def __init__(self, which_case, LUT, RandomSamples, interp_type):
print 'SciPy Interpolating ', which_case
select = {\
"rhoe":('Density','StaticEnergy'),\
"PT":('Pressure','Temperature'),\
"Prho":('Pressure','Density'),\
"rhoT":('Density','Temperature'),\
"Ps":('Pressure','Entropy'),\
"hs":('Enthalpy','Entropy')\
}
thermo1, thermo2, = select[which_case]
x =getattr(LUT,thermo1)
y =getattr(LUT,thermo2)
samples_x = getattr(RandomSamples,thermo1)
samples_y = getattr(RandomSamples,thermo2)
setattr(self,thermo1, samples_x)
setattr(self,thermo2, samples_y)
variables = sp.array(['Temperature','Density','Enthalpy','StaticEnergy',\
'Entropy','Pressure','SoundSpeed2','dPdrho_e','dPde_rho',\
'dTdrho_e','dTde_rho','Cp','Mu','Kt']);
for var in variables[sp.where((variables!=thermo1) * (variables!=thermo2))]:
z = getattr(LUT,var)
interp_func = sp.interpolate.griddata((x,y),z,sp.column_stack((samples_x,samples_y)),\
method=interp_type)
nan_index = sp.where(sp.isnan(interp_func))
interp_func[nan_index]= sp.interpolate.griddata((x,y),z,\
sp.column_stack((samples_x[nan_index],samples_y[nan_index])),\
method='nearest')
setattr(self,var,interp_func)
return
def GetFermiSigns(filename, refstate=None, channel=None):
attr = GetAttr(filename)
filetype = ''
try:
filetype = attr['type']
except KeyError:
mo = re.match('.*/?[0-9]+-(.*)\.h5', filename)
filetype = mo.groups()[0]
L = attr['L']
if refstate == None:
refstate = sc.zeros(2 * L * L)
refstate[0::2] = 1
if filetype == 'WaveFunction':
hfile = h5py.File(filename, 'r')
if 'states_up' in hfile.keys():
states = sc.column_stack([hfile['states_up'], hfile['states_do']])
else:
states = sc.column_stack([hfile['states_0'], hfile['states_1']])
hfile.close()
return sf.fermisigns(states, refstate)
else:
if channel == None:
channel = attr['channel']
L = int(attr['L'])
if 'phasex' in attr.keys():
shift = [attr['phasex'] / 2.0, attr['phasey'] / 2.0]
else:
shift = [attr['phase_shift_x'] / 2.0, attr['phase_shift_y'] / 2.0]
q = [float(attr['qx']) / L, float(attr['qy']) / L]
if channel == 'trans':
return sf.transfermisigns(L, L, shift, q)
elif channel == 'long':
return sf.longfermisigns(L, L, shift, q)
else:
raise KeyError('\"channel\" must be either \"trans\" or \"long\".')
def _packData(self, G1, indices2select, effect):
if effect == 'fixed':
if G1 is None and self.G0 is None:
data = self.X[self.data_permutation][indices2select]
elif G1 is None:
data = sp.column_stack((self.G0[self.data_permutation][indices2select],
self.X[self.data_permutation][indices2select]))
elif self.G0 is None:
data = sp.column_stack((G1[self.data_permutation][indices2select],
self.X[self.data_permutation][indices2select]))
else:
data = sp.column_stack((self.G0[self.data_permutation][indices2select],
G1[self.data_permutation][indices2select],
self.X[self.data_permutation][indices2select]))
elif effect == 'mixed':
X = self.X[self.data_permutation]
if self.G0 is not None:
G0 = self.G0[self.data_permutation]
if G1 is not None:
G1 = G1[self.data_permutation]
data = []
for i in range(len(indices2select)):
lis = [X[indices2select[i]]]
if G0 is not None:
lis.append( G0[indices2select[i]] )
if G1 is not None:
lis.append( G1[indices2select[i]] )
data.append( lis )
else:
assert False, 'Unkown effect type.'
return (data, self.Y[self.data_permutation][indices2select])
def _packData(self, G1, indices2select, effect):
if effect == 'fixed':
if G1 is None and self.G0 is None:
data = self.X[self.data_permutation][indices2select]
elif G1 is None:
data = sp.column_stack((self.G0[self.data_permutation][indices2select],
self.X[self.data_permutation][indices2select]))
elif self.G0 is None:
data = sp.column_stack((G1[self.data_permutation][indices2select],
self.X[self.data_permutation][indices2select]))
else:
data = sp.column_stack((self.G0[self.data_permutation][indices2select],
G1[self.data_permutation][indices2select],
self.X[self.data_permutation][indices2select]))
elif effect == 'mixed':
X = self.X[self.data_permutation]
if self.G0 is not None:
G0 = self.G0[self.data_permutation]
if G1 is not None:
G1 = G1[self.data_permutation]
data = []
for i in range(len(indices2select)):
lis = [X[indices2select[i]]]
if G0 is not None:
lis.append( G0[indices2select[i]] )
if G1 is not None:
lis.append( G1[indices2select[i]] )
data.append( lis )
else:
assert False, 'Unkown effect type.'
return (data, self.Y[self.data_permutation][indices2select])
def GetFermiSigns(filename,refstate=None,channel=None):
attr=GetAttr(filename)
filetype=''
try:
filetype=attr['type']
except KeyError:
mo=re.match('.*/?[0-9]+-(.*)\.h5',filename)
filetype=mo.groups()[0]
L=attr['L']
if refstate==None:
refstate=sc.zeros(2*L*L)
refstate[0::2]=1
if filetype=='WaveFunction':
hfile=h5py.File(filename,'r')
if 'states_up' in hfile.keys():
states=sc.column_stack([hfile['states_up'],hfile['states_do']])
else:
states=sc.column_stack([hfile['states_0'],hfile['states_1']])
hfile.close()
return sf.fermisigns(states,refstate)
else:
if channel==None:
channel=attr['channel']
L=int(attr['L'])
if 'phasex' in attr.keys():
shift=[attr['phasex']/2.0,attr['phasey']/2.0]
else:
shift=[attr['phase_shift_x']/2.0,attr['phase_shift_y']/2.0]
q=[float(attr['qx'])/L,float(attr['qy'])/L]
if channel=='trans':
return sf.transfermisigns(L,L,shift,q)
elif channel=='long':
return sf.longfermisigns(L,L,shift,q)
else:
raise KeyError('\"channel\" must be either \"trans\" or \"long\".')
def bm29write(self,
filename=None,
newdata=None,
comment=True,
newdatacol_head=None,
columns=None):
"""function to write a bm29 file, define a series of array with the same name
of column defined in the file
input \n
filename =>string
newdata =>numpy array
comment =>boolean or new comments line
col_head =>string heders of column
columns =>list of strings with the columns to write
P.S or newdata and col_head or columns
"""
if not (filename):
try:
filename = getattr(self, "fullfilename")
except:
raise FileFormatError(
'no filename specified and self.fullfilenames not defined')
if os.path.exists(filename):
filename += ".1"
outFile = open(filename, 'w')
if comment is True:
if hasattr(self, "comments"):
outFile.writelines(self.comments[:-2])
elif comment is False:
pass
else:
outFile.writelines(comment)
if newdata is None:
if columns:
outFile.writelines("#N " + str(len(columns)) + "\n")
col_head = "#L " + " ".join(columns)
outFile.writelines(col_head + "\n")
f = lambda x: getattr(self, x)
newdata = scipy.column_stack(map(f, columns))
else:
if self.All_Column == False:
outFile.writelines("#N 2\n")
outFile.writelines("#L E Mu\n")
newdata = scipy.column_stack((self.E, self.Mu))
elif self.All_Column == True:
try:
outFile.writelines(self.comments[-2])
outFile.write("#L " +
" ".join(getattr(self, "col_head")))
outFile.write("\n")
newdata = self.data
except:
pass
scipy.savetxt(outFile, newdata, fmt='%1.10f')
outFile.close
return
def __init__(self,ionoin,configfile,timein=None,mattype='matrix'):
""" This will create the RadarSpaceTimeOperator object.
Inputs
ionoin - The input ionocontainer. This can be either an string that is a ionocontainer file,
a list of ionocontainer objects or a list a strings to ionocontainer files.
config - The ini file that used to set up the simulation.
timein - A Ntx2 numpy array of times.
RSTOPinv - The inverse operator object.
invmat - The inverse matrix to the original operator.
"""
mattype=mattype.lower()
accepttypes=['matrix','sim','real']
if not mattype in accepttypes:
raise ValueError('Matrix type can only be {0}'.format(', '.join(accepttypes)))
d2r = sp.pi/180.0
(sensdict,simparams) = readconfigfile(configfile)
# determine if the input ionocontainer is a string, a list of strings or a list of ionocontainers.
ionoin=makeionocombined(ionoin)
#Input location
self.Cart_Coords_In = ionoin.Cart_Coords
self.Sphere_Coords_In = ionoin.Sphere_Coords
# Set the input times
if timein is None:
self.Time_In = ionoin.Time_Vector
else:
self.Time_In = timein
#Create an array of output location based off of the inputs
rng_vec2 = simparams['Rangegatesfinal']
nrgout = len(rng_vec2)
angles = simparams['angles']
nang =len(angles)
ang_data = sp.array([[iout[0],iout[1]] for iout in angles])
rng_all = sp.repeat(rng_vec2,(nang),axis=0)
ang_all = sp.tile(ang_data,(nrgout,1))
self.Sphere_Coords_Out = sp.column_stack((rng_all,ang_all))
(R_vec,Az_vec,El_vec) = (self.Sphere_Coords_Out[:,0],self.Sphere_Coords_Out[:,1],
self.Sphere_Coords_Out[:,2])
xvecmult = sp.sin(Az_vec*d2r)*sp.cos(El_vec*d2r)
yvecmult = sp.cos(Az_vec*d2r)*sp.cos(El_vec*d2r)
zvecmult = sp.sin(El_vec*d2r)
X_vec = R_vec*xvecmult
Y_vec = R_vec*yvecmult
Z_vec = R_vec*zvecmult
self.Cart_Coords_Out = sp.column_stack((X_vec,Y_vec,Z_vec))
self.Time_Out = sp.column_stack((simparams['Timevec'],simparams['Timevec']+simparams['Tint']))+self.Time_In[0,0]
self.simparams=simparams
self.sensdict=sensdict
self.lagmat = self.simparams['amb_dict']['WttMatrix']
self.mattype=mattype
# create the matrix
(self.RSTMat,self.overlaps,self.blocklocs) = makematPA(ionoin.Sphere_Coords,ionoin.Cart_Coords,ionoin.Time_Vector,configfile,ionoin.Velocity,mattype)
def makedata(testpath, tint):
""" This will make the input data for the test case. The data will have cases
where there will be enhancements in Ne, Ti and Te in one location. Each
case will have 3 integration periods. The first 3 integration periods will
be the default set of parameters Ne=Ne=1e11 and Te=Ti=2000.
