def direct2cartesian(self):
"""Convert atom coordinates from direct to cartesian"""
if self.cartesian:
return
self.atoms = m.transpose(m.dot(self.lattice_constant*self.basis_vectors, \
m.transpose(self.atoms)))
self.cartesian = True
def rotate_molecule(coords, rotp = m.array((0.,0.,0.)), phi = 0., \
theta = 0., psi = 0.):
"""Rotate a molecule via Euler angles.
See http://mathworld.wolfram.com/EulerAngles.html for definition.
Input arguments:
coords: Atom coordinates, as Nx3 2d pylab array.
rotp: The point to rotate about, as a 1d 3-element pylab array
phi: The 1st rotation angle around z axis.
theta: Rotation around x axis.
psi: 2nd rotation around z axis.
"""
# First move the molecule to the origin
# In contrast to MATLAB, numpy broadcasts the smaller array to the larger
# row-wise, so there is no need to play with the Kronecker product.
rcoords = coords - rotp
# First Euler rotation about z in matrix form
D = m.array(((m.cos(phi), m.sin(phi), 0.), (-m.sin(phi), m.cos(phi), 0.), \
(0., 0., 1.)))
# Second Euler rotation about x:
C = m.array(((1., 0., 0.), (0., m.cos(theta), m.sin(theta)), \
(0., -m.sin(theta), m.cos(theta))))
# Third Euler rotation, 2nd rotation about z:
B = m.array(((m.cos(psi), m.sin(psi), 0.), (-m.sin(psi), m.cos(psi), 0.), \
(0., 0., 1.)))
# Total Euler rotation
A = m.dot(B, m.dot(C, D))
# Do the rotation
rcoords = m.dot(A, m.transpose(rcoords))
# Move back to the rotation point
return m.transpose(rcoords) + rotp
def plotEnsemble2D(ens,v1,v2,colordata=None,hess=None,\
size=50,labelBest=True,ensembleAlpha=0.75,contourAlpha=1.0):
"""
Plots a 2-dimensional projection of a given parameter
ensemble, along given directions:
-- If v1 and v2 are scalars, project onto plane given by
those two bare parameter directions.
-- If v1 and v2 are vectors, project onto those two vectors.
When given colordata (either a single color, or an array
of different colors the length of ensemble size), each point
will be assigned a color based on the colordata.
With labelBest set, the first point in the ensemble is
plotted larger (to show the 'best fit' point for a usual
parameter ensemble).
If a Hessian is given, cost contours will be plotted
using plotContours2D.
"""
if pylab.shape(v1) is ():
xdata = pylab.transpose(ens)[v1]
ydata = pylab.transpose(ens)[v2]
# label axes
param1name, param2name = '',''
try:
paramLabels = ens[0].keys()
except:
paramLabels = None
if paramLabels is not None:
param1name = ' ('+paramLabels[param1]+')'
param2name = ' ('+paramLabels[param2]+')'
pylab.xlabel('Parameter '+str(v1)+param1name)
pylab.ylabel('Parameter '+str(v2)+param2name)
else:
xdata = pylab.dot(ens,v1)
ydata = pylab.dot(ens,v2)
if colordata==None:
colordata = pylab.ones(len(xdata))
if labelBest: # plot first as larger circle
if pylab.shape(colordata) is (): # single color
colordata0 = colordata
colordataRest = colordata
else: # specified colors
colordata0 = [colordata[0]]
colordataRest = colordata[1:]
scatterColors(xdata[1:],ydata[1:],colordataRest, \
size,alpha=ensembleAlpha)
scatterColors([xdata[0]],[ydata[0]],colordata0, \
size*4,alpha=ensembleAlpha)
else:
scatterColors(xdata,ydata,colordata,size,alpha=ensembleAlpha)
if hess is not None:
plotApproxContours2D(hess,param1,param2,pylab.array(ens[0]), \
alpha=contourAlpha)
def cartesian2direct(self):
"""Convert atom coordinates from cartesian to direct"""
if not self.cartesian:
return
self.atoms = m.transpose(m.linalg.solve(self.lattice_constant * \
self.basis_vectors, \
m.transpose(self.atoms)))
self.cartesian = False
def save_rsj_params(self):
mat = pl.vstack((pl.array(self.idx), pl.transpose(self.c),\
self.icarr, self.rnarr, self.ioarr, self.voarr,\
self.ic_err_arr, self.rn_err_arr, self.io_err_arr, self.vo_err_arr))
header_c = ''
for n in range(self.cdim):
header_c = header_c + 'Control%d '%(n+1)
header_ = 'Index ' + header_c + \
'Ic Rn Io Vo Ic_err Rn_err Io_err Vo_err'
pl.savetxt(self.get_fullpath(self.fn_rsjparams), pl.transpose(mat),\
header=header_)
def degraderesolution(prefix,factor,dlogstring):
covar = M.load(prefix+'covar.dat')
pnl = M.load(prefix+'pnl.dat')
dlog = M.load(prefix+dlogstring)[:,1]
k = pnl[:,0]*1.
p = pnl[:,1]*1.
gausspart = M.load(prefix+'gausspart.dat')
nbins = len(k)
nongausspart = covar - gausspart
nongausspartnew = nongausspart[:nbins-factor:factor,:nbins-factor:factor]*0.
knew = k[:nbins-factor:factor]*0.
pnew = p[:nbins-factor:factor]*0.
gausspartnew = gausspart[:nbins-factor:factor,:nbins-factor:factor]*0.
nbinsnew = len(knew)
dlognew = dlog[:nbins-factor:factor]*0.
