thickened crust and relat
ively unthickened mantle lithosphere and an interior plateau region of
both thickened crust and mantle lithosphere. If the thermal resistanc
e and/or the rate of internal heat production of crust is greater than
that of mantle, then mantle lithosphere at the peripheral region can
be thermally eroded to the point that the base of the crust comes into
contact with bulk mantle. This creates a peripheral weak zone that al
lows thickened mantle lithosphere of the interior plateau region to be
come mechanically detached and sink into bulk mantle. The instability
is akin to delamination, as originally defined, and its delay time is
roughly the thermal diffusion time across the thinnest portion of mant
le lithosphere.