Inputs
testpath - Directory that will hold the data.
tint - The integration time in seconds.
"""
testpath = Path(testpath).expanduser()
finalpath = testpath.joinpath('Origparams')
if not finalpath.is_dir():
finalpath.mkdir()
data = sp.array([[1e11, 1100.], [1e11, 2100.]])
z = (50. + sp.arange(50) * 10.)
nz = len(z)
params = sp.tile(data[sp.newaxis, sp.newaxis], (nz, 1, 1, 1))
epnt = range(20, 22)
p2 = sp.tile(params, (1, 4, 1, 1))
#enhancement in Ne
p2[epnt, 1, :, 0] = 5e11
#enhancement in Ti
p2[epnt, 2, 0, 1] = 2200.
#enhancement in Te
p2[epnt, 3, 1, 1] = 4200.
coords = sp.column_stack((sp.ones(nz), sp.ones(nz), z))
species = ['O+', 'e-']
times = sp.array([[0, 1e3]])
times2 = sp.column_stack((sp.arange(0, 4), sp.arange(1, 5))) * 3 * tint
vel = sp.zeros((nz, 1, 3))
vel2 = sp.zeros((nz, 4, 3))
Icontstart = IonoContainer(coordlist=coords,
paramlist=params,
times=times,
sensor_loc=sp.zeros(3),
ver=0,
coordvecs=['x', 'y', 'z'],
paramnames=None,
species=species,
velocity=vel)
Icont1 = IonoContainer(coordlist=coords,
paramlist=p2,
times=times2,
sensor_loc=sp.zeros(3),
ver=0,
coordvecs=['x', 'y', 'z'],
paramnames=None,
species=species,
velocity=vel2)
finalfile = finalpath.joinpath('0 stats.h5')
Icont1.saveh5(str(finalfile))
Icontstart.saveh5(str(testpath.joinpath('startfile.h5')))
def writeCSVOutput(hdf5File=None,cout=None):
f = h5py.File(hdf5File,'r')
csv_filename = os.path.join(cout,f['phenotype_name'].value.replace(" ","_") + ".csv")
csv_header = None
csv_matrix = None
if "betas" in f.keys():
csv_header = sp.array(["CHR","Positions","P-Value","TestStatistic","Q-Value","Benjamini-Hochberg-P-Value","Benjamini-Hochberg-Yekutieli-P-Value","Beta0","SEBeta0","Beta1","SEBeta1","MAF","SNP-Hash"])
else:
csv_header = sp.array(["CHR","Positions","P-Value","TestStatistic","Q-Value","Benjamini-Hochberg-P-Value","Benjamini-Hochberg-Yekutieli-P-Value","MAF","SNP-Hash"])
tmp_matrix = None
if "betas" in f.keys():
tmp_matrix = sp.column_stack([sp.array(f["chromosomes"],dtype="S50"),
f['positions'],
f['p_values'],
f['scores'],
f['q_values'],
f['bh_p_values'],
f['bhy_p_values'],
f['betas'][:,0],
f['betas_se'][:,0],
f['betas'][:,1],
f['betas_se'][:,1],
f['maf'],
f['snp_hash']])
else:
tmp_matrix = sp.column_stack([sp.array(f["chromosomes"],dtype="S50"),
f['positions'],
f['p_values'],
f['scores'],
f['q_values'],
f['bh_p_values'],
f['bhy_p_values'],
f['maf'],
f['snp_hash']])
csv_matrix = tmp_matrix
mf = open(csv_filename,'w')
string = ""
for i in xrange(csv_header.shape[0]):
string += str(csv_header[i]) + ","
mf.write(string[:-1] + "\n")
for i in xrange(csv_matrix.shape[0]):
string = ""
for j in xrange(csv_matrix.shape[1]):
string += str(csv_matrix[i,j]) + ","
mf.write(string[:-1] + "\n")
mf.close()
f.close()
def bm29write(self, filename= None, newdata=None, comment=True, newdatacol_head=None, columns=None):
"""function to write a bm29 file, define a series of array with the same name
of column defined in the file
input \n
filename =>string
newdata =>numpy array
comment =>boolean or new comments line
col_head =>string heders of column
columns =>list of strings with the columns to write
P.S or newdata and col_head or columns
"""
if not(filename):
try:
filename =getattr(self,"fullfilename")
except:
raise FileFormatError('no filename specified and self.fullfilenames not defined')
if os.path.exists(filename):
filename += ".1"
outFile = open(filename, 'w')
if comment is True:
if hasattr(self, "comments"):
outFile.writelines(self.comments[:-2])
elif comment is False:
pass
else: outFile.writelines(comment)
if newdata is None:
if columns:
outFile.writelines("#N "+str(len(columns))+ "\n")
col_head= "#L "+" ".join(columns)
outFile.writelines(col_head+"\n")
f=lambda x: getattr(self,x)
newdata= scipy.column_stack(map(f,columns))
else:
if self.All_Column == False:
outFile.writelines("#N 2\n")
outFile.writelines("#L E Mu\n")
newdata= scipy.column_stack((self.E, self.Mu))
elif self.All_Column == True:
try:
outFile.writelines(self.comments[-2])
outFile.write("#L "+" ".join(getattr(self, "col_head")))
outFile.write("\n")
newdata = self.data
except:
pass
scipy.savetxt(outFile, newdata, fmt= '%1.10f')
outFile.close
return
def create_csv(file_path=None, csv_filename=None):
f = h5py.File(file_path, 'r')
csv_filename = os.path.join(
csv_filename, f['phenotype_name'].value.replace(" ", "_") + ".csv")
csv_header = None
csv_matrix = None
if "betas" in f.keys():
csv_header = sp.array([
"CHR", "Positions", "P-Value", "TestStatistic", "Q-Value",
"Benjamini-Hochberg-P-Value",
"Benjamini-Hochberg-Yekutieli-P-Value", "Beta0", "SEBeta0",
"Beta1", "SEBeta1", "MAF", "SNP-Hash"
])
else:
csv_header = sp.array([
"CHR", "Positions", "P-Value", "TestStatistic", "Q-Value",
"Benjamini-Hochberg-P-Value",
"Benjamini-Hochberg-Yekutieli-P-Value", "MAF", "SNP-Hash"
])
tmp_matrix = None
if "betas" in f.keys():
tmp_matrix = sp.column_stack([
sp.array(f["chromosomes"], dtype="S50"), f['positions'],
f['p_values'], f['scores'], f['q_values'], f['bh_p_values'],
f['bhy_p_values'], f['betas'][:, 0], f['betas_se'][:, 0],
f['betas'][:, 1], f['betas_se'][:, 1], f['maf'], f['snp_hash']
])
else:
tmp_matrix = sp.column_stack([
sp.array(f["chromosomes"], dtype="S50"), f['positions'],
f['p_values'], f['scores'], f['q_values'], f['bh_p_values'],
f['bhy_p_values'], f['maf'], f['snp_hash']
])
csv_matrix = tmp_matrix
mf = open(csv_filename, 'w')
string = ""
for i in xrange(csv_header.shape[0]):
string += str(csv_header[i]) + ","
mf.write(string[:-1] + "\n")
for i in xrange(csv_matrix.shape[0]):
string = ""
for j in xrange(csv_matrix.shape[1]):
string += str(csv_matrix[i, j]) + ","
mf.write(string[:-1] + "\n")
mf.close()
f.close()
def pyglowinput(
latlonalt=[65.1367, -147.4472, 250.00],
dn_list=[datetime(2015, 3, 21, 8, 00),
datetime(2015, 3, 21, 20, 00)],
z=None):
if z is None:
z = sp.linspace(50., 1000., 200)
dn_diff = sp.diff(dn_list)
dn_diff_sec = dn_diff[-1].seconds
timelist = sp.array([calendar.timegm(i.timetuple()) for i in dn_list])
time_arr = sp.column_stack((timelist, sp.roll(timelist, -1)))
time_arr[-1, -1] = time_arr[-1, 0] + dn_diff_sec
v = []
coords = sp.column_stack((sp.zeros((len(z), 2), dtype=z.dtype), z))
all_spec = ['O+', 'NO+', 'O2+', 'H+', 'HE+']
Param_List = sp.zeros((len(z), len(dn_list), len(all_spec), 2))
for idn, dn in enumerate(dn_list):
for iz, zcur in enumerate(z):
latlonalt[2] = zcur
pt = Point(dn, *latlonalt)
pt.run_igrf()
pt.run_msis()
pt.run_iri()
# so the zonal pt.u and meriodinal winds pt.v will coorispond to x and y even though they are
# supposed to be east west and north south. Pyglow does not seem to have
# vertical winds.
v.append([pt.u, pt.v, 0])
for is1, ispec in enumerate(all_spec):
Param_List[iz, idn, is1, 0] = pt.ni[ispec] * 1e6
Param_List[iz, idn, :, 1] = pt.Ti
Param_List[iz, idn, -1, 0] = pt.ne * 1e6
Param_List[iz, idn, -1, 1] = pt.Te
Param_sum = Param_List[:, :, :, 0].sum(0).sum(0)
spec_keep = Param_sum > 0.
species = sp.array(all_spec)[spec_keep[:-1]].tolist()
species.append('e-')
Param_List[:, :] = Param_List[:, :, spec_keep]
Iono_out = IonoContainer(coords,
Param_List,
times=time_arr,
species=species)
return Iono_out
def readMahalih5(filename,des_site):
""" This function will read the mahali GPS data into a GeoData data structure.