for i1 in range(0,nbins-factor,factor):
i1new = i1/factor
print i1,i1+factor-1,nbins
print i1new,nbinsnew
weights = k[i1:i1+factor-1]**3
sumweights = M.sum(weights)
pnew[i1new] = M.sum(p[i1:i1+factor-1]*weights)/sumweights
knew[i1new] = M.sum(k[i1:i1+factor-1]*weights)/sumweights
dlognew[i1new] = M.sum(dlog[i1:i1+factor-1]*weights)/sumweights
sqrtkfact = M.sqrt(k[1]/k[0])
for i1 in range(0,nbins-factor,factor):
i1new = i1/factor
for i2 in range(0,nbins-factor,factor):
i2new = i2/factor
weights2 = M.outer(k[i1:i1+factor-1]**3,k[i2:i2+factor-1]**3)
sumweights2 = M.sum(M.sum(weights2))
nongausspartnew[i1new,i2new] = M.sum(M.sum(nongausspart[i1:i1+factor-1,i2:i2+factor-1]*weights2))/sumweights2
if i1new == i2new:
vk = (4.*M.pi/3.)*((k[i1+factor-1]*sqrtkfact)**3 - (k[i1]/sqrtkfact)**3)
gausspartnew[i1new,i2new] = (2.*M.pi)**3 * 2.*(pnew[i1new]**2)/vk
covarnew = gausspartnew + nongausspartnew
prefixnew = prefix+'degrade'+str(factor)+'/'
os.system('mkdir '+prefixnew)
M.save(prefixnew+'pnl.dat',M.transpose([knew,pnew]), fmt = '%18.16e')
M.save(prefixnew+'covar.dat',covarnew, fmt = '%18.16e')
M.save(prefixnew+'gausspart.dat',gausspartnew, fmt = '%18.16e')
M.save(prefixnew+dlogstring,M.transpose([knew,dlognew]), fmt = '%18.16e')
M.save(prefix+'nbins.dat',M.array([nbinsnew],shape=(1,1,)), fmt = '%d')
def Q_calc(self,X): """ calculates Q (n_x by n_theta) matrix of the IDE model at each time step Arguments ---------- X: list of ndarray state vectors Returns --------- Q : list of ndarray (n_x by n_theta) """ Q=[] T=len(X) Psi=self.model.Gamma_inv_psi_conv_Phi Psi_T=pb.transpose(self.model.Gamma_inv_psi_conv_Phi,(0,2,1)) for t in range(T): firing_rate_temp=pb.dot(X[t].T,self.model.Phi_values) firing_rate=self.model.act_fun.fmax/(1.+pb.exp(self.model.act_fun.varsigma*(self.model.act_fun.v0-firing_rate_temp))) #calculate q g=pb.dot(firing_rate,Psi_T) g *=(self.model.spacestep**2) q=self.model.Ts*g q=q.reshape(self.model.nx,self.model.n_theta) Q.append(q) return Q
def f(filename, theClass=1):
fs, data = wavfile.read(filename) # load the data
# b=[(ele/2**8.)*2-1 for ele in data] # this is 8-bit track, b is now normalized on [-1,1)
print "Sample rates is: "
print fs
X = stft(data, fs, 256.0 / fs, 256.0 / fs)
X = X[:, 0:(X.shape[1] / 2)]
shortTimeFFT = scipy.absolute(X.T)
shortTimeFFT = scipy.log10(shortTimeFFT)
# Plot the magnitude spectrogram.
pylab.figure()
pylab.imshow(shortTimeFFT,
origin='lower',
aspect='auto',
interpolation='nearest')
pylab.xlabel('Time')
pylab.ylabel('Frequency')
savefig(filename + 'SFFT.png', bbox_inches='tight')
features = mean(shortTimeFFT, axis=1)
pylab.figure()
pylab.plot(features, 'r')
savefig(filename + 'AFFT.png', bbox_inches='tight')
with open(filename + '.csv', 'w') as fp:
a = csv.writer(fp, delimiter=',')
row = pylab.transpose(features)
row = pylab.append(row, theClass)
a.writerow(row)
def loadMNISTImages(filename):
f = open(filename, 'rb')
# Verify Magic Number
s = f.read(4)
magic = int(s.encode('hex'),16)
assert(magic == 2051)
# Get Number of Images
s = f.read(4)
numImages = int(s.encode('hex'),16)
s = f.read(4)
numRows = int(s.encode('hex'),16)
s = f.read(4)
numCols = int(s.encode('hex'),16)
# Get Data
s = f.read()
a = frombuffer(s, uint8)
# Use 'F' to ensure that we read by column
a = reshape(a, (numCols , numRows, numImages), order='F');
images = transpose(a, (1, 0, 2))
f.close()
# Reshape to #pixels * #examples
images = reshape(a, (shape(images)[0] * shape(images)[1], numImages),
order='F');
images = double(images)/255
return images
def load_data(filename=None, datastr=None, skip_rows=False,use_cols=False):
"""Load a file with numeric column data into a numpy array.
Automatically skips header unless "skip_rows" is specified.
Loads all columns unless "use_cols" is specified."""
if filename is not None:
textiter = open(filename, 'r')
else:
textiter = iter(datastr.split("\n"))
#datare=re.compile('\s*(-?\d+(\.\d+)?([Ee][+-]?\d+)?(\s+|$)){2,}')
if skip_rows == False:
skip_rows=0
nx=textiter.next()
while datare.match(nx)==None:
# print "skipping row ", skip_rows
skip_rows+=1
print nx
nx=textiter.next()
if filename is not None:
textiter.close()
textiter = open(filename, 'r')
# else:
# textiter=iter(datastr.split("\n"))
if use_cols:
tmp_data=load(textiter,datastr,skiprows=skip_rows,usecols=use_cols)
else:
tmp_data=load(textiter,datastr,skiprows=skip_rows)
if filename is not None:
textiter.close()
return transpose(tmp_data)
def Global_Stiffness(self):
'''
Generates Global Stiffness Matrix for the plane structure
'''
elem = self.element;
B = py.zeros((6,6))
for i in range (0,py.size(elem,0)):
#for each element find the stifness matrix
K = py.zeros((self.n_nodes*2,self.n_nodes*2))
el = elem[i]
#nodes formatted for input
[node1, node2, node3] = el;
node1x = 2*(node1-1);node2x = 2*(node2-1);node3x = 2*(node3-1);
node1y = 2*(node1-1)+1;node2y = 2*(node2-1)+1;node3y = 2*(node3-1)+1;
#Area, Strain Matrix and E Matrix multiplied to get element stiffness
[J,B] = self.B(el)
local_k =0.5*abs(J)*py.dot(py.transpose(B),py.dot(self.E_matrix,B))
if self.debug:
print 'K for elem', el, '\n', local_k
#Element K-Matrix converted into Global K-Matrix format
K[py.ix_([node1x,node1y,node2x,node2y,node3x,node3y],[node1x,node1y,node2x,node2y,node3x,node3y])] = K[py.ix_([node1x,node1y,node2x,node2y,node3x,node3y],[node1x,node1y,node2x,node2y,node3x,node3y])]+local_k
#Adding contibution into Global Stiffness
self.k_global = self.k_global + K
if self.debug:
print 'Global Stiffness','\n', self.k_global
def read_all_csc(data_folder, dtype='int16', assume_same_fs=True, memmap=False, memmap_folder=None, save_for_spikedetekt=False, channels_to_save=None, return_sliced_data=False):
if sys.version_info[0] > 2:
mode = 'br'
else:
mode = 'r'
os_name = platform.system()
if os_name == 'Windows':
sep = '\\'
elif os_name=='Linux':
sep = r'/'
files = [os.path.join(data_folder, f) for f in os.listdir(data_folder) if f.endswith('.ncs')]
