# Difference between revisions of "Higher order velocity schemes"

From Interactive System for Ice sheet Simulation

(New page: *HO model; what distinguishes it from a LO model, why is it useful. *Available HO schemes (e.g. Full Stokes, Blatter-Pattyn, Bueler & Pollard Hybrids) *Architecture (transport, and non-lin...) |
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*Boundary conditions + masking, one sided differences, basal BC (no-slip, viscous, and plastic behavior all through Beta^2 implementation) | *Boundary conditions + masking, one sided differences, basal BC (no-slip, viscous, and plastic behavior all through Beta^2 implementation) | ||

*Run verification suites; ISMIP-HOM, Ross IS | *Run verification suites; ISMIP-HOM, Ross IS | ||

− | *Apply HO velocity fields to 1st-order upwind transport (dH/dt) scheme (see "adding a module") | + | *Apply HO velocity fields to 1st-order upwind transport (dH/dt) scheme (see "adding a module"[http://websrv.cs.umt.edu/isis/index.php/Adding_a_module_to_Glimmer_I]) |

## Revision as of 11:44, 16 July 2009

- HO model; what distinguishes it from a LO model, why is it useful.
- Available HO schemes (e.g. Full Stokes, Blatter-Pattyn, Bueler & Pollard Hybrids)
- Architecture (transport, and non-linear iteration on diffusivity) of Glimmer an how it differs from a HO model architecture
- Introduce HO CISM (Blatter-Pattyn 1st-order scheme)
- Discretization and solution (elliptic solve, operator splitting approach, etc)
- Boundary conditions + masking, one sided differences, basal BC (no-slip, viscous, and plastic behavior all through Beta^2 implementation)
- Run verification suites; ISMIP-HOM, Ross IS
- Apply HO velocity fields to 1st-order upwind transport (dH/dt) scheme (see "adding a module"[1])