The user only has to give a filename and name of the desired site.
Input
filename - A string that holds the file name.
des_site - The site name. Should be listed in the h5 file in the
table sites.
"""
h5fn = Path(filename).expanduser()
with h5py.File(str(h5fn), "r", libver='latest') as f:
despnts = sp.where(f['data']['site']==des_site)[0]
# TODO: hard coded for now
doy = doy= f['data']['time'][despnts]
year = 2015*sp.ones_like(doy,dtype=int)
TEC = f['data']['los_tec'][despnts]
nTEC = f['data']['err_los_tec'][despnts]
vTEC = f['data']['vtec'][despnts]
az2sat = f['data']['az'][despnts]
el2sat = f['data']['az'][despnts]
piercelat = f['data']['pplat'][despnts]
piercelong = f['data']['pplon'][despnts]
satnum= f['data']['prn'][despnts]
recBias = f['data']['rec_bias'][despnts]
nrecBias = f['data']['err_rec_bias'][despnts]
# Make the integration time on the order of 15 seconds.
if (year==year[1]).all():
unixyear =(datetime(year[0],1,1,0,0,0,tzinfo=UTC) - EPOCH).total_seconds()
uttime = unixyear + sp.round_(24*3600*sp.column_stack((doy,doy+15./24./3600.))) # Making the difference in time to be a minute
else:
(y_u,y_iv) = np.unique(year,return_inverse=True)
unixyearu = sp.array([(datetime(iy,1,1,0,0,0,tzinfo=UTC) - EPOCH).total_seconds() for iy in y_u])
unixyear = unixyearu[y_iv]
uttime = unixyear + 24*3600*sp.column_stack((doy,doy+15./24./3600.))
data = {'TEC':TEC,'nTEC':nTEC,'vTEC':vTEC,'recBias':recBias,'nrecBias':nrecBias,'satnum':satnum,'az2sat':az2sat,'el2sat':el2sat}
coordnames = 'WGS84'
sensorloc = sp.nan*sp.ones(3)
dataloc = sp.column_stack((piercelat,piercelong, 350e3*sp.ones_like(piercelat)))
return (data,coordnames,dataloc,sensorloc,uttime)
def readMahalih5(filename,des_site):
""" This function will read the mahali GPS data into a GeoData data structure.
The user only has to give a filename and name of the desired site.
Input
filename - A string that holds the file name.
des_site - The site name. Should be listed in the h5 file in the
table sites.
"""
h5fn = Path(filename).expanduser()
with h5py.File(str(h5fn), "r", libver='latest') as f:
despnts = sp.where(f['data']['site']==des_site)[0]
# TODO: hard coded for now
doy = doy= f['data']['time'][despnts]
year = 2015*sp.ones_like(doy,dtype=int)
TEC = f['data']['los_tec'][despnts]
nTEC = f['data']['err_los_tec'][despnts]
vTEC = f['data']['vtec'][despnts]
az2sat = f['data']['az'][despnts]
el2sat = f['data']['az'][despnts]
piercelat = f['data']['pplat'][despnts]
piercelong = f['data']['pplon'][despnts]
satnum= f['data']['prn'][despnts]
recBias = f['data']['rec_bias'][despnts]
nrecBias = f['data']['err_rec_bias'][despnts]
# Make the integration time on the order of 15 seconds.
if (year==year[1]).all():
unixyear =(datetime(year[0],1,1,0,0,0,tzinfo=UTC) - EPOCH).total_seconds()
uttime = unixyear + sp.round_(24*3600*sp.column_stack((doy,doy+15./24./3600.))) # Making the difference in time to be a minute
else:
(y_u,y_iv) = np.unique(year,return_inverse=True)
unixyearu = sp.array([(datetime(iy,1,1,0,0,0,tzinfo=UTC) - EPOCH).total_seconds() for iy in y_u])
unixyear = unixyearu[y_iv]
uttime = unixyear + 24*3600*sp.column_stack((doy,doy+15./24./3600.))
data = {'TEC':TEC,'nTEC':nTEC,'vTEC':vTEC,'recBias':recBias,'nrecBias':nrecBias,'satnum':satnum,'az2sat':az2sat,'el2sat':el2sat}
coordnames = 'WGS84'
sensorloc = sp.nan*sp.ones(3)
dataloc = sp.column_stack((piercelat,piercelong, 350e3*sp.ones_like(piercelat)))
return (data,coordnames,dataloc,sensorloc,uttime)
def makedata(testpath):
"""
This will make the input data for the test case. The data will have the
default set of parameters Ne=Ne=1e11 and Te=Ti=2000.
Inputs
testpath - Directory that will hold the data.
"""
finalpath = testpath.joinpath('Origparams')
if not finalpath.exists():
finalpath.mkdir()
data = SIMVALUES
z = sp.linspace(50., 1e3, 50)
nz = len(z)
params = sp.tile(data[sp.newaxis, sp.newaxis, :, :], (nz, 1, 1, 1))
coords = sp.column_stack((sp.ones(nz), sp.ones(nz), z))
species = ['O+', 'e-']
times = sp.array([[0, 1e9]])
vel = sp.zeros((nz, 1, 3))
Icont1 = IonoContainer(coordlist=coords,
paramlist=params,
times=times,
sensor_loc=sp.zeros(3),
ver=0,
coordvecs=['x', 'y', 'z'],
paramnames=None,
species=species,
velocity=vel)
finalfile = finalpath.joinpath('0 stats.h5')
Icont1.saveh5(str(finalfile))
# set start temp to 1000 K.
Icont1.Param_List[:, :, :, 1] = 1e3
Icont1.saveh5(str(testpath.joinpath('startfile.h5')))
def main():
saved_handler = sp.seterrcall(err_handler)
saved_err = sp.seterr(all='call')
print('============ Part 1: Plotting =============================')
x, y = load_data('ex2/ex2data1.txt')
plot_data(x, y)
pl.show()
print('============ Part 2: Compute Cost and Gradient ============')
m, n = x.shape
x = sp.column_stack((sp.ones((m, 1)), x))
init_theta = sp.asmatrix(sp.zeros((n + 1, 1)))
cost, grad = cost_function(init_theta, x, y)
print('Cost at initial theta: %s' % cost)
print('Gradient at initial theta:\n %s' % grad)
print('============ Part 3: Optimizing minimize ====================')
# res = op.minimize(cost_function, init_theta, args=(x, y), jac=True, method='Newton-CG')
res = op.minimize(cost_function_without_grad, init_theta, args=(x, y), method='Powell')
# print('Cost at theta found by fmin: %s' % cost)
print('Result by minimize:\n%s' % res)
plot_decision_boundary(res.x, x, y)
pl.show()
print('============ Part 4: Optimizing fmin ====================')
res = op.fmin(cost_function_without_grad, init_theta, args=(x, y))
# print('Cost at theta found by fmin: %s' % cost)
print('Result by fmin:\n%s' % res)
plot_decision_boundary(res, x, y)
pl.show()
sp.seterrcall(saved_handler)
sp.seterr(**saved_err)
def makedata(testpath):
""" This will make the input data for the test case. The data will have the
default set of parameters Ne=Ne=1e11 and Te=Ti=2000.
Inputs
testpath - Directory that will hold the data.
"""
finalpath = testpath.joinpath('Origparams')
if not finalpath.exists():
finalpath.mkdir()
data=SIMVALUES
z = sp.linspace(50.,1e3,50)
nz = len(z)
params = sp.tile(data[sp.newaxis,sp.newaxis,:,:],(nz,1,1,1))
coords = sp.column_stack((sp.ones(nz),sp.ones(nz),z))
species=['O+','e-']
times = sp.array([[0,1e3]])
vel = sp.zeros((nz,1,3))
Icont1 = IonoContainer(coordlist=coords,paramlist=params,times = times,sensor_loc = sp.zeros(3),ver =0,coordvecs =
['x','y','z'],paramnames=None,species=species,velocity=vel)
finalfile = finalpath.joinpath('0 stats.h5')
Icont1.saveh5(str(finalfile))
# set start temp to 1000 K.
Icont1.Param_List[:,:,:,1]=1e3
Icont1.saveh5(str(testpath.joinpath('startfile.h5')))
def apply_flow(self,flowrate):
r'''
Convert the invaded sequence into an invaded time for a given flow rate
considering the volume of invaded pores and throats.
Parameters
----------
flowrate : float
The flow rate of the injected fluid
Returns
-------
Creates a throat array called 'invasion_time' in the Algorithm
dictionary
'''
P12 = self._net['throat.conns'] # List of throats conns
a = self['throat.invasion_sequence'] # Invasion sequence
b = sp.argsort(self['throat.invasion_sequence'])
P12_inv = self['pore.invasion_sequence'][P12] # Pore invasion sequence
# Find if the connected pores were invaded with or before each throat
P1_inv = P12_inv[:,0] == a
P2_inv = P12_inv[:,1] == a
c = sp.column_stack((P1_inv,P2_inv))
d = sp.sum(c,axis=1,dtype=bool) # List of Pores invaded with each throat
# Find volume of these pores
P12_vol = sp.zeros((self.Nt,))
P12_vol[d] = self._net['pore.volume'][P12[c]]
# Add invaded throat volume to pore volume (if invaded)
T_vol = P12_vol + self._net['throat.volume']
# Cumulative sum on the sorted throats gives cumulated inject volume
e = sp.cumsum(T_vol[b]/flowrate)
t = sp.zeros((self.Nt,))
t[b] = e # Convert back to original order
self._phase['throat.invasion_time'] = t
def apply_flow(self, flowrate):
r"""
Convert the invaded sequence into an invaded time for a given flow rate
considering the volume of invaded pores and throats.