order = [int(file.split('.')[0].split('CSC')[1]) for file in files]
sort_order = sorted(range(len(order)),key=order.__getitem__)
ordered_files = [files[i] for i in sort_order]
if memmap:
if not memmap_folder:
raise NameError("A memmap_folder should be defined for memmapped data")
out_filename = data_folder.split(sep)[-1]+'.dat'
out_full_filename = os.path.join(memmap_folder, out_filename)
data = None
i = 0;
for file in ordered_files:
fin = open(file, mode=mode)
x = read_single_csc(fin, assume_same_fs=assume_same_fs, memmap=memmap)
if not assume_same_fs or memmap:
channel_data = x['packets']['samp'].ravel()
if data is None:
data = pylab.memmap(out_full_filename, dtype=dtype, mode='w+', shape=(pylab.size(files), channel_data.size))
else:
data[i,:] = channel_data
data.flush()
i = i+1
print(i)
else:
channel_data = x['trace']
if data is None:
data = pylab.zeros(shape=(pylab.size(files), channel_data.size), dtype=dtype)
else:
data[i,:] = channel_data
i = i+1
print(i)
data_to_return = data
if save_for_spikedetekt:
if channels_to_save:
data2 = data[channels_to_save,:]
if return_sliced_data:
data_to_return = data2
else:
data2 = data
data2 = pylab.transpose(data2)
data2.reshape(data2.size)
filename = os.path.join(memmap_folder, 'spikedetekt_'+out_filename)
data2.astype(dtype).tofile(filename)
return data_to_return
def datagen(N):
"""
Produces N pairs of training data and desired output;
each sample of training data contains -1 in its first position,
this corresponds to the interpretation of the threshold as first
element of the weight vector
"""
fun1 = lambda x1,x2: -2*x1**3-x2+.5*x1**2
fun2 = lambda x1,x2: x1**2*x2+2*x1*x2+1
fun3 = lambda x1,x2: .5*x1*x2**2+x2**2-2*x1**2
rarr1 = rand(1,N)
rarr2 = rand(1,N)
teacher = sign(rand(1,N)-.5)
idplus = (teacher<0)
idminus = -idplus
rarr1[idplus] = rarr1[idplus]-1
y1=fun1(rarr1,rarr2)
y2=fun2(rarr1,rarr2)
y3=fun3(rarr1,rarr2)
x=transpose(concatenate((-ones((1,N)),y1,y2)))
return x, teacher[0]
def f(filename, theClass=1):
fs, data = wavfile.read(filename) # load the data
# b=[(ele/2**8.)*2-1 for ele in data] # this is 8-bit track, b is now normalized on [-1,1)
print "Sample rates is: "
print fs
X = stft(data, fs, 256.0 / fs, 256.0 / fs)
X = X[:, 0 : (X.shape[1] / 2)]
shortTimeFFT = scipy.absolute(X.T)
shortTimeFFT = scipy.log10(shortTimeFFT)
# Plot the magnitude spectrogram.
pylab.figure()
pylab.imshow(shortTimeFFT, origin="lower", aspect="auto", interpolation="nearest")
pylab.xlabel("Time")
pylab.ylabel("Frequency")
savefig(filename + "SFFT.png", bbox_inches="tight")
features = mean(shortTimeFFT, axis=1)
pylab.figure()
pylab.plot(features, "r")
savefig(filename + "AFFT.png", bbox_inches="tight")
with open(filename + ".csv", "w") as fp:
a = csv.writer(fp, delimiter=",")
row = pylab.transpose(features)
row = pylab.append(row, theClass)
a.writerow(row)
def datafit2ah_ic_rn(self, tn):
self.read_rsj_params(step=self.step)
self.tnarr = pl.ones(self.ndata2) * tn
guess_arr = pl.transpose(
pl.array(
[self.icarr, self.rnarr, self.ioarr, self.voarr, self.tnarr]))
self.fit2ah_ic_rn_array(guess_arr, self.reportprog)
def solve(f1, f2, f3, f4, a, b, h, tol, max_steps):
"""
uxx(x,yt) + uyy(x,y) = 0 on R = {(x,y): 0 <= x <= a, 0 <= y <= b},
u(x,0) = f1(x), u(x,b) = f2(x) for 0 <= x <= a, u(0,y) = f3(y), u(a,y) = f4(y) for 0 <= y <= b,
:param f1: u(x,0)
:param f2: u(x,b)
:param f3: u(0,y)
:param f4: u(a,y)
:param a: right boundary for x
:param b: right boundary for y
:param h: step
:param tol: maximum delta
:param max_steps: max count of steps
:return: x - vector of x coordinates, y - vector of y coordinates, u - result (matrix of z coordinates)
"""
# initialize parameters in u
n = int(a / h) + 1
m = int(b / h) + 1
ave = (a * (f1(0) + f2(0)) + b * (f3(0) + f4(0))) / (2 * a + 2 * b)
u = ave * pylab.ones((n, m))
# boundary conditions
u[0, :] = [f3(i * h) for i in range(0, m)]
u[n - 1, :] = [f4(i * h) for i in range(0, m)]
u[:, 0] = [f1(i * h) for i in range(0, n)]
u[:, m - 1] = [f2(i * h) for i in range(0, n)]
u[0, 0] = (u[0, 1] + u[1, 0]) / 2
u[0, m - 1] = (u[0, m - 2] + u[1, m - 1]) / 2
u[n - 1, 0] = (u[n - 2, 0] + u[n - 1, 1]) / 2
u[n - 1, m - 1] = (u[n - 2, m - 1] + u[n - 1, m - 2]) / 2
# The parameter of consistent method of relax
w = 4 / (2 + math.sqrt(4 - (math.cos(math.pi /
(n - 1)) + math.cos(math.pi /
(m - 1)))**2))
# Improved approximation operator purification throughout the lattice
error = 1
count = 0
while error > tol and count <= max_steps:
error = 0
for j in range(1, m - 1):
for i in range(1, n - 1):
relax = w * (u[i][j + 1] + u[i][j - 1] + u[i + 1][j] +
u[i - 1, j] - 4 * u[i][j]) / 4
u[i, j] += relax
if error <= math.fabs(relax):
error = math.fabs(relax)
count += 1
x = [i * h for i in range(n)]
y = [i * h for i in range(m)]
u = pylab.flipud(pylab.transpose(u))
return x, y, u
def load_data(directory, file_):
# load the data matrix from the data file
data = loadtxt(directory + "data/" + file_ + ".txt", unpack=True)
if type(data[0]) is float64: # check if the first column is a column
data = array(transpose(matrix(data)))
return data
def save_ah_params(self, n):
n += 1
mat = pl.vstack((pl.array(self.idx)[:n], pl.transpose(self.c[:n]),\
self.icarr[:n], self.rnarr[:n], self.ioarr[:n], self.voarr[:n],\
self.tnarr[:n],\
self.ic_err_arr[:n], self.rn_err_arr[:n], self.io_err_arr[:n],\
self.vo_err_arr[:n], self.tn_err_arr[:n]))
n -= 1
header_c = ''
for m in range(self.cdim):
header_c = header_c + 'Control%d '%(m+1)
header_ = 'Index ' + header_c + \
'Ic Rn Io Vo Tn Ic_err Rn_err Io_err Vo_err Tn_err'
pl.savetxt(self.get_fullpath(self.fn_ahparams), pl.transpose(mat),\
header=header_)
def getInfoCurve():
"""
Various functions to calculate example parameter error bars as in
Neyrinck & Szapudi 2007, MNRAS 375, L51
"""
c = pt.Camb(hubble = 70., ombh2 = 0.05*(0.7)**2, omch2 = 0.25*(0.7)**2)
c.run()
c.kextend(-10,60) # necessary to make sigma(m) integral converge well.
