modified post processing script to work for any piece of output data

This commit is contained in:
Bryan Herman 2012-03-03 15:44:19 -05:00
parent 73fd4449df
commit 4ea142cc27

View file

@ -12,20 +12,22 @@ class EigenFunction:
'''Represents the reference eigenfunction'''
reference = 0.
#
def __init__(self):
def __init__(self,data):
#
'''Initializes the eigenfunction'''
self.function = 0.
self.data = data
#
def read_hdf5(self,h5_file,cycle):
#
'''Read data from HDF5 file'''
self.cycle = cycle
f = h5py.File(h5_file,'r')
group = '/cycle'+str(cycle)+'/openmc_src'
group = '/cycle'+str(cycle)+'/'+self.data
dataset = f[group]
self.function = np.empty(dataset.shape,dataset.dtype)
dataset.read_direct(self.function)
self.function = self.function * ((16)**2-5*2**2)*177
self.iamref = 'F'
#
def set_reference(self):
@ -38,102 +40,162 @@ class EigenFunction:
#
'''Computes RMS value'''
Np = self.function.size
tmp = (self.function - EigenFunction.reference)*(self.function - EigenFunction.reference)
Np = ((16)**2-5*2**2)*177
tmp = (self.function - EigenFunction.reference)**2
tmp2 = tmp.sum()
self.rms = np.sqrt((1.0/float(Np))*tmp2)
#
if sys.argv[1] != 'restart':
def read_runs(runpath,hdfile,cycle_start,cycle_end,run_start,run_end,data):
runlist = []
tmp = EigenFunction(data)
tmp.read_hdf5(runpath+str(run_start)+'/'+hdfile,cycle_start)
indices = tmp.function.shape # extent of all dimensions
i = cycle_start
while i <= cycle_end:
meantmp = EigenFunction(data) # init mean object
j = run_start
runs = np.zeros((run_end - run_start + 1,indices[0],indices[1],indices[2],indices[3])) # init runs array
while j <= run_end:
tmp.read_hdf5(runpath+str(j)+'/'+hdfile,i) # read hdf5 file
runs[j-run_start] = tmp.function # put function into runs
j += 1
meantmp.function = np.average(runs, axis=0) # compute the mean
runlist.append(meantmp)
print 'Read in from path: '+runpath+' Cycle: '+str(i)
i += 1
return runlist
# calculate reference solution
def create_reference(runpath,hdfile,cycle,run_start,run_end,data):
# calculate reference solution
print 'Calculating Reference solution...'
runpath = '/media/Backup/opr_runs/1mil/run' # the directory prefix
hdfile = '/output.h5' # hdf5 file name
cycle = 840 # cycle number to extract
run_end = 25 # number of runs to look at
tmp = EigenFunction()
tmp.read_hdf5(runpath+str(1)+hdfile,cycle) # load first eigenfunction
tmp = EigenFunction(data)
tmp.read_hdf5(runpath+str(run_start)+'/'+hdfile,cycle) # load first eigenfunction
indices = tmp.function.shape # extent of all dimensions
ref = np.zeros((run_end,indices[0],indices[1],indices[2],indices[3])) # initialize ref array
ref[0] = tmp.function # set the first run in ref
i = 2
i = run_start + 1
while i <= run_end: # begin loop around all runs
tmp.read_hdf5(runpath+str(i)+hdfile,cycle)
tmp.read_hdf5(runpath+str(i)+'/'+hdfile,cycle)
print 'Read in: '+runpath+str(i)+hdfile
ref[i-1] = tmp.function
ref[i - run_start] = tmp.function
i += 1
meanref = np.average(ref, axis=0) # compute average of all runs
EigenFunction.reference = meanref # set to global space in EigenFunction instances
return meanref
# calculate rms for 1 million case
print 'Calculating 1million History case...'
onemil = []
cycle_start = 201
cycle_end = 840
run_end = 10
i = cycle_start
while i <= cycle_end:
meantmp = EigenFunction() # init mean object
j = 1
runs = np.zeros((run_end,indices[0],indices[1],indices[2],indices[3])) # init runs array
while j <= run_end:
tmp.read_hdf5(runpath+str(j)+hdfile,i) # read hdf5 file
runs[j-1] = tmp.function # put function into runs
j += 1
meantmp.function = np.average(runs, axis=0) # compute the mean
onemil.append(meantmp)
print 'Read in from path: '+runpath+' Cycle: '+str(i)
i += 1
def compute_rms(runlist):
