############################################################################# # # # ww3_tic1.4:Test script for WW III, one-dimensional propagation # # through an ice layer with ice floes and ice thickness inputs # # # # Remarks : # # # # - Test case input (default): # # * ww3_grid_1000m_nondisp.inp # # + Spectral grid (applies to all) # # Number of directions : 24 # # Directional increment (deg.): 15.0 # # First direction (deg.): 0.0 # # Number of frequencies : 3 # # Frequency range (Hz) : 0.0800-0.1250 # # Increment factor : 1.250 # # + Spatial grid (applies to ww3_grid_2500m.inp only, many others # # are avaliable) # # Dimensions : 153 3 # # Increments (km) : 1.00 1.00 # # X range (km) : -1.00 152.00 # # Y range (km) : -1.00 1.00 # # # # Waves propagate from low-x to high-x. Boundary forcing is constant (not # # updated) defined at x=0. SWH~1 m at boundary. Direction is 270 deg. # # Waves propagate through ice, starting from rest (except at # # boundary). Ice concentration and ice floe are uniforms but ice # # thickness is growing from 0.1 to 1.0 with the time on all the grid. # # Scattering of waves by ice floes is treated separately from # # IC0/IC1/IC2 and is activated by IS2 which is included in this test case.# # # # Example run_test commands: # # # # ./bin/run_test -g 1000m -w work_IC0IS2 -s IC0IS2 -o netcdf # # ../model ww3_tic1.4 # # # # ./bin/run_test -g 1000m -w work_IC1IS2 -s IC1IS2 -o netcdf # # ../model ww3_tic1.4 # # # # bin/run_test -g IC2b_1000m -w work_IC2IS2 -s IC2IS2 -o netcdf # # ../model ww3_tic1.4 # # bin/run_test -g IC2d_1000m -w work_IC2IS2 -s IC2IS2 -o netcdf # # ../model ww3_tic1.4 # # bin/run_test -g IC2d_1000m -w work_IC2IS2 -s IC2IS2 -o netcdf -N # # ../model ww3_tic1.4 # # # # origination: Mickael Accensi, Oct 2015 # # last updated: Mickael Accensi, Jan 2018 # # # # Copyright 2009-2015 National Weather Service (NWS), # # National Oceanic and Atmospheric Administration. All rights # # reserved. WAVEWATCH III is a trademark of the NWS. # # No unauthorized use without permission. # # # #############################################################################