pt.normalizePk(c,0.8) #sigma_8
outputdir = 'example/'
#Sheth-Tormen
h = halo.HaloModel(c,st_big_a = 0., st_little_a=0.707, stq = 0.3, k = 10.**M.arange(-2,1.01,0.25),massdivsperdex=5)
#For final calculations, should use more massdivsperdex, e.g. 20 (maybe 10 is ok)
#also, k is really coarse, as you'll see if you run this.
# get covariance matrix from halo-model trispectrum (saves it in the 'prefix' directory)
# it also automatically runs halo.getHaloPknl
halo.getHaloCov(outputdir,c,h)
# power spectrum at h.k (range of k at which halo model quantities are evaluated)
M.loglog(h.k,h.pnl)
M.show()
# get derivs wrt ln A, tilt
h.dloga = halo.getdlogPnldCosmoParam(c,h,'scalar_amp',linlog='log')
h.dtilt = halo.getdlogPnldCosmoParam(c,h,'scalar_spectral_index',linlog='lin')
M.loglog(h.k,h.dloga**2,label='ln A')
M.loglog(h.k,h.dtilt**2,label='tilt')
M.legend()
M.show()
M.save(outputdir+'dlogpnldloga.dat',M.transpose([h.k,h.dloga]),fmt='%6.5e')
M.save(outputdir+'dlogpnldtilt.dat',M.transpose([h.k,h.dtilt]),fmt='%6.5e')
# get parameter covariance matrix (just a function of k, since there's only one variable)
k, covmat = info.getParamCovMat(outputdir,dlogfilenames=['dlogpnldloga.dat','dlogpnldtilt.dat'])
# plot the unmarginalized error bars in ln A and the tilt,
# if the matter power spectrum is analyzed from k= k[0] to k.
M.loglog(k, M.sqrt(covmat[0,0,:]),label='ln A')
M.loglog(k, M.sqrt(covmat[1,1,:]),label='tilt')
M.legend()
M.show()
def plot_simple(in_file):
try:
data = pylab.loadtxt(sys.argv[1])
except:
raise IOError("Can't read %s." % in_file)
for i in pylab.transpose(data):
pylab.plot(i)
def read_poscar(self, filename):
"""Parses a POSCAR file"""
f = open(filename)
poscar = f.readlines()
f.close()
# First line should contain the atom names , eg. "Ag Ge" in
# the same order
# as later in the file (and POTCAR for the full vasp run)
atomNames = poscar[0].split()
self.lattice_constant = float(poscar[1])
# Now the lattice vectors
a = []
for vector in poscar[2:5]:
s = vector.split()
floatvect = float(s[0]), float(s[1]), float(s[2])
a.append( floatvect)
# Transpose to make natural ordering for linear algebra
self.basis_vectors = m.transpose(m.array(a))
# Number of atoms. Again this must be in the same order as
# in the first line
# and in the POTCAR file
numofatoms = poscar[5].split()
for i in xrange(len(numofatoms)):
numofatoms[i] = int(numofatoms[i])
if (len(atomNames) < i + 1):
atomNames.append("Unknown")
[self.atom_symbols.append(atomNames[i]) for n in xrange(numofatoms[i])]
# Check if Selective dynamics is switched on
sdyn = poscar[6]
add = 0
if sdyn[0] == "S" or sdyn[0] == "s":
add = 1
self.selective_dynamics = True
# Check if atom coordinates are cartesian or direct
acType = poscar[6+add]
if acType[0] == "C" or acType[0] == "c" or acType[0] == "K" or acType[0] == "k":
self.cartesian = 1
else:
self.cartesian = 0
offset = add+7
tot_natoms = sum(numofatoms)
self.atoms = m.zeros((tot_natoms, 3))
self.selective_flags = []
for atom in xrange(tot_natoms):
ac = poscar[atom+offset].split()
self.atoms[atom] = (float(ac[0]), float(ac[1]), float(ac[2]))
if self.selective_dynamics:
self.selective_flags.append((ac[3], ac[4], ac[5]))
if self.cartesian:
self.atoms *= self.lattice_constant
def plot_slice( self, value, logplot=True, colorbar=False, box=[0,0], nx=200, ny=200, center=False, axes=[0,1], minimum=1e-8, newfig=True ):
if type( center ) == list:
center = pylab.array( center )
elif type( center ) != np.ndarray:
center = self.center
dim0 = axes[0]
dim1 = axes[1]
if (box[0] == 0 and box[1] == 0):
box[0] = max( abs( self.data[ "pos" ][:,dim0] ) ) * 2
box[1] = max( abs( self.data[ "pos" ][:,dim1] ) ) * 2
slice = self.get_slice( value, box, nx, ny, center, axes )
x = (pylab.array( range( nx+1 ) ) - nx/2.) / nx * box[0]
y = (pylab.array( range( ny+1 ) ) - ny/2.) / ny * box[1]
if (newfig):
fig = pylab.figure( figsize = ( 13, int(12*box[1]/box[0] + 0.5) ) )
pylab.spectral()
if logplot:
pc = pylab.pcolor( x, y, pylab.transpose( pylab.log10( pylab.maximum( slice, minimum ) ) ), shading='flat' )
else:
pc = pylab.pcolor( x, y, pylab.transpose( slice ), shading='flat' )
if colorbar:
cb = pylab.colorbar()
pylab.axis( "image" )
xticklabels = []
for tick in pc.axes.get_xticks():
if (tick == 0):
xticklabels += [ r'$0.0$' ]
else:
xticklabels += [ r'$%.2f \cdot 10^{%d}$' % (tick/10**(ceil(log10(abs(tick)))), ceil(log10(abs(tick)))) ]
pc.axes.set_xticklabels( xticklabels, size=16, y=-0.1, va='baseline' )
yticklabels = []
for tick in pc.axes.get_yticks():
if (tick == 0):
yticklabels += [ r'$0.0$' ]
else:
yticklabels += [ r'$%.2f \cdot 10^{%d}$' % (tick/10**(ceil(log10(abs(tick)))), ceil(log10(abs(tick)))) ]