# calculate rms array
print 'Calculating rms...'
rms = np.zeros((cycle_end - cycle_start + 1))
rms = np.zeros(len(runlist))
i = 0
while i < len(onemil):
onemil[i].compute_rms()
rms[i] = onemil[i].rms
while i < len(runlist):
runlist[i].compute_rms()
rms[i] = runlist[i].rms
i += 1
return rms
# write out numpy array to binary file
print 'Writing output...'
output = {}
output.update({'1milrms':rms})
output.update({'ref':meanref})
fileout = open('rms.out','wb')
cPickle.dump(output,fileout)
fileout.close()
else:
# load in data
print 'Loading input...'
filein = open('rms.out','r')
output = cPickle.load(filein)
filein.close()
rms = output['1milrms']
meanref = output['ref']
EigenFunction.reference = meanref
def plot_rms(rms):
print 'Generating plot...'
ax = plt.subplot(111)
size = rms.shape[0]
x = np.linspace(1,size,size)*1e6
y = (rms[size-1]/x[size-1]**(-0.5))*x**(-0.5)
plt.loglog(x,rms*100,'b+')
plt.loglog(x,y*100,'g--')
ax.xaxis.grid(True,'minor')
ax.yaxis.grid(True,'minor')
ax.xaxis.grid(True,'major',linewidth=2)
ax.yaxis.grid(True,'major',linewidth=2)
plt.xlabel('# of Total Neutron Histories (active cycles)')
plt.ylabel('RMS Error [%]')
plt.legend(('1 million (10 runs)','Ideal Error 1 mil'))
return
def plot_source(source):
plt.figure()
X = np.linspace(1,272,272)
Y = np.linspace(1,272,272)
Y,X = np.meshgrid(Y,X)
plt.contourf(X,Y,source[0,:,:,0],100)
plt.colorbar()
plt.xlabel('Mesh Cell in x-direction')
plt.ylabel('Mesh Cell in y-direction')
plt.title('OPR Converged Fission Source Distribution')
plt.show()
#
if __name__ == "__main__":
if sys.argv[1] == 'restart':
# load in data
print 'Loading input...'
filein = open('rms.out','r')
output = cPickle.load(filein)
filein.close()
rms = output['1milrms']
meanref = output['ref']
EigenFunction.reference = meanref
# plot rms
plot_rms(rms)
# plot mean source distribution
plot_source(meanref)
elif sys.argv[1] == 'interactive':
# load in data
print 'Loading input...'
filein = open('rms.out','r')
output = cPickle.load(filein)
filein.close()
rms = output['1milrms']
meanref = output['ref']
EigenFunction.reference = meanref
# pop an interactive python shell
from IPython import embed
embed()
else:
# calculate reference solution
runpath = '/media/Backup/opr_runs/1mil/run'
hdfile = 'output.h5'
cycle = 840
run_start = 1
run_end = 25
data = 'openmc_src'
meanref = create_reference(runpath,hdfile,cycle,run_start,run_end,data)
# calculate rms for 1 million case
runpath = '/media/Backup/opr_runs/1mil/run'
hdfile = 'output.h5'
cycle_start = 201
cycle_end = 840
run_start = 1
run_end = 1
data = 'openmc_src'
onemil = read_runs(runpath,hdfile,cycle_start,cycle_end,run_start,run_end,data)
# calculate rms array
rms = compute_rms(onemil)
# write out numpy array to binary file
print 'Writing output...'
output = {}
output.update({'1milrms':rms})
output.update({'ref':meanref})
fileout = open('rms.out','wb')
cPickle.dump(output,fileout)
fileout.close()
# plot rms
plot_rms(rms)
# plot mean source distribution
plot_source(meanref)
# plot rms
print 'Generating plot...'
ax = plt.subplot(111)
x = np.linspace(1,640,640)*1e6
y = rms[0]/1e-3*x**(-0.5)
plt.loglog(x,rms*100,'b--')
plt.loglog(x,y*100,'g-')
ax.xaxis.grid(True,'minor')
ax.yaxis.grid(True,'minor')
ax.xaxis.grid(True,'major',linewidth=2)
ax.yaxis.grid(True,'major',linewidth=2)
plt.xlabel('# of Total Neutron Histories (active cycles)')
plt.ylabel('RMS Error [%]')
plt.legend(('1 million (10 runs)','Ideal Error 1 mil'))
# plot mean source distribution
plt.figure()
X = np.linspace(1,272,272)
Y = np.linspace(1,272,272)
Y,X = np.meshgrid(Y,X)
plt.contourf(X,Y,meanref[0,:,:,0],100)
plt.colorbar()
plt.xlabel('Mesh Cell in x-direction')
plt.ylabel('Mesh Cell in y-direction')
plt.title('OPR Converged Fission Source Distribution')
plt.show()