z-logo
open-access-imgOpen Access
On topography and geoid from 2‐D stagnant lid convection calculations
Author(s) -
King Scott D.
Publication year - 2009
Publication title -
geochemistry, geophysics, geosystems
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.928
H-Index - 136
ISSN - 1525-2027
DOI - 10.1029/2008gc002250
Subject(s) - viscosity , geoid , convection , magnitude (astronomy) , mechanics , thermodynamics , cutoff , ocean surface topography , geology , physics , geophysics , geodesy , astrophysics , quantum mechanics , measured depth
Temperature‐dependent convection in the stagnant lid regime with a Frank‐Kamenetskii and Arrhenius viscosity formulation are compared. When properly scaled, the Nusselt number and root‐mean‐square velocity of the fluid for the two viscosity formulations are similar but the surface stresses and hence predicted dynamic topography and geoid differ significantly. The Arrhenius viscosity formulation results are insensitive to a viscosity cutoff at the high viscosity limit as long as the cutoff is 10 4 times the basal viscosity. The condition number for stagnant lid convection matrices using a penalty formulation is smaller than the penalty number times viscosity contrast value (a reasonable estimate of the condition number), explaining why large viscosity contrast convection problems with the penalty method agree with other formulations and analytic solutions. The difference in magnitude between the maximum and minimum dynamic topography could be used to constrain the magnitude of the viscosity contrast across the stagnant lid in planetary bodies.

The content you want is available to Zendy users.

Already have an account? Click here to sign in.
Having issues? You can contact us here