pc.axes.set_yticklabels( yticklabels, size=16, ha='right' )
return pc
def plot_simple(in_file):
try:
data = pylab.loadtxt(sys.argv[1])
except:
print "Error %s is not a readable file.\n" % (sys.argv[1])
return
for i in pylab.transpose(data):
pylab.plot(i)
def peakLocations(date, hd):
mode = "fiber"
flatname = "/tous/mir7/flats/chi"+date+"."+mode+"flat.fits"
flat = pyfits.getdata(flatname)
peakarr = np.zeros(flat.shape[1])
for zaidx in range(flat.shape[1]):
maxspot = pylab.transpose(pylab.where(flat[2,zaidx,:] == max(flat[2,zaidx,:])))
peakarr[zaidx] = maxspot[0]
return peakarr
def solve(f1, f2, f3, f4, a, b, h, tol, max_steps):
"""
uxx(x,yt) + uyy(x,y) = 0 on R = {(x,y): 0 <= x <= a, 0 <= y <= b},
u(x,0) = f1(x), u(x,b) = f2(x) for 0 <= x <= a, u(0,y) = f3(y), u(a,y) = f4(y) for 0 <= y <= b,
:param f1: u(x,0)
:param f2: u(x,b)
:param f3: u(0,y)
:param f4: u(a,y)
:param a: right boundary for x
:param b: right boundary for y
:param h: step
:param tol: maximum delta
:param max_steps: max count of steps
:return: x - vector of x coordinates, y - vector of y coordinates, u - result (matrix of z coordinates)
"""
# initialize parameters in u
n = int(a / h) + 1
m = int(b / h) + 1
ave = (a * (f1(0) + f2(0)) + b * (f3(0) + f4(0))) / (2 * a + 2 * b)
u = ave * pylab.ones((n, m))
# boundary conditions
u[0, :] = [f3(i * h) for i in range(0, m)]
u[n - 1, :] = [f4(i * h) for i in range(0, m)]
u[:, 0] = [f1(i * h) for i in range(0, n)]
u[:, m - 1] = [f2(i * h) for i in range(0, n)]
u[0, 0] = (u[0, 1] + u[1, 0]) / 2
u[0, m - 1] = (u[0, m - 2] + u[1, m - 1]) / 2
u[n - 1, 0] = (u[n - 2, 0] + u[n - 1, 1]) / 2
u[n - 1, m - 1] = (u[n - 2, m - 1] + u[n - 1, m - 2]) / 2
# The parameter of consistent method of relax
w = 4 / (2 + math.sqrt(4 - (math.cos(math.pi / (n - 1)) + math.cos(math.pi / (m - 1))) ** 2))
# Improved approximation operator purification throughout the lattice
error = 1
count = 0
while error > tol and count <= max_steps:
error = 0
for j in range(1, m - 1):
for i in range(1, n - 1):
relax = w * (u[i][j + 1] + u[i][j - 1] + u[i + 1][j] + u[i - 1, j] - 4 * u[i][j]) / 4
u[i, j] += relax
if error <= math.fabs(relax):
error = math.fabs(relax)
count += 1
x = [i * h for i in range(n)]
y = [i * h for i in range(m)]
u = pylab.flipud(pylab.transpose(u))
return x, y, u
def readColumns(fname,ignore=0):
"""
read columns of a file into a (newly created) array
optionally ignore the first ingnore lines
comments with # allowed
"""
data = M.transpose(readRaws(fname,ignore))
return data
def peakLocations(date, hd):
mode = "fiber"
flatname = "/tous/mir7/flats/chi" + date + "." + mode + "flat.fits"
flat = pyfits.getdata(flatname)
peakarr = np.zeros(flat.shape[1])
for zaidx in range(flat.shape[1]):
maxspot = pylab.transpose(
pylab.where(flat[2, zaidx, :] == max(flat[2, zaidx, :])))
peakarr[zaidx] = maxspot[0]
return peakarr
def calculate_mslp(p,pb,ph,phb,t,qvapor):
'''
calculate sea level pressure starting from 'raw' wrf output fields
usage:
>>> calculate_mslp(p,pb,ph,phb,t,qvapor)
where the arguments names correspond to the variable names in the
wrfout files e.g. p(lvl,lat,lon) or p(time,lvl,lat,lon)
'''
import from_wrf_to_grads as fw2g
cs = fw2g.from_wrf_to_grads.compute_seaprs
if len(p.shape) == 3:
# recover the full pressure field by adding perturbation and base
p = p + pb
p_t = p.transpose()
# same geopotential height
ph = (ph + phb) / 9.81
ph_t = ph.transpose()
qvapor_t = qvapor.transpose()
# do not add the wrf specified 300 factor as the wrapped fortran code
# does that for us
t_t = t.transpose()
nz = ph_t.shape[2]
# populate the geopotential_height at mid_levels array with
# averages between layers below and above
z = (ph_t[:,:,:nz-1] + ph_t[:,:,1:nz]) / 2.0
# finally "in one fell sweep"
# the zero is for debug purposes
return cs(z,t_t,p_t,qvapor_t,0).transpose()
elif len(p.shape) == 4:
mslp_shape = (p.shape[0], p.shape[2], p.shape[3])
mslp = n.zeros(mslp_shape)
for time_idx in range(p.shape[0]):
# recover the full pressure field by adding perturbation and base
dummy_p = p[time_idx] + pb[time_idx]
dummy_p_t = dummy_p.transpose()
# same geopotential height
dummy_ph = (ph[time_idx] + phb[time_idx]) / 9.81
dummy_ph_t = dummy_ph.transpose()
dummy_qvapor_t = qvapor[time_idx].transpose()
# do not add the wrf specified 300 factor as the wrapped fortran code
# does that for us
dummy_t_t = t[time_idx].transpose()
nz = dummy_ph_t.shape[2]
# populate the geopotential_height at mid_levels array with
# averages between layers below and above
z = (dummy_ph_t[:,:,:nz-1] + dummy_ph_t[:,:,1:nz]) / 2.0