Parameters
----------
flowrate : float
The flow rate of the injected fluid
Returns
-------
Creates a throat array called 'invasion_time' in the Algorithm
dictionary
"""
P12 = self._net['throat.conns']
a = self['throat.invasion_sequence']
b = sp.argsort(self['throat.invasion_sequence'])
P12_inv = self['pore.invasion_sequence'][P12]
# Find if the connected pores were invaded with or before each throat
P1_inv = P12_inv[:, 0] == a
P2_inv = P12_inv[:, 1] == a
c = sp.column_stack((P1_inv, P2_inv))
d = sp.sum(c, axis=1, dtype=bool) # List of Pores invaded with each throat
# Find volume of these pores
P12_vol = sp.zeros((self.Nt,))
P12_vol[d] = self._net['pore.volume'][P12[c]]
# Add invaded throat volume to pore volume (if invaded)
T_vol = P12_vol + self._net['throat.volume']
# Cumulative sum on the sorted throats gives cumulated inject volume
e = sp.cumsum(T_vol[b] / flowrate)
t = sp.zeros((self.Nt,))
t[b] = e # Convert back to original order
self._phase['throat.invasion_time'] = t
def makeinputh5(Iono, basedir):
basedir = Path(basedir).expanduser()
Param_List = Iono.Param_List
dataloc = Iono.Cart_Coords
times = Iono.Time_Vector
velocity = Iono.Velocity
zlist, idx = sp.unique(dataloc[:, 2], return_inverse=True)
siz = list(Param_List.shape[1:])
vsiz = list(velocity.shape[1:])
datalocsave = sp.column_stack(
(sp.zeros_like(zlist), sp.zeros_like(zlist), zlist))
outdata = sp.zeros([len(zlist)] + siz)
outvel = sp.zeros([len(zlist)] + vsiz)
for izn, iz in enumerate(zlist):
arr = sp.argwhere(idx == izn)
outdata[izn] = sp.mean(Param_List[arr], axis=0)
outvel[izn] = sp.mean(velocity[arr], axis=0)
Ionoout = IonoContainer(datalocsave,
outdata,
times,
Iono.Sensor_loc,
ver=0,
paramnames=Iono.Param_Names,
species=Iono.Species,
velocity=outvel)
ofn = basedir / 'startdata.h5'
print('writing {}'.format(ofn))
Ionoout.saveh5(str(ofn))
def train(self):
if self.__algo_model=="MWUrt" or self.__algo_model=="WCrt":
data = asso.MatrixData(x=self.__x,y=self.__y,covariates=self.__cov)
self.__ass.setData(data)
self.__ass.train()
else:
self.__ass.setPhenotype(self.__y)
self.__ass.setGenotype(self.__x)
if not self.__cov is None:
self.__ass.setCovariates(sp.column_stack([sp.ones(self.__y.shape),self.__cov]))
if self.__permutation==True:
if self.__x.shape[1]<1000:
self.__perms = 1000000
elif self.__x.shape[1]<10000:
self.__perms = 100000
elif self.__x.shape[1]<100000:
self.__perms = 10000
elif self.__x.shape[1]<1000000:
self.__perms = 1000
elif self.__x.shape[1]<10000000:
self.__perms = 100
else:
self.__perms = 10
print "SNPS: ", self.__x.shape[1]
print "Perms: ", self.__perms
self.__ass.permutations(self.__perms)
else:
self.__ass.test_associations()
def backsolve(self, T=None, vterm=None):
"""Solve finite system by backward recursion
Parameters
-------------
T : int, optional
Number of periods of time.
Returns
----------
X : array, shape (n, T)
Optimal controls. An optimal policy for each starting state
V : array, shape (n, T + 1)
Value function.
"""
if T is None:
if self.T is not None:
T = self.T
else:
print ("Not a finite time model")
return
if vterm is None and self.vterm is None:
vterm = sp.zeros(self.n)
else:
vterm = self.vterm
x = sp.zeros((self.n, T), dtype=int)
v = sp.column_stack((sp.zeros((self.n, T)), vterm))
pstar = sp.zeros((self.n, self.n, T))
for t in sp.arange(T - 1, -1, -1):
v[ :, t] , x[ :, t] = self.valmax(v[ : , t + 1])
pstar[..., t] = self.valpol(x[:, t])[0]
return (x, v, pstar)
def train(self):
if self.__algo_model == "MWUrt" or self.__algo_model == "WCrt":
data = asso.MatrixData(x=self.__x,
y=self.__y,
covariates=self.__cov)
self.__ass.setData(data)
self.__ass.train()
else:
self.__ass.setPhenotype(self.__y)
self.__ass.setGenotype(self.__x)
if not self.__cov is None:
self.__ass.setCovariates(
sp.column_stack([sp.ones(self.__y.shape), self.__cov]))
if self.__permutation == True:
if self.__x.shape[1] < 1000:
self.__perms = 1000000
elif self.__x.shape[1] < 10000:
self.__perms = 100000
elif self.__x.shape[1] < 100000:
self.__perms = 10000
elif self.__x.shape[1] < 1000000:
self.__perms = 1000
elif self.__x.shape[1] < 10000000:
self.__perms = 100
else:
self.__perms = 10
print "SNPS: ", self.__x.shape[1]
print "Perms: ", self.__perms
self.__ass.permutations(self.__perms)
else:
self.__ass.test_associations()
def kmeanspp_initialisation( self, X ):
"""Initialise means using K-Means++"""
N, _ = X.shape
k, d = self.k, self.d
M = []
# Choose one center amongst the X at random
m = sc.random.randint( N )
M.append( X[m] )
# Choose k centers
while( len( M ) < self.k ):
# Create a probability distribution D^2 from the previous mean
D = cdist( X, M ).min( 1 )**2
assert( D.shape == (N,) )
# Normalise and sample a new point
D /= D.sum()
m = sc.random.multinomial( 1, D ).argmax()
M.append( X[m] )
M = sc.column_stack( M )
sigma = sc.sqrt(cdist( X, M.T, 'sqeuclidean').sum(0)/(N))
w = ones( k )/float(k)
return M, sigma, w
def PathSPCA(A, k):
M, N = A.shape
# Loop through variables
As = ((A * A).sum(axis=0))
vmax = As.max()
vp = As.argmax()
subset = [vp]
vars = []
res = subset
rhos = [(A[:, vp] * A[:, vp]).sum()]
Stemp = array([rhos])
for i in range(1, k):
lev, v = la.eig(Stemp)
vars.append(real(lev).max())
vp = real(lev).argmax()
x = dot(A[:, subset], v[:, vp])
x = x / la.norm(x)
seto = list(range(0, N))
for j in subset:
seto.remove(j)
vals = dot(x.T, A[:, seto])
vals = vals * vals
rhos.append(vals.max())
vpo = seto[vals.argmax()]
Stemp = column_stack((Stemp, dot(A[:, subset].T, A[:, vpo])))
vbuf = append(dot(A[:, vpo].T, A[:, subset]),
array([(A[:, vpo] * A[:, vpo]).sum()]))
Stemp = row_stack((Stemp, vbuf))
subset.append(vpo)
lev, v = la.eig(Stemp)
vars.append(real(lev).max())
return vars, res, rhos
def makeinputh5(Iono,basedir):
basedir = Path(basedir).expanduser()
Param_List = Iono.Param_List
dataloc = Iono.Cart_Coords
times = Iono.Time_Vector
velocity = Iono.Velocity
zlist,idx = sp.unique(dataloc[:,2],return_inverse=True)
siz = list(Param_List.shape[1:])
vsiz = list(velocity.shape[1:])
datalocsave = sp.column_stack((sp.zeros_like(zlist),sp.zeros_like(zlist),zlist))
outdata = sp.zeros([len(zlist)]+siz)
outvel = sp.zeros([len(zlist)]+vsiz)
for izn,iz in enumerate(zlist):
arr = sp.argwhere(idx==izn)
outdata[izn]=sp.mean(Param_List[arr],axis=0)
outvel[izn]=sp.mean(velocity[arr],axis=0)
Ionoout = IonoContainer(datalocsave,outdata,times,Iono.Sensor_loc,ver=0,
paramnames=Iono.Param_Names, species=Iono.Species,velocity=outvel)
ofn = basedir/'startdata.h5'
print('writing {}'.format(ofn))
Ionoout.saveh5(str(ofn))
def generate_data_case(sigma, beta, rho, N, t_delta, x, y, z):
"""
Generate output data for a given case for later processing. The output
is a 2D array containing the all the states and the conditions
used to generate them as columns for the given case. This will simplify
the processing and plotting at a later stage.
