예제 #1
0
#string that the fortran code automatically uses. Not sure how to 
#change this at the moment.

#initializing variable to store output file name string
#will probably need to be incremented as model is run
outputfile_iter = 0
outputfile = 'workrslt.{:0>3d}'.format(outputfile_iter)

#need to write out outputfile_iter as a text file required by the
#fortran code
f = open('filenum.dat', 'w')
f.write('{:0>3d}'.format(outputfile_iter))
f.close()

#Evaluate model using fortran code to get synthetic observation
interface.exec_rtmod()

#Read result file into python
syn_obs = observation.Synthetic(filename = outputfile)

#below is testing ... remove when find_best_model.py is finished
initial_csq = compare.calc_chisq(datacuts, syn_obs)

print "Chi-square: {}".format(initial_csq)

#diagnostic:
real = observation.concat(datacuts)
syn = syn_obs.concat(3)


#remove temporary working model files
예제 #2
0
def calc_deriv(atm_model, synobs):
	"""
	Calculate derivatives (changes in synthetic observation) produced by changes introduced by adjusting the parameters. 
	"""
	
	#determine number of parameters
	nparams = atm_model.nflags
	
#create synthetic observation I/F data vector (i.e. 1 numpy array combining
#all spectral channels)
	syn_vec = synobs.concat(synobs.nangles)
	
#initialize derivative array
	deriv_array = np.array([])
	
	#create copy of input model for testing
	tmp_model = copy.deepcopy(atm_model)
	
	epsilon = 0.01
	
#parse input atmospheric model for flags, change parameter one at a time
	
#for each atmospheric layer
	for i in range(tmp_model.nlayers):

#first, extract said layer
		l = getattr(tmp_model, 'l'+str(i+1))
		
#parse layer for flags
#determine index locations
		flaglocs = [a for a in range(len(l.flaglist)) \
					if type(l.flaglist[a]) == str]
#source
#http://stackoverflow.com/questions/7270321/finding-the-index-of-elements-based-on-a-condition-using-python-list-comprehensi


		for j in flaglocs:
#when encountering flag:
#determine old value
			old_param_val = getattr(l, l.param_names[j])

#adjust parameter by epsilon
#note, this is currently ALWAYS a positive change
#since this is only calculating derivative, not adjusting the model towards
#a best-fit.
			l.adj_param_epsilon(l.param_names[j])
#determine change in parameter
			new_param_val = getattr(l, l.param_names[j])
			diff_param = new_param_val - old_param_val
			
#replace modified layer in atmosphere object
# i = layer number
# l = new layer object
			tmp_model.replace_layer(i+1, l)			

#run model with changed parameter
#set up temporary files for output / RT model execution
			f = open('filenum.dat', 'w')
			f.write('{:0<3d}'.format(999))  
			#999 = code for tmp/fleeting file in radtran model
			f.close()
			
#write out temp model for RT code
			tmp_model.write_ft_input(filename='workmodl999')
			
#Evaluate model using fortran code to get synthetic observation
			interface.exec_rtmod()

#Read result file into python
			tmp_syn = observation.Synthetic(filename = 'workrslt.999')

#create tmp synthetic observation concatenated vector
			tmp_syn_vec = tmp_syn.concat(synobs.nangles)

#determine change in I/F
			diff = (tmp_syn_vec - syn_vec)/(diff_param)

#store in derivative array
			if deriv_array.size == 0:
				deriv_array = np.append(deriv_array, diff)
			else:
				deriv_array = np.vstack((deriv_array, diff))

#restore tmp_model to the old state
			tmp_model = copy.deepcopy(atm_model)
			
#delete temporary working model
			os.system('rm -f workmodl999')
	
	return deriv_array