# finally "in one fell sweep"
# the zero is for debug purposes
mslp[time_idx] = cs(z,dummy_t_t,dummy_p_t,dummy_qvapor_t,0).transpose()
return mslp
else:
print 'Wrong shape of the array'
return
def calcCorrcoef(widget, msg):
global g_frhist, g_behavhist, g_corrcoef
print("length of history %d\n" % len(g_frhist));
a = pylab.zeros((len(g_frhist),256+4))
i = 0
for v in g_frhist:
j=0
for u in v:
a[i,j] = u
j = j+1
i = i+1
g_corrcoef = pylab.corrcoef(pylab.transpose(a))
def plot_raw(self):
self.fig = pl.figure(figsize=(8,6))
self.fig.clf()
xv, yv = pl.meshgrid(pl.array(self.idx) + 1, self.iarr[0])
self.ax = self.fig.add_subplot(211)
#self.ax.hold(True)
im = self.ax.pcolormesh(xv, pl.transpose(self.iarr),\
pl.transpose(self.varr))
self.fig.colorbar(im)
self.ax.set_ylabel('I (A)')
self.ax.set_xlabel('Index')
self.ax2 = self.fig.add_subplot(212)
#self.ax2.hold(True)
self.ax2.plot(pl.array(self.idx) + 1, self.c[:,0])
self.ax2.set_ylabel('Control 1')
self.ax2.set_xlabel('Index')
self.ax2.grid(True)
pl.show()
def plot_cylav( self, value, logplot=True, box=[0,0], nx=512, ny=512, center=False, minimum=1e-8 ):
if type( center ) == list:
center = pylab.array( center )
elif type( center ) != np.ndarray:
center = self.center
if (box[0] == 0 and box[1] == 0):
box[0] = max( abs( self.data[ "pos" ][:,0] ) ) * 2
box[1] = max( abs( self.data[ "pos" ][:,1:] ) ) * 2
grid = calcGrid.calcGrid( self.pos.astype('float64'), self.data["hsml"].astype('float64'), self.data["mass"].astype('float64'), self.data["rho"].astype('float64'), self.data[value].astype('float64').astype('float64'), nx, ny, ny, box[0], box[1], box[1], 0, 0, 0 )
cylav = calcGrid.calcCylinderAverage( grid )
x = (pylab.array( range( nx+1 ) ) - nx/2.) / nx * box[0]
y = (pylab.array( range( ny+1 ) ) - ny/2.) / ny * box[1]
fig = pylab.figure( figsize = ( 13, int(12*box[1]/box[0] + 0.5) ) )
pylab.spectral()
if logplot:
pc = pylab.pcolor( x, y, pylab.transpose( pylab.log10( pylab.maximum( cylav, minimum ) ) ), shading='flat' )
else:
pc = pylab.pcolor( x, y, pylab.transpose( slice ), shading='flat' )
pylab.axis( "image" )
xticklabels = []
for tick in pc.axes.get_xticks():
if (tick == 0):
xticklabels += [ r'$0.0$' ]
else:
xticklabels += [ r'$%.2f \cdot 10^{%d}$' % (tick/10**(ceil(log10(abs(tick)))), ceil(log10(abs(tick)))) ]
pc.axes.set_xticklabels( xticklabels, size=16, y=-0.1, va='baseline' )
yticklabels = []
for tick in pc.axes.get_yticks():
if (tick == 0):
yticklabels += [ r'$0.0$' ]
else:
yticklabels += [ r'$%.2f \cdot 10^{%d}$' % (tick/10**(ceil(log10(abs(tick)))), ceil(log10(abs(tick)))) ]
pc.axes.set_yticklabels( yticklabels, size=16, ha='right' )
return pc
def main():
XC = loadtxt('iris.data', delimiter=',', dtype=float, converters={4: cnvt})
ind = arange(150) # indices into the dataset
ind = permutation(ind) # random permutation
L = ind[0:90] # learning set indices
T = ind[90:] # test set indices
# Learning Set
X = transpose(XC[L, 0:4])
nnc = NNb(X, XC[L, -1])
# Classification of Test Set
c = zeros(len(T))
for i in arange(len(T)):
print sys.argv[1]
print int(sys.argv[1])
c[i] = nnc.classify(XC[T[i], 0:4], int(sys.argv[1]))
# Confusion Matrix
CM = zeros((3, 3))
for i in range(3):
for j in range(3):
CM[i, j] = sum(logical_and(XC[T, 4] == (i + 1), c == (j + 1)))
print(CM)
# Plot Test Set
figure(1)
color = array([[1, 0, 0], [0, 1, 0], [0, 0, 1]])
for i in range(4):
for j in range(4):
subplot(4, 4, 4 * i + j + 1)
if i == j:
continue
print color[XC[T, 4].astype(int) - 1]
print[1, 1, 1] * len(T)
print color[c.astype(int) - 1]
scatter(XC[T, i],
XC[T, j],
s=100,
marker='s',
edgecolor=color[XC[T, 4].astype(int) - 1],
facecolor=[1, 1, 1] * len(T))
scatter(XC[T, i],
XC[T, j],
s=30,
marker='+',
edgecolor=color[c.astype(int) - 1])
savefig('figures/nnbtest.pdf')
def read_data(f):
try:
data = pylab.loadtxt(f)
except:
print "Error %s is not a readable file.\n" % (f)
return 0
data = pylab.transpose(data)
if len(data) < 2:
print "Data %s doesn't have at least two dimensions\n" % (f)
return 0
return data
def plotFrame(f):
gkd = gkedata.GkeData("s3-dg-euler-rt_q_%d.h5" % f)
dgd = gkedgbasis.GkeDgSerendip2DPolyOrder2Basis(gkd)
Xc, Yc, rho = dgd.project(0)
pylab.figure(1)
pylab.pcolormesh(Xc, Yc, pylab.transpose(rho))
pylab.axis('image')
pylab.gca().set_xticks([])
pylab.gca().set_yticks([])
pylab.axis('image')
pylab.clim(35000, 65000)
pylab.title('t = %g' % gkd.time)
pylab.savefig('s3-dg-euler-rt_rho_%05d.png' % f, bbox_inches='tight')
pylab.close()
def load(fname=None,datastr=None,comments='#',delimiter=None, converters=None,skiprows=0,
usecols=None, userows=-1, unpack=False):
"""
Norped from matplotlib/mlab.py and modified...
