############################################################################# # # # ww3_tp2.10 Test script for WW-III, two-dimensional propagation. # # Propagation on SMC grid with UNO2 scheme. # # # # Model should be compiled with the switches : # # # # see the switch files in subdirectory input/. # # # # Remarks : # # # # - This is a simplified version of the SMC0512 grid (to be introduced in # # cases), covering the Lake Erie only for a quick regression test. # # Corresponding input files are labeled with id 'Erie'. # # # # Output is converted into text files by ww3_outf as type 4 output, which # # is added as a new type for all sea points. Plotting of the output is # # achieved with a proper projection method with the help of the cell # # information file ErieSMCel.dat and the grid parameters stored in # # ww3_grid.inp. IDL scripts for plotting SMC grid output is available on # # demand until it is agreed to add them into the WW3 package as a post- # # procession tool. Regular grid at the base resolution is also possible # # as type 3 for instance but the refined cells are merged into base # # resolution regular grid ones. # # # # Further details about SMC grid, please see the guide documents: # # guide/SMC_Grid_Guide.pdf # # or contact me at Jian-Guo.Li@metoffice.gov.uk # # # # # # Sample run_test commands : # # (Note: mpirun commands differ by local system) # # ./bin/run_test ../model ww3_tp2.10 # # ./bin/run_test -s MPI -n 3 -p mpirun -f ../model ww3_tp2.10 # # # # Jian-Guo Li, Nov 2013 # # U. K. Met Office # # Last Mod : Dec 2013 # # # # The smc grid package is updated for V5.xx with a 3rd order advection # # scheme (UNO3) and extra smoothing term. They can be invoked by extra # # namelist (PSMC) parameters (UNO3 AVERG) to replace the default UNO2 # # scheme. Note the diffusion (set by DTIME) is still available. # # Jian-Guo Li, Oct 2015 # # # # National Oceanic and Atmospheric Administration. All rights # # reserved. WAVEWATCH III is a trademark of the NWS. # # No unauthorized use without permission. # # # #############################################################################