{"push_id":3120114438,"size":1,"distinct_size":1,"ref":"refs/heads/lipscomb/inversion_glp_nov2018","head":"b01fb4ab6ae3bc01963d45bd40b04045b2d8b965","before":"6389616d82550591d33c7a0e4824b5bb5ae6c000","commits":[{"sha":"b01fb4ab6ae3bc01963d45bd40b04045b2d8b965","author":{"name":"William Lipscomb","email":"671c22eb6dc2555f33d5a29c41156ce38e1d524e@ucar.edu"},"message":"Added code to process ISMIP6 ocean forcing data\n\nFor ISMIP6, the recommended way to compute melt rates is to read in a thermal forcing field\n(both a climatology and a transient thermal forcing field are available), and then\ncompute the melt rate as a quadratic function of temperature using a parameterization\nthat has been optimized for each of ~16 IMBIE basins.\n\nThis commit includes the infrastructure to support the new parameterization.\n\nText to be added explaining the various changes...\n\n Changes to be committed:\n       modified:   glide_setup.F90\n       modified:   glide_types.F90\n       modified:   glide_vars.def\n       modified:   ../libglimmer/parallel_mpi.F90\n       modified:   ../libglimmer/parallel_slap.F90\n       modified:   ../libglissade/glissade.F90\n       modified:   ../libglissade/glissade_bmlt_float.F90\n\nThe new code currently compiles but has not yet been tested and debugged.","distinct":true,"url":"https://api.github.com/repos/ESCOMP/cism/commits/b01fb4ab6ae3bc01963d45bd40b04045b2d8b965"}]}
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