Input:
sigma: Integer for the sigma attractor parameter
beta: Float64 for the beta attractor parameter
rho: Integer for the rho attractor parameter
N: Integer for the total number of steps of the solver
t_delta: Float64 for the step size of the solver
x: Scipy array for the x-positions
y: Scipy array for the y-positions
z: Scipy array for the z-positions
"""
S = sigma * sp.ones([N, 1])
B = beta * sp.ones([N, 1])
R = rho * sp.ones([N, 1])
Na = N * sp.ones([N, 1])
T = t_delta * sp.ones([N, 1])
data = sp.column_stack((S, B, R, Na, T, x, y, z))
return data
def kmeanspp_initialisation(self, X):
"""Initialise means using K-Means++"""
N, _ = X.shape
k, d = self.k, self.d
M = []
# Choose one center amongst the X at random
m = sc.random.randint(N)
M.append(X[m])
# Choose k centers
while (len(M) < self.k):
# Create a probability distribution D^2 from the previous mean
D = cdist(X, M).min(1)**2
assert (D.shape == (N, ))
# Normalise and sample a new point
D /= D.sum()
m = sc.random.multinomial(1, D).argmax()
M.append(X[m])
M = sc.column_stack(M)
sigma = sc.sqrt(cdist(X, M.T, 'sqeuclidean').sum(0) / (N))
w = ones(k) / float(k)
return M, sigma, w
def get_data():
# data is a 2d array which now contains the data
data = sp.genfromtxt(os.path.join(DATA_DIR, "visitors_per_hour.txt"),
delimiter="\t")
temp = data[0:740 * 24, 1]
temp_1 = data[0:740 * 24, 0]
day = sp.arange(1, 366, 1)
#print(day)
hits = data[0:731, 1]
#print(temp)
# Cleaning the data i.e. removing NAN values if present
temp = temp[~sp.isnan(temp)]
for i in range(1, len(temp)):
temp_1[i - 1] = temp[i] - temp[i - 1]
#print(temp_1)
for i in range(0, 731):
x = 0
for j in range(0, 24):
x += temp_1[i * 24 + j]
hits[i] = x
sp.savetxt(os.path.join(DATA_DIR, "visitors_per_day_train.txt"),
sp.column_stack([day.astype(int), hits[0:365].astype(int)]),
fmt='%.18g',
delimiter=' ')
return [day, hits]
def makeinputh5(Iono,basedir):
"""This will make a h5 file for the IonoContainer that can be used as starting
points for the fitter. The ionocontainer taken will be average over the x and y dimensions
of space to make an average value of the parameters for each altitude.
Inputs
Iono - An instance of the Ionocontainer class that will be averaged over so it can
be used for fitter starting points.
basdir - A string that holds the directory that the file will be saved to.
"""
# Get the parameters from the original data
Param_List = Iono.Param_List
dataloc = Iono.Cart_Coords
times = Iono.Time_Vector
velocity = Iono.Velocity
zlist,idx = sp.unique(dataloc[:,2],return_inverse=True)
siz = list(Param_List.shape[1:])
vsiz = list(velocity.shape[1:])
datalocsave = sp.column_stack((sp.zeros_like(zlist),sp.zeros_like(zlist),zlist))
outdata = sp.zeros([len(zlist)]+siz)
outvel = sp.zeros([len(zlist)]+vsiz)
# Do the averaging across space
for izn,iz in enumerate(zlist):
arr = sp.argwhere(idx==izn)
outdata[izn]=sp.mean(Param_List[arr],axis=0)
outvel[izn]=sp.mean(velocity[arr],axis=0)
Ionoout = IonoContainer(datalocsave,outdata,times,Iono.Sensor_loc,ver=0,
paramnames=Iono.Param_Names, species=Iono.Species,velocity=outvel)
Ionoout.saveh5(os.path.join(basedir,'startdata.h5'))
def run(self):
# Parameters passed are current data array, along with time step
# between current data points
self.times = sp.arange(0,self.Tfinal,self.dt)
self.sim = odeint(self.eqns,self.init,self.times,(self.inj,self.injdt))
sp.savetxt('simulation.txt',sp.column_stack((self.times,self.sim)))
def recover_topics( P, T, k, a0 ):
"""Recover the k components given input Pairs and Triples and
$\\alpha_0$"""
# Consider the k rank approximation of P,
P = approxk( P, k )
# Get the whitening matrix and coloring matrices
W, Wt = get_whitener( P, k )
# Whiten the third moment
Tw = lambda theta: W.T.dot( T( W.dot(theta) ) ).dot( W )
# Project Tw onto a matrix
theta = orthogonal( k ).T[0]
U, S, _ = svd( Tw( theta ) )
assert( (S > 1e-10).all() ) # Make sure it is non-singular
O = []
for i in xrange( k ):
v = U.T[i]
Zinv = (a0 + 2)/2 * (v.T.dot(Tw(v)).dot(v))
O.append( Zinv * Wt.T.dot( v ) )
O = sc.column_stack( O )
return abs( O )
def makeinputh5(Iono,basedir):
"""This will make a h5 file for the IonoContainer that can be used as starting
points for the fitter. The ionocontainer taken will be average over the x and y dimensions
of space to make an average value of the parameters for each altitude.
Inputs
Iono - An instance of the Ionocontainer class that will be averaged over so it can
be used for fitter starting points.
basdir - A string that holds the directory that the file will be saved to.
"""
# Get the parameters from the original data
Param_List = Iono.Param_List
dataloc = Iono.Cart_Coords
times = Iono.Time_Vector
velocity = Iono.Velocity
zlist,idx = sp.unique(dataloc[:,2],return_inverse=True)
siz = list(Param_List.shape[1:])
vsiz = list(velocity.shape[1:])
datalocsave = sp.column_stack((sp.zeros_like(zlist),sp.zeros_like(zlist),zlist))
outdata = sp.zeros([len(zlist)]+siz)
outvel = sp.zeros([len(zlist)]+vsiz)
# Do the averaging across space
for izn,iz in enumerate(zlist):
arr = sp.argwhere(idx==izn)
outdata[izn] = sp.mean(Param_List[arr],axis=0)
outvel[izn] = sp.mean(velocity[arr],axis=0)
Ionoout = IonoContainer(datalocsave,outdata,times,Iono.Sensor_loc,ver=0,
paramnames=Iono.Param_Names, species=Iono.Species,velocity=outvel)
Ionoout.saveh5(basedir/'startdata.h5')
def historial():
"""Funcion que permite graficar la energia a lo largo del tiempo especificiado por el usuario"""
global EnergiaK, EnergiaP, EnergiaT
t = dt * np.arange(npasos_temporales + 1)
plt.figure('Energias del sistema')
plt.title('Energies')
plt.plot(t, EnergiaP, 'b', label='Potential')
plt.plot(t, EnergiaK, 'r', label='Kinetic')
plt.plot(t, EnergiaT, 'black', label='Total')
plt.xlabel('t', fontsize=18)
plt.xticks(np.linspace(0, 14, 6), fontsize=18)
plt.yticks(np.linspace(0, 35e-7, 6), fontsize=18)
plt.ylim(0, 40e-7)
plt.xlim(0, 14)
plt.legend(loc=1)
plt.ticklabel_format(style='sci', axis='y', scilimits=(0, 0))
plt.figure('Potential Energy')
plt.plot(t, EnergiaP, 'b')
plt.xlabel('t', fontsize=18)
plt.ylabel('Ex Energy', fontsize=18)
plt.xticks(np.linspace(0, 100, 11), fontsize=18)
plt.yticks(np.linspace(0, 16, 8), fontsize=18)
plt.xlim(0, 100)
plt.ylim(0, 25)
if os.path.exists("Energias") and\
os.path.isfile("Energias/Energias.png")==\
True:
os.remove("Energias/Energias.png")
plt.savefig('Energias.png', dpi=720)
shutil.move('Energias.png', "Energias")
os.remove("Energias/energies.out")
# Escribe y guarda el archivo con los valores de la energia en el tiempo:
sp.savetxt('energies.out',
sp.column_stack((t, EnergiaP, EnergiaK, EnergiaT)),
fmt=('%1.4e', '%1.4e', '%1.4e', '%1.4e'))
shutil.move('energies.out', "Energias")
else:
os.mkdir("Energias")
plt.savefig('Energias.png', dpi=720)
shutil.move('Energias.png', "Energias")
# Escribe y guarda el archivo con los valores de la energia en el tiempo:
sp.savetxt('energies.out',
sp.column_stack((t, EnergiaP, EnergiaK, EnergiaT)),
fmt=('%1.4e', '%1.4e', '%1.4e', '%1.4e'))
shutil.move('energies.out', "Energias")
def analysisdump(maindir, configfile, suptitle=None):
""" This function will perform all of the plotting functions in this module
given the main directory that all of the files live.
Inputs
maindir - The directory for the simulation.
configfile - The name of the configuration file used.
suptitle - The supertitle used on the files.