"""
if converters is None: converters = {}
if type(fname)==str:
if fname.endswith('.gz'):
import gzip
fh = gzip.open(fname)
else:
fh = file(fname)
elif hasattr(fname, 'seek'):
fh = fname
else:
#raise ValueError('fname must be a string or file handle')
fh=datastr.split("\n")
X = []
converterseq = None
for i,ln in enumerate(fh):
if i<skiprows: continue
#print ln
line = ln
#[:ln.find(comments)].strip()
#print line
if (not len(line)) or (datare.match(line) is None):
# print "nix"
continue
if converterseq is None:
# print "making converterseq..."
converterseq = [converters.get(j,float) for j,val in
enumerate(map(lambda s: s.strip(", \t"), line.split(delimiter)))]
if usecols is not None:
vals = line.split(delimiter)
row = [converterseq[j](vals[j]) for j in usecols]
else:
row = [converterseq[j](val) for j,val in enumerate(map(lambda s: s.strip(", \t"), line.split(delimiter)))]
thisLen = len(row)
#print row
X.append(row)
X = array(X, float)
r,c = X.shape
if r==1 or c==1:
X.shape = max([r,c]),
if unpack: return transpose(X)
else: return X
def plothuv(xh, yh, xu, yu, xv, yv, h, h0, u, v):
"plot the height and velocity for A- or C-grid variables"
dx = xh[-1] - xh[-2]
dy = yh[-1] - yh[-2]
py.clf()
py.ion()
x = py.append(xh - 0.5 * dx, xh[-1] + 0.5 * dx)
y = py.append(yh - 0.5 * dy, yh[-1] + 0.5 * dy)
py.colorbar(py.pcolormesh(x, y, py.transpose(h + h0)))
if (np.max(h0) > np.min(h0)):
py.contour(xh, yh, py.transpose(h0))
if (xh == xu).all():
py.quiver(xu, yu, py.transpose(u), py.transpose(v), scale=1e3)
else:
py.quiver(xu, yu, py.transpose(u), py.transpose(vatu(v)), scale=1e3)
py.quiver(xv, yv, py.transpose(uatv(u)), py.transpose(v), scale=1e3)
py.axis([np.min(x), np.max(x), np.min(y), np.max(y)])
def QuadArr(Func, a, b, args=()):
"""Integrates Func from a to b for args. One element of args may be array.
Outputs array of integrated values.
args is tuple of floats and/or ints and/or numpy arrays.
Currently only one element of args may be array.
The purpose of this function is to calculate an array of values where each element requires an integral."""
l = 1
for arg in args:
if type(arg) is not float and type(arg) is not int:
l = len(arg)
break
argarr = py.transpose(py.array([py.ones(l) * arg for arg in args]))
return py.array(
[integrate.quad(Func, a, b, args=tuple(ars))[0] for ars in argarr])
def __init__(self, x, y, cov, deg):
self.deg = deg
self.x = x
self.y = y
self.cov = cov
self.icov = pl.linalg.inv(cov)
self.M = pl.zeros([deg + 1, len(x)])
for i in range(deg + 1):
self.M[i, :] = x**(deg - i)
self.MC = pl.dot(self.M, self.icov)
self.MCM = pl.dot(self.M, pl.transpose(self.MC))
self.fit()
def __init__(self,x,y,cov,deg): self.deg = deg self.x = x self.y = y self.cov = cov self.icov = pl.linalg.inv(cov) self.M = pl.zeros([deg+1,len(x)]) for i in range(deg+1): self.M[i,:]=x**(deg-i) self.MC = pl.dot(self.M,self.icov) self.MCM = pl.dot(self.M,pl.transpose(self.MC)) self.fit()
def pcolor_matrix_pylab(A, fname='pcolor_matrix_matplotlib'):
"""
pcolor_matrix_pylab() implements a matlab-like 'pcolor' function to
display the large elements of a matrix in pseudocolor using the Python Imaging
Library.
"""
try:
import matplotlib
matplotlib.use('Agg')
import pylab
except ImportError:
if pedobj.kw['messages'] == 'verbose':
print '[ERROR]: pyp_graphics/pcolor_matrix_pylab() was unable to import the matplotlib module!'
logging.error(
'pyp_graphics/pcolor_matrix_pylab() was unable to import the matplotlib module!'
)
return 0
try:
import numpy
pylab.clf()
x = pylab.arange(A.shape[0])
X, Y = pylab.meshgrid(x, x)
xmin = min(pylab.ravel(X))
xmax = max(pylab.ravel(X))
pylab.xlim(xmin, xmax)
ymin = min(pylab.ravel(Y))
ymax = max(pylab.ravel(Y))
pylab.ylim(ymin, ymax)
pylab.axis('off')
pylab.pcolor(X, Y, pylab.transpose(A)) #, shading='flat')
pylab.clim(0.0, 1.0)
plotfile = '%s.png' % (fname)
myplotfile = open(plotfile, 'w')
pylab.savefig(myplotfile)
myplotfile.close()
return 1
except:
if pedobj.kw['messages'] == 'verbose':
print '[ERROR]: pyp_graphics/pcolor_matrix_pylab() was unable to create the plot %s.' % (
plotfile)
logging.error(
'pyp_graphics/pcolor_matrix_pylab() was unable to create the plot %s.',
(plotfile))
return 0
def simulationWithDruga(numViruses, maxPop, maxBirthProb, clearProb,
resistances, mutProb, numTrials):
"""
Runs simulations and plots graphs for problem 5.
