HR: 0830h
AN: T41C-0232 [PDF]
TI: The Anisotropic and Rheological Structure of the Oceanic Upper Mantle From a Simple Model of Plate
Shear
AU: * Podolefsky, N S
EM: noah.podolefsky@colorado.edu
AF: University of Colorado, Campus Box 390, Boulder, CO 80309
AU: Zhong, S
EM: szhong@spice.colorado.edu
AF: University of Colorado, Campus Box 390, Boulder, CO 80309
AU: McNamara, A K
EM: allen.mcnamara@colorado.edu
AF: University of Colorado, Campus Box 390, Boulder, CO 80309
AB:
We have developed a channel flow model that dynamically couples plate
motion and mantle stress with a composite rheology (diffusion creep
and dislocation creep) to study rheological and anisotropic structures
of the oceanic upper mantle. A semi-analytic approach is used to solve
for mantle stress and viscosity, allowing fast calculations and
exploration of a wide range of rheological parameters. Mantle stress
in our model is due to shearing by a moving plate. By comparing mantle
stress to a transition stress for dislocation creep, we identify
regions where either diffusion creep or dislocation creep is
active. Deformation by dislocation creep results in mineral fabric
that may be responsible for observed seismic anisotropy. Our study
suggests that there is an important relation between plate motion,
seismic anisotropy, mantle viscosity, and transition stress. Using
laboratory results for rheological parameters, we find that
dislocation creep exists only in a layer at certain depths in the
upper mantle. For plate velocity of 10 cm/yr, asthenospheric viscosity
of $10^{19}$ Pa-s, and asthenospheric transition stress of 0.1 MPa,
our model predicts a ~200 km thick dislocation creep layer, which is
broadly consistent with the observations of seismic anisotropy. For
plate velocity of 10 cm/yr and asthenospheric transition stress of 0.1
MPa, the asthenospheric viscosity needs to be greater than $5x10^{18}$
Pa-s to produce any dislocation creep deformation, and the
asthenospheric viscosity needs to be larger for slower plate motion or
larger transition stress. Slower plate motion leads to a thinner
dislocation creep layer, which may partially explain the observed
asymmetry in anisotropic structure in the East Pacific Rise.
DE: 8120 Dynamics of lithosphere and mantle--general
SC: Tectonophysics [T]
MN: 2003 Fall Meeting