"""
maindir = Path(maindir)
plotdir = maindir.joinpath("AnalysisPlots")
if not plotdir.is_dir():
plotdir.mkdir()
# plot spectrums
filetemplate1 = str(maindir.joinpath("AnalysisPlots", "Spec"))
filetemplate3 = str(maindir.joinpath("AnalysisPlots", "ACF"))
filetemplate4 = str(maindir.joinpath("AnalysisPlots", "AltvTime"))
(sensdict, simparams) = readconfigfile(configfile)
angles = simparams["angles"]
ang_data = sp.array([[iout[0], iout[1]] for iout in angles])
if not sensdict["Name"].lower() in ["risr", "pfisr"]:
ang_data_temp = ang_data.copy()
beamlistlist = sp.array(simparams["outangles"]).astype(int)
ang_data = sp.array([ang_data_temp[i].mean(axis=0) for i in beamlistlist])
zenang = ang_data[sp.argmax(ang_data[:, 1])]
rnggates = simparams["Rangegatesfinal"]
rngchoices = sp.linspace(sp.amin(rnggates), sp.amax(rnggates), 4)
angtile = sp.tile(zenang, (len(rngchoices), 1))
coords = sp.column_stack((sp.transpose(rngchoices), angtile))
times = simparams["Timevec"]
filetemplate2 = str(maindir.joinpath("AnalysisPlots", "Params"))
if simparams["Pulsetype"].lower() == "barker":
params = ["Ne"]
if suptitle is None:
plotbeamparametersv2(times, configfile, maindir, params=params, filetemplate=filetemplate2, werrors=True)
else:
plotbeamparametersv2(
times, configfile, maindir, params=params, filetemplate=filetemplate2, suptitle=suptitle, werrors=True
)
else:
params = ["Ne", "Nepow", "Te", "Ti", "Vi"]
if suptitle is None:
plotspecs(coords, times, configfile, maindir, cartcoordsys=False, filetemplate=filetemplate1)
plotacfs(coords, times, configfile, maindir, cartcoordsys=False, filetemplate=filetemplate3)
plotbeamparametersv2(times, configfile, maindir, params=params, filetemplate=filetemplate2, werrors=True)
beamvstime(configfile, maindir, params=params, filetemplate=filetemplate4)
else:
plotspecs(
coords, times, configfile, maindir, cartcoordsys=False, filetemplate=filetemplate1, suptitle=suptitle
)
plotacfs(
coords, times, configfile, maindir, cartcoordsys=False, filetemplate=filetemplate3, suptitle=suptitle
)
plotbeamparametersv2(
times, configfile, maindir, params=params, filetemplate=filetemplate2, suptitle=suptitle, werrors=True
)
beamvstime(configfile, maindir, params=params, filetemplate=filetemplate4, suptitle=suptitle)
def getColourFeatures(df):
BV = sp.array(df["BV"].tolist())
BR = sp.array(df["BR"].tolist())
BI = sp.array(df["BI"].tolist())
VR = sp.array(df["VR"].tolist())
VI = sp.array(df["VI"].tolist())
RI = sp.array(df["RI"].tolist())
return sp.column_stack((BV, BR, BI, VR, VI, RI))
def generate_Custom(cleaned, file_name, line_count, state_th, state_tth, state_chi, state_phi, state_x, state_y, state_temp,
start, stop):
line_count = int(line_count)
start = int(start)
stop = int(stop)
temperature = cleaned[:,0] - 273
chi = cleaned[:,1]
phi = cleaned[:,2]
tx = cleaned[:,3]
ty = cleaned[:,4]
om = cleaned[:,5]
tth = cleaned[:,7]
angle = cleaned[:,8]
intensity = cleaned[:,9]
if ((start!=0) or (stop!=0)):
temperature = crop_data(temperature,line_count, start, stop, 0, 0)
chi = crop_data(chi,line_count, start, stop, 0, 0)
phi = crop_data(phi,line_count, start, stop, 0, 0)
tx = crop_data(tx,line_count, start, stop, 0, 0)
ty = crop_data(ty,line_count, start, stop, 0, 0)
om = crop_data(om,line_count, start, stop, 0, 0)
tth = crop_data(tth,line_count, start, stop, 0, 0)
angle = crop_data(angle,line_count, start, stop, 0, 0)
intensity = crop_data(intensity,line_count, start, stop, 0, 0)
line_count = line_count - start - stop
temperature = temperature[::int(line_count)]
chi = chi[::int(line_count)]
phi = phi[::int(line_count)]
tx = tx[::int(line_count)]
ty = ty[::int(line_count)]
om = om[::int(line_count)]
tth = tth[::int(line_count)]
angle = angle[:int(line_count):]
int_matrix = intensity.reshape(int(len(intensity)/line_count), int(line_count))
for i in range(shape(int_matrix)[0]):
out_scan = column_stack((angle, int_matrix[i,:]))
name = file_name + "_Scan"+str(i)
if state_temp == 1:
name += " T= " + str(round(temperature[i],2))
if state_chi == 1:
name += " CHI= " + str(round(chi[i],2))
if state_phi == 1:
name += " PHI= " + str(round(phi[i],2))
if state_x == 1:
name += " X= " + str(round(tx[i],2))
if state_y == 1:
name += " Y= " + str(round(ty[i],2))
if state_th == 1:
name += " TH= " + str(round(om[i],3))
if state_tth == 1:
name += " TTH= " + str(round(tth[i],3))
savetxt(name+".txt", out_scan, fmt = '%10.8f')
return 1
def SRIparams2iono(filename):
fullfile = h5file(filename)
fullfiledict = fullfile.readWholeh5file()
#Size = Nrecords x Nbeams x Nranges x Nions+1 x 4 (fraction, temperature, collision frequency, LOS speed)
fits = fullfiledict['/FittedParams']['Fits']
(nt,nbeams,nrng,nspecs,nstuff) = fits.shape
nlocs = nbeams*nrng
fits = fits.transpose((1,2,0,3,4))
fits = fits.reshape((nlocs,nt,nspecs,nstuff))
# Nrecords x Nbeams x Nranges
Ne = fullfiledict['/FittedParams']['Ne']
Ne = Ne.transpose((1,2,0))
Ne = Ne.reshape((nlocs,nt))
param_lists =sp.zeros((nlocs,nt,nspecs,2))
param_lists[:,:,:,0] = fits[:,:,:,0]
param_lists[:,:,:,1] = fits[:,:,:,1]
param_lists[:,:,-1,0]=Ne
Velocity = fits[:,:,0,3]
if fullfiledict['/FittedParams']['IonMass']==16:
species = ['O+','e-']
pnames = sp.array([['Ni','Ti'],['Ne','Te']])
time= fullfiledict['/Time']['UnixTime']
time = time
rng = fullfiledict['/FittedParams']['Range']
bco = fullfiledict['/']['BeamCodes']
angles = bco[:,1:3]
(nang,nrg) = rng.shape
allang = sp.tile(angles[:,sp.newaxis],(1,nrg,1))
all_loc = sp.column_stack((rng.flatten(),allang.reshape(nang*nrg,2)))
lkeep = ~ sp.any(sp.isnan(all_loc),1)
all_loc = all_loc[lkeep]
Velocity = Velocity[lkeep]
param_lists = param_lists[lkeep]
all_loc[:,0]=all_loc[:,0]*1e-3
iono1 = IonoContainer(all_loc,param_lists,times=time,ver = 1,coordvecs = ['r','theta','phi'],
paramnames = pnames,species=species,velocity=Velocity)
# MSIS
tn = fullfiledict['/MSIS']['Tn']
tn = tn.transpose((1,2,0))
tn = tn.reshape((nlocs,nt))
startparams = sp.ones((nlocs,nt,2,2))
startparams[:,:,0,1] = tn
startparams[:,:,1,1] = tn
startparams = startparams[lkeep]
ionoS = IonoContainer(all_loc,startparams,times=time,ver = 1,coordvecs = ['r','theta','phi'],
paramnames = pnames,species=species)
return iono1,ionoS
def count_feature(X, tbl_lst = None, min_cnt = 1):
X_lst = [pd.Series(X[:, i]) for i in range(X.shape[1])]
if tbl_lst is None:
tbl_lst = [x.value_counts() for x in X_lst]
if min_cnt > 1:
tbl_lst = [s[s >= min_cnt] for s in tbl_lst]
X = sp.column_stack([x.map(tbl).values for x, tbl in zip(X_lst, tbl_lst)])
# NA(unseen values) to 0
return np.nan_to_num(X), tbl_lst
def planeFromPoints(points):
""" Produces a plane from N points using least squares, and returns of the form:
Z = aX + bY + c
Follows logic from http://www.velocityreviews.com/forums/t368189-re-linear-regression-in-3-dimensions.html
"""
x, y, z = zip(*points)
A = column_stack([x, y, ones_like(x)])
abc, residuals, rank, s = lstsq(A,z)
return abc
def count_feature(X, tbl_lst=None, min_cnt=1):
X_lst = [pd.Series(X[:, i]) for i in range(X.shape[1])]
if tbl_lst is None:
tbl_lst = [x.value_counts() for x in X_lst]
if min_cnt > 1:
tbl_lst = [s[s >= min_cnt] for s in tbl_lst]
X = sp.column_stack([x.map(tbl).values for x, tbl in zip(X_lst, tbl_lst)])
# NA(unseen values) to 0
return np.nan_to_num(X), tbl_lst
def centre_of_mass(geometry, vertices='throat.offset_vertices', **kwargs):
r"""
Calculate the centre of mass of the throat from the voronoi vertices.
"""
Nt = geometry.num_throats()
outer_verts = geometry['throat.vertices']
offset_verts = geometry[vertices]
normal = geometry['throat.normal']
z_axis = [0, 0, 1]
value = _sp.ndarray([Nt, 3])
for i in range(Nt):
if len(offset_verts[i]) > 2:
verts = offset_verts[i]
elif len(outer_verts[i]) > 2:
verts = outer_verts[i]
else:
verts = []
if len(verts) > 0:
# For boundaries some facets will already be aligned with the axis -
# if this is the case a rotation is unnecessary and could also cause
# problems
angle = tr.angle_between_vectors(normal[i], z_axis)
if angle == 0.0 or angle == _sp.pi:
"We are already aligned"
rotate_input = False
facet = verts
else:
rotate_input = True
M = tr.rotation_matrix(
tr.angle_between_vectors(normal[i], z_axis),
tr.vector_product(normal[i], z_axis))
facet = _sp.dot(verts, M[:3, :3].T)
# Now we have a rotated facet aligned with the z axis - make 2D
facet_2D = _sp.column_stack((facet[:, 0], facet[:, 1]))
z = _sp.unique(_sp.around(facet[:, 2], 10))
if len(z) == 1:
# We need the vertices arranged in order so perform a convex hull
hull = ConvexHull(facet_2D)
ordered_facet_2D = facet_2D[hull.vertices]
# Call the routine to calculate an area wighted centroid from the
# 2D polygon
COM_2D = vo.PolyWeightedCentroid2D(ordered_facet_2D)
COM_3D = _sp.hstack((COM_2D, z))
# If we performed a rotation we need to rotate back
if (rotate_input):
MI = tr.inverse_matrix(M)
# Unrotate the offset coordinates using the inverse of the
# original rotation matrix
value[i] = _sp.dot(COM_3D, MI[:3, :3].T)
else:
value[i] = COM_3D
else:
logger.error('Rotation Failed: ' +
str(_sp.unique(facet[:, 2])))
return value
def compare_arrays(a, b, inc_time=False):
diffAbs = (sp.absolute(sp.subtract(a, b)))
diffMax = sp.nanmax(diffAbs)
diffEps = (diffMax / sys.float_info.epsilon
) * 2 # we have to mult by two as python epsilon is not correct
if inc_time:
return sp.column_stack((a[:, 0], diffAbs)), diffMax, diffEps
else:
return diffAbs, diffMax, diffEps
def nstats(self, upto):
"""Given an n-values array returns the average and standard deviation
of the n-values taken at each stage-height for each cross-section.
'nvals' - array of n-values with shape (x,y) with cross-sections
along the x axis and stage-heights along the y axis"""
self.get_xs_n(upto)
means = scipy.mean(self.xs_nvals, axis=1)
stdevs = scipy.std(self.xs_nvals, axis=1)
# if filename = True: # Write to csv
return scipy.column_stack((self.handstage[:upto], means, stdevs))
def __init__(self,ionoin,configfile):
r2d = 180.0/sp.pi
d2r = sp.pi/180.0
(sensdict,simparams) = readconfigfile(configfile)
nt = ionoin.Time_Vector.shape[0]
nloc = ionoin.Sphere_Coords.shape[0]
#Input location
self.Cart_Coords_in = ionoin.Cart_Coords
self.Sphere_Coords_In = ionoin.Sphere_Coords,
self.Time_In = ionoin.Time_Vector
self.Cart_Coords_In_Rep = sp.tile(ionoin.Cart_Coords,(nt,1))
self.Sphere_Coords_In_Rep = sp.tile(ionoin.Sphere_Coords,(nt,1))
self.Time_In_Rep = sp.repeat(ionoin.Time_Vector,nloc,axis=0)
#output locations
rng_vec2 = simparams['Rangegatesfinal']
nrgout = len(rng_vec2)
angles = simparams['angles']
nang =len(angles)
ang_data = sp.array([[iout[0],iout[1]] for iout in angles])
rng_all = sp.tile(rng_vec2,(nang))
ang_all = sp.repeat(ang_data,nrgout,axis=0)
nlocout = nang*nrgout
ntout = len(simparams['Timevec'])
self.Sphere_Coords_Out = sp.column_stack((rng_all,ang_all))
(R_vec,Az_vec,El_vec) = (self.Sphere_Coords_Out[:,0],self.Sphere_Coords_Out[:,1],self.Sphere_Coords_Out[:,2])
xvecmult = sp.cos(Az_vec*d2r)*sp.cos(El_vec*d2r)
yvecmult = sp.sin(Az_vec*d2r)*sp.cos(El_vec*d2r)
zvecmult = sp.sin(El_vec*d2r)
X_vec = R_vec*xvecmult
Y_vec = R_vec*yvecmult
Z_vec = R_vec*zvecmult
self.Cart_Coords_Out = sp.column_stack((X_vec,Y_vec,Z_vec))
self.Time_Out = simparams['Timevec']
self.Time_Out_Rep =sp.repeat(simparams['Timevec'],nlocout,axis=0)
self.Sphere_Coords_Out_Rep =sp.tile(self.Sphere_Coords_Out,(ntout,1))
self.RSTMat = makematPA(ionoin.Sphere_Coords,ionoin.Time_Vector)
def pyglowinput(latlonalt=[65.1367, -147.4472, 250.00], dn_list=[datetime(2015, 3, 21, 8, 00), datetime(2015, 3, 21, 20, 00)], z=None):
if z is None:
z = sp.linspace(50., 1000., 200)
dn_diff = sp.diff(dn_list)
dn_diff_sec = dn_diff[-1].seconds
timelist = sp.array([calendar.timegm(i.timetuple()) for i in dn_list])
time_arr = sp.column_stack((timelist, sp.roll(timelist, -1)))
time_arr[-1, -1] = time_arr[-1, 0]+dn_diff_sec
v=[]
coords = sp.column_stack((sp.zeros((len(z), 2), dtype=z.dtype), z))
all_spec = ['O+', 'NO+', 'O2+', 'H+', 'HE+']
Param_List = sp.zeros((len(z), len(dn_list),len(all_spec),2))
for idn, dn in enumerate(dn_list):
for iz, zcur in enumerate(z):
latlonalt[2] = zcur
pt = Point(dn, *latlonalt)
pt.run_igrf()
pt.run_msis()
pt.run_iri()
# so the zonal pt.u and meriodinal winds pt.v will coorispond to x and y even though they are
# supposed to be east west and north south. Pyglow does not seem to have
# vertical winds.
v.append([pt.u, pt.v, 0])
for is1, ispec in enumerate(all_spec):
Param_List[iz, idn, is1, 0] = pt.ni[ispec]*1e6
Param_List[iz, idn, :, 1] = pt.Ti
Param_List[iz, idn, -1, 0] = pt.ne*1e6
Param_List[iz, idn, -1, 1] = pt.Te
Param_sum = Param_List[:, :, :, 0].sum(0).sum(0)
spec_keep = Param_sum > 0.
species = sp.array(all_spec)[spec_keep[:-1]].tolist()
species.append('e-')
Param_List[:, :] = Param_List[:, :, spec_keep]
Iono_out = IonoContainer(coords, Param_List, times = time_arr, species=species)
return Iono_out
def centre_of_mass(geometry, vertices='throat.offset_vertices', **kwargs):
r"""
Calculate the centre of mass of the throat from the voronoi vertices.
"""
Nt = geometry.num_throats()
outer_verts = geometry['throat.vertices']
offset_verts = geometry[vertices]
normal = geometry['throat.normal']
z_axis = [0, 0, 1]
value = _sp.ndarray([Nt, 3])
for i in range(Nt):
if len(offset_verts[i]) > 2:
verts = offset_verts[i]
elif len(outer_verts[i]) > 2:
verts = outer_verts[i]
else:
verts = []
if len(verts) > 0:
# For boundaries some facets will already be aligned with the axis -
# if this is the case a rotation is unnecessary and could also cause
# problems
angle = tr.angle_between_vectors(normal[i], z_axis)
if angle == 0.0 or angle == _sp.pi:
"We are already aligned"
rotate_input = False
facet = verts
else:
rotate_input = True
M = tr.rotation_matrix(tr.angle_between_vectors(normal[i], z_axis),
tr.vector_product(normal[i], z_axis))
facet = _sp.dot(verts, M[:3, :3].T)
# Now we have a rotated facet aligned with the z axis - make 2D
facet_2D = _sp.column_stack((facet[:, 0], facet[:, 1]))
z = _sp.unique(_sp.around(facet[:, 2], 10))
if len(z) == 1:
# We need the vertices arranged in order so perform a convex hull
hull = ConvexHull(facet_2D)
ordered_facet_2D = facet_2D[hull.vertices]
# Call the routine to calculate an area wighted centroid from the
# 2D polygon
COM_2D = vo.PolyWeightedCentroid2D(ordered_facet_2D)
COM_3D = _sp.hstack((COM_2D, z))
# If we performed a rotation we need to rotate back
if (rotate_input):
MI = tr.inverse_matrix(M)
# Unrotate the offset coordinates using the inverse of the
# original rotation matrix
value[i] = _sp.dot(COM_3D, MI[:3, :3].T)
else:
value[i] = COM_3D
else:
print('Rotation Failed: ' + str(_sp.unique(facet[:, 2])))
return value
def run_clock(beta_file):
"""
Function to run clock given the path to a CSV
file containing the normalised beta values
"""
probes = np.load("model/probes.npy")
newx, samples = read_file(beta_file, probes)
nbeta = np.load("model/nbeta.npy")
result = scipy.dot(scipy.column_stack((scipy.ones([newx.shape[0], 1]), newx)), nbeta)[:, 0]
return scipy.row_stack((samples, result.flatten()))
def makedata(testpath,tint):
""" This will make the input data for the test case. The data will have cases
where there will be enhancements in Ne, Ti and Te in one location. Each
case will have 3 integration periods. The first 3 integration periods will
be the default set of parameters Ne=Ne=1e11 and Te=Ti=2000.
Inputs
testpath - Directory that will hold the data.
tint - The integration time in seconds.
"""
testpath = Path(testpath).expanduser()
finalpath = testpath.joinpath('Origparams')
if not finalpath.is_dir():
finalpath.mkdir()
data = sp.array([[1e11,1100.], [1e11,2100.]])
z = (50.+sp.arange(50)*10.)
nz = len(z)
params = sp.tile(data[sp.newaxis, sp.newaxis],(nz, 1, 1, 1))
epnt = range(20,22)
p2 = sp.tile(params, (1, 4, 1, 1))
#enhancement in Ne
p2[epnt, 1, :, 0] = 5e11
#enhancement in Ti
p2[epnt,2,0,1] = 2200.
#enhancement in Te
p2[epnt,3,1,1] = 4200.
coords = sp.column_stack((sp.zeros(nz), sp.zeros(nz), z))
species=['O+', 'e-']
times = sp.array([[0, 1e3]])
times2 = sp.column_stack((sp.arange(0, 4), sp.arange(1, 5)))*3*tint
vel = sp.zeros((nz, 1, 3))
vel2 = sp.zeros((nz, 4, 3))
Icontstart = IonoContainer(coordlist=coords, paramlist=params, times=times,
sensor_loc=sp.zeros(3), ver=0, coordvecs=['x', 'y', 'z'],
paramnames=None, species=species, velocity=vel)
Icont1 = IonoContainer(coordlist=coords, paramlist=p2, times=times2,
sensor_loc=sp.zeros(3), ver=0, coordvecs=['x', 'y', 'z'],
paramnames=None, species=species, velocity=vel2)
finalfile = finalpath.joinpath('0 stats.h5')
Icont1.saveh5(str(finalfile))
Icontstart.saveh5(str(testpath.joinpath('startfile.h5')))
def makedata(testpath,tint):
""" This will make the input data for the test case. The data will have cases
where there will be enhancements in Ne, Ti and Te in one location. Each
case will have 3 integration periods. The first 3 integration periods will
be the default set of parameters Ne=Ne=1e11 and Te=Ti=2000.