For each of numTrials trials, instantiates a patient, runs a simulation for
150 timesteps, adds guttagonol, and runs the simulation for an additional
150 timesteps. At the end plots the average virus population size
(for both the total virus population and the guttagonol-resistant virus
population) as a function of time.
numViruses: number of ResistantVirus to create for patient (an integer)
maxPop: maximum virus population for patient (an integer)
maxBirthProb: Maximum reproduction probability (a float between 0-1)
clearProb: maximum clearance probability (a float between 0-1)
resistances: a dictionary of drugs that each ResistantVirus is resistant to
(e.g., {'guttagonol': False})
mutProb: mutation probability for each ResistantVirus particle
(a float between 0-1).
numTrials: number of simulation runs to execute (an integer)
"""
pop = pylab.zeros([300, 2])
for _ in range(numTrials):
viruses = [
ResistantVirus(maxBirthProb, clearProb, resistances, mutProb)
for _ in range(numViruses)
]
patient = TreatedPatient(viruses, maxPop)
result1 = [[patient.update(),
patient.getResistPop(['guttagonol'])] for _ in range(150)]
patient.addPrescription('guttagonol')
result2 = [[patient.update(),
patient.getResistPop(['guttagonol'])] for _ in range(150)]
pop += pylab.concatenate((result1, result2))
pop = pylab.transpose(pop) / numTrials
pylab.plot(pop[0], label="avg_pop")
pylab.plot(pop[1], label="resistant_pop")
pylab.title("ResistantVirus Simulation")
pylab.xlabel("Time Steps")
pylab.ylabel("Average Virus Population")
pylab.legend(loc="best")
pylab.show()
def pcolor_matrix_pylab(A, fname='pcolor_matrix_matplotlib'):
"""
pcolor_matrix_pylab() implements a matlab-like 'pcolor' function to
display the large elements of a matrix in pseudocolor using the Python Imaging
Library.
"""
try:
import matplotlib
matplotlib.use('Agg')
import pylab
except ImportError:
if pedobj.kw['messages'] == 'verbose':
print '[ERROR]: pyp_graphics/pcolor_matrix_pylab() was unable to import the matplotlib module!'
logging.error('pyp_graphics/pcolor_matrix_pylab() was unable to import the matplotlib module!')
return 0
try:
import numpy
pylab.clf()
x = pylab.arange(A.shape[0])
X, Y = pylab.meshgrid(x,x)
xmin = min(pylab.ravel(X))
xmax = max(pylab.ravel(X))
pylab.xlim(xmin, xmax)
ymin = min(pylab.ravel(Y))
ymax = max(pylab.ravel(Y))
pylab.ylim(ymin, ymax)
pylab.axis('off')
pylab.pcolor(X, Y, pylab.transpose(A))#, shading='flat')
pylab.clim(0.0, 1.0)
plotfile = '%s.png' % (fname)
myplotfile = open(plotfile,'w')
pylab.savefig(myplotfile)
myplotfile.close()
return 1
except:
if pedobj.kw['messages'] == 'verbose':
print '[ERROR]: pyp_graphics/pcolor_matrix_pylab() was unable to create the plot %s.' % (plotfile)
logging.error('pyp_graphics/pcolor_matrix_pylab() was unable to create the plot %s.', (plotfile))
return 0
def main(k):
XC = loadtxt('data/iris.data', delimiter=',', dtype=float,
converters={4: cnvt})
ind = arange(150) # indices into the dataset
ind = permutation(ind) # random permutation
L = ind[0:90] # learning set indices
T = ind[90:] # test set indices
# Learning Set
# The k-NNb classifier is called for given k.
X = transpose(XC[L, 0:4])
nnc = NNb(X, XC[L, -1], k)
# Classification of Test Set
c = zeros(len(T))
for i in range(len(T)):
c[i] = nnc.classify(XC[T[i], 0:4])
# Confusion Matrix
CM = zeros((3, 3))
for i in range(3):
for j in range(3):
CM[i, j] = sum(logical_and(XC[T, 4] == (i + 1), c == (j + 1)))
print(CM)
# Plot Test Set
plt.figure(1)
color = array([[1, 0, 0], [0, 1, 0], [0, 0, 1]])
for i in range(4):
for j in range(4):
plt.subplot(4, 4, 4 * i + j + 1)
if i == j:
continue
plt.scatter(XC[T, i], XC[T, j], s=100, marker='s',
edgecolor=color[XC[T, 4].astype(int) - 1],
facecolor=[1, 1, 1] * len(T))
plt.scatter(XC[T, i], XC[T, j], s=30, marker='+',
edgecolor=color[c.astype(int) - 1])
plt.savefig('lab_42.png')
def StiffnessAndStrain(self):
'''
Function to obtain stiffness matrix and strains in each element
'''
for el in range(self.n_element): #enumerate through all the elements
K = py.zeros((self.n_nodes*2,self.n_nodes*2))#Full stiffness matrix for one element
if self._debug:
print 'bar element:', el+1
startNode = self._connectivity[el,0]-1 #start and end node of the element
endNode = self._connectivity[el,1]-1
startXY = self._xy[startNode] #start and end coordinates of the element
endXY = self._xy[endNode]
L = py.norm(endXY - startXY) # Length of the element
self.L[el]= L
#new start and end coordinates of the element
newstartXY=self._xy[startNode]+self._displacement[startNode]
newendXY=self._xy[endNode]+self._displacement[endNode]
newL=py.norm(newendXY - newstartXY) # Deformed Length of the element
self.strain_global.append((newL-L)/L); # Axial Strain in element
T = py.zeros((4,2))
T = self.Transform2D(startXY,endXY) #get the Transformation matrix for the element
if self._debug:
print startNode, endNode, startXY, endXY
print 'T'
print T
L_inv = 1.0/L
k0=py.array([[L_inv, -L_inv],[-L_inv, L_inv]])#Stiffness matrix in 1D
k_element = py.dot(T,py.dot(k0,py.transpose(T)) )#Stiffness matrix in 2D
#Convert from 2x2 local K matrix to a full stiffness matrix but for single element
K[py.ix_([2*startNode,2*startNode+1,2*endNode,2*endNode+1],[2*startNode,2*startNode+1,2*endNode,2*endNode+1])] = K[py.ix_([2*startNode,2*startNode+1,2*endNode,2*endNode+1],[2*startNode,2*startNode+1,2*endNode,2*endNode+1])]+k_element
if self._debug:
print 'element stiffness', 'L_inv', L_inv
print k_element
print 'K'
print K
self.k_global = self.k_global + K # Assemble all the stiffness into