#!/usr/bin/env python # -*- Mode: Python; coding: utf-8; indent-tabs-mode: nil; tab-width: 4 -*- # Post-diagnostic of STATION_ASF / L. Brodeau, 2019 import sys #from os import path as path #from string import replace import math import numpy as nmp #import scipy.signal as signal from netCDF4 import Dataset import matplotlib as mpl mpl.use('Agg') import matplotlib.pyplot as plt import matplotlib.dates as mdates #from string import find #import warnings #warnings.filterwarnings("ignore") #import time #import barakuda_plot as bp #import barakuda_tool as bt reload(sys) sys.setdefaultencoding('utf8') cy1 = '2016' ; # First year cy2 = '2018' ; # Last year dir_figs='.' size_fig=(13,7) fig_ext='png' clr_red = '#AD0000' clr_sat = '#ffed00' clr_mod = '#008ab8' rDPI=200. L_ALGOS = [ 'COARE3p6' , 'ECMWF' , 'NCAR' ] l_color = [ '#ffed00' , '#008ab8' , '0.4' ] ; # colors to differentiate algos on the plot l_width = [ 3 , 2 , 1 ] ; # line-width to differentiate algos on the plot l_style = [ '-' , '-' , '--' ] ; # line-style L_VNEM = [ 'qla' , 'qsb' , 'qt' , 'qlw' , 'taum' , 'dt_skin' ] L_VARO = [ 'Qlat' , 'Qsen' , 'Qnet' , 'Qlw' , 'Tau' , 'dT_skin' ] ; # name of variable on figure L_VARL = [r'$Q_{lat}$',r'$Q_{sens}$',r'$Q_{net}$',r'$Q_{lw}$',r'$|\tau|$',r'$\Delta T_{skin}$' ] ; # name of variable in latex mode L_VUNT = [ r'$W/m^2$' , r'$W/m^2$' , r'$W/m^2$' , r'$W/m^2$' , r'$N/m^2$' , 'K' ] L_VMAX = [ 75. , 75. , 800. , 25. , 1.2 , -0.7 ] L_VMIN = [ -250. , -125. , -400. , -150. , 0. , 0.7 ] L_ANOM = [ True , True , True , True , True , False ] nb_algos = len(L_ALGOS) ; print(nb_algos) # Getting arguments: narg = len(sys.argv) if narg != 3: print 'Usage: '+sys.argv[0]+' '; sys.exit(0) cdir_data = sys.argv[1] cyyyy = sys.argv[2] # Files to be read: cf_in = [] for ja in range(nb_algos): cf_in.append(cdir_data+'/output/'+'STATION_ASF-'+L_ALGOS[ja]+'_1h_'+cy1+'0101_'+cy2+'1231_gridT.nc') print('Files we are goin to use:') for ja in range(nb_algos): print(cf_in[ja]) # Getting time array from the first file: id_in = Dataset(cf_in[0]) vt = id_in.variables['time_counter'][:] cunit_t = id_in.variables['time_counter'].units ; print(' "time_counter" is in "'+cunit_t+'"') id_in.close() nbr = len(vt) vtime = nmp.zeros(nbr) vt = vt + 1036800. # BUG!??? don't get why false in epoch to date conversion, and yet ncview gets it right! for jt in range(nbr): vtime[jt] = mdates.epoch2num(vt[jt]) ii=nbr/300 ib=max(ii-ii%10,1) xticks_d=int(30*ib) font_inf = { 'fontname':'Open Sans', 'fontweight':'normal', 'fontsize':14 } nb_var = len(L_VNEM) xF = nmp.zeros((nbr,nb_algos)) xFa = nmp.zeros((nbr,nb_algos)) for jv in range(nb_var): print('\n *** Treating variable: '+L_VARO[jv]+' !') for ja in range(nb_algos): id_in = Dataset(cf_in[ja]) xF[:,ja] = id_in.variables[L_VNEM[jv]][:,1,1] # only the center point of the 3x3 spatial domain! if ja == 0: cvar_lnm = id_in.variables[L_VNEM[jv]].long_name id_in.close() #print(' => '+L_ALGOS[ja]+' => ok!') fig = plt.figure(num = jv, figsize=size_fig, facecolor='w', edgecolor='k') ax1 = plt.axes([0.07, 0.22, 0.9, 0.75]) ax1.set_xticks(vtime[::xticks_d]) ax1.xaxis.set_major_formatter(mdates.DateFormatter('%Y-%m-%d %H:%M:%S')) plt.xticks(rotation='60') for ja in range(nb_algos): plt.plot(vtime, xF[:,ja], '-', color=l_color[ja], linestyle=l_style[ja], linewidth=l_width[ja], label=L_ALGOS[ja], zorder=10+ja) ax1.set_ylim(L_VMIN[jv], L_VMAX[jv]) ; ax1.set_xlim(vtime[0],vtime[nbr-1]) plt.ylabel(L_VARL[jv]+' ['+L_VUNT[jv]+']') ax1.grid(color='k', linestyle='-', linewidth=0.3) plt.legend(bbox_to_anchor=(0.45, 0.2), ncol=1, shadow=True, fancybox=True) ax1.annotate(cvar_lnm, xy=(0.3, 0.97), xycoords='axes fraction', bbox={'facecolor':'w', 'alpha':1., 'pad':10}, zorder=50, **font_inf) plt.savefig(L_VARO[jv]+'.'+fig_ext, dpi=int(rDPI), transparent=False) plt.close(jv) if L_ANOM[jv]: for ja in range(nb_algos): xFa[:,ja] = xF[:,ja] - nmp.mean(xF,axis=1) # Want a symetric y-range that makes sense for the anomaly we're looking at: rmax = nmp.max(xFa) ; rmin = nmp.min(xFa) rmax = max( abs(rmax) , abs(rmin) ) romagn = math.floor(math.log(rmax, 10)) ; # order of magnitude of the anomaly we're dealing with rmlt = 10.**(int(romagn)) / 2. yrng = math.copysign( math.ceil(abs(rmax)/rmlt)*rmlt , rmax) #print 'yrng = ', yrng ; #sys.exit(0) fig = plt.figure(num = 10+jv, figsize=size_fig, facecolor='w', edgecolor='k') ax1 = plt.axes([0.07, 0.22, 0.9, 0.75]) ax1.set_xticks(vtime[::xticks_d]) ax1.xaxis.set_major_formatter(mdates.DateFormatter('%Y-%m-%d %H:%M:%S')) plt.xticks(rotation='60') for ja in range(nb_algos): plt.plot(vtime, xFa[:,ja], '-', color=l_color[ja], linewidth=l_width[ja], label=L_ALGOS[ja], zorder=10+ja) ax1.set_ylim(-yrng,yrng) ; ax1.set_xlim(vtime[0],vtime[nbr-1]) plt.ylabel(L_VARL[jv]+' ['+L_VUNT[jv]+']') ax1.grid(color='k', linestyle='-', linewidth=0.3) plt.legend(bbox_to_anchor=(0.45, 0.2), ncol=1, shadow=True, fancybox=True) ax1.annotate('Anomaly of '+cvar_lnm, xy=(0.3, 0.97), xycoords='axes fraction', bbox={'facecolor':'w', 'alpha':1., 'pad':10}, zorder=50, **font_inf) plt.savefig(L_VARO[jv]+'_anomaly.'+fig_ext, dpi=int(rDPI), transparent=False) plt.close(10+jv)