Inputs
testpath - Directory that will hold the data.
tint - The integration time in seconds.
"""
finalpath = os.path.join(testpath,'Origparams')
if not os.path.isdir(finalpath):
os.mkdir(finalpath)
z = sp.linspace(50.,750,150)
nz = len(z)
Z_0 = 250.
H_0=30.
N_0=6.5e11
c1 = Chapmanfunc(z,H_0,Z_0,N_0)+5e10
z0=50.
T0=600.
Te,Ti = TempProfile(z,T0,z0)
params = sp.zeros((nz,1,2,2))
params[:,0,0,0] = c1
params[:,0,1,0] = c1
params[:,0,0,1] = Ti
params[:,0,1,1] = Te
coords = sp.column_stack((sp.zeros(nz),sp.zeros(nz),z))
species=['O+','e-']
times = sp.array([[0,1e3]])
times2 = sp.column_stack((sp.arange(0,1),sp.arange(1,2)))*3*tint
vel = sp.zeros((nz,1,3))
vel2 = sp.zeros((nz,4,3))
Icontstart = IonoContainer(coordlist=coords,paramlist=params,times = times,sensor_loc = sp.zeros(3),ver =0,coordvecs =
['x','y','z'],paramnames=None,species=species,velocity=vel)
Icont1 = IonoContainer(coordlist=coords,paramlist=params,times = times,sensor_loc = sp.zeros(3),ver =0,coordvecs =
['x','y','z'],paramnames=None,species=species,velocity=vel2)
finalfile = os.path.join(finalpath,'0 stats.h5')
Icont1.saveh5(finalfile)
Icontstart.saveh5(os.path.join(testpath,'startfile.h5'))
def getFeatures(df):
B = sp.array(df["cB"].tolist())
R = sp.array(df["cR"].tolist())
I = sp.array(df["cI"].tolist())
V = sp.array(df["cV"].tolist())
Ha = sp.array(df["lHa"].tolist())
Hb = sp.array(df["lHb"].tolist())
Hg = sp.array(df["lHg"].tolist())
totCounts = sp.array(df["cTotal"].tolist())
randomFeature = sp.random.normal(0.5, 0.2, len(totCounts))
return sp.column_stack((B - V, B - R, B - I, V - R, V - I, R - I,
totCounts, Ha, Hb, Hg, randomFeature))
def generate( k, n, scale = 10, prior = "uniform" ):
"""Generate k topics, each with n words"""
if prior == "uniform":
# Each topic is a multinomial generated from a Dirichlet
topics = sc.column_stack( [ dirichlet( sc.ones( n ) * scale
) for i in xrange( k ) ] )
# We also draw the weights of each topic
weights = dirichlet( sc.ones(k) * scale )
return TopicModel( weights, topics )
else:
# TODO: Support the anchor word assumption.
raise NotImplementedError
def getFeatures(df):
BV = sp.array(df["BV"].tolist())
BR = sp.array(df["BR"].tolist())
BI = sp.array(df["BI"].tolist())
VR = sp.array(df["VR"].tolist())
VI = sp.array(df["VI"].tolist())
RI = sp.array(df["RI"].tolist())
Ha = sp.array(df["Ha"].tolist())
Hb = sp.array(df["Hb"].tolist())
Hg = sp.array(df["Hg"].tolist())
totCounts = sp.array(df["totalCounts"].tolist())
#spike = sp.array(df["spike"].tolist())
randomFeature = sp.random.normal(0.5, 0.2, len(totCounts))
return sp.column_stack((BV, BR, BI, VR, VI, RI, totCounts, Ha, Hb, Hg,
randomFeature)) #,spike,randomFeature))
def main(self):
bins = 50
halfwidth=0.5
histories = 10000
iterations = 50
restarts = 5
geo = Geometry.Geometry(bins, [[-halfwidth,halfwidth]])
xs = CrossSection.CrossSection(xS=0.5,nu=1.0,xF=0.5,xG=0)
self.mark = Markov.Markov(geo, xs, histories)
self.mark.score = self.score
self.Q = scipy.zeros((bins,0))
for i in xrange(bins):
print "I am at %i" %i
point = scipy.zeros((bins))
point[i] = 1
pSource = fissionSource.histogramSource(point,geo)
self.response = fissionBank.fissionBank()
self.mark.transport(pSource)
q = fissionSource.histogramSource(self.response,geo)
q = q*(1.0/self.mark.histories)
self.printVector(q)
self.Q = scipy.column_stack((self.Q,q))
q = scipy.ones(bins)
q = q/scipy.linalg.norm(q,2)
print "Calling Deterministic Arnoldi"
adtm = ArnoldiDtm.Arnoldi(self.Q, iterations, restarts)
eValues, eVectors = adtm.Arnoldi(q)
print "Eigenvalues: "
self.printVector(eValues)
print "Dominant eigenvector: "
self.printVector(eVectors[:,-1])
print "\nAll eigenvectors: "
self.printM(eVectors)
Chart = Gnuplot.Gnuplot()
Chart.title("Histories per 'vector': %i, bins = %i" %(histories, bins))
length = len(eValues)-1
for i in xrange(5):
data = Gnuplot.Data(eVectors[:,length-i],with='lines',
title='vector %i' %i)
Chart.replot(data)
def make2dhist(testpath, xaxis=TE, yaxis=TI, figmplf=None, curax=None):
"""
This will plot a 2-D histogram of two variables.
Args:
testpath (obj:`str`): The path where the SimISR data is stored.
npulses (obj:`int`): The number of pulses.
xaxis (obj: `dict`): default TE, Dictionary that holds the parameter info along the x axis of the distribution.
yaxis (obj: `dict`): default TE, Dictionary that holds the parameter info along the y axis of the distribution.
figmplf (obj: `matplotb figure`): default None, Figure that the plot will be placed on.
curax (obj: `matplotlib axis`): default None, Axis that the plot will be made on.
Returns:
figmplf (obj: `matplotb figure`), curax (obj: `matplotlib axis`):,hist_h (obj: `matplotlib axis`)):
The figure handle the plot is made on, the axis handle the plot is on, the plot handle itself.
"""
sns.set_style("whitegrid")
sns.set_context("notebook")
params = [xaxis['param'], yaxis['param']]
datadict, _, _, _ = makehistdata(params, testpath)
if (figmplf is None) and (curax is None):
(figmplf, curax) = plt.subplots(1, 1, figsize=(6, 6), facecolor='w')
b1 = sp.linspace(*xaxis['lims'])
b2 = sp.linspace(*yaxis['lims'])
bins = [b1, b2]
d1 = sp.column_stack((datadict[params[0]], datadict[params[1]]))
H, xe, ye = sp.histogram2d(d1[:, 0].real,
d1[:, 1].real,
bins=bins,
normed=True)
hist_h = curax.pcolor(xe[:-1],
ye[:-1],
sp.transpose(H),
cmap='viridis',
vmin=0)
curax.set_xlabel(r'$' + xaxis['paramLT'] + '$')
curax.set_ylabel(r'$' + yaxis['paramLT'] + '$')
curax.set_title(r'Joint distributions for $' + xaxis['paramLT'] + '$' +
' and $' + yaxis['paramLT'] + '$')
plt.colorbar(hist_h, ax=curax, label='Probability', format='%1.1e')
return (figmplf, curax, hist_h)
def _calc_eVectors(self, Q, V):
"""
calc_eVectors will calculate the eigenvectors. The
eigevector is a linear combination of the vectors of Q with the elements
of an eigenvector of H as the expansion coefficients. calc_eVecctors
returns a matrix who's columns are the eigenvectors.
Q: List of orthornormal basis vectors
V: Matrix of column vectors
"""
n = len(V)
m = len(Q[0])
Vectors = scipy.zeros((m, 0))
for j in xrange(n):
Vector = scipy.zeros(m)
for i in xrange(n):
Vector = Vector + V[i, j] * Q[i]
Vectors = scipy.column_stack((Vectors, Vector))
return Vectors
def _calc_eVectors(self, Q, V):
"""
calc_eVectors will calculate the eigenvectors. The
eigevector is a linear combination of the vectors of Q with the elements
of an eigenvector of H as the expansion coefficients. calc_eVecctors
returns a matrix who's columns are the eigenvectors.
Q: List of orthornormal basis vectors
V: Matrix of column vectors
"""
n = len(V)
m = len(Q[0])
Vectors = scipy.zeros((m,0))
for j in xrange(n):
Vector = scipy.zeros(m)
for i in xrange(n):
Vector = Vector + V[i,j]*Q[i]
Vectors = scipy.column_stack((Vectors,Vector))
return Vectors
def get_logit_endog(true_params, exog, noise_level):
"""
Gets an endogenous response that is consistent with the true_params,
perturbed by noise at noise_level.
"""
N = exog.shape[0]
### Create the probability of entering the different classes,
### given exog and true_params
Xdotparams = sp.dot(exog, true_params)
noise = noise_level * sp.randn(*Xdotparams.shape)
eXB = sp.column_stack((sp.ones(len(Xdotparams)), sp.exp(Xdotparams)))
class_probabilities = eXB / eXB.sum(1)[:, None]
### Create the endog
cdf = class_probabilities.cumsum(axis=1)
endog = sp.zeros(N)
for i in xrange(N):
endog[i] = sp.searchsorted(cdf[i, :], sp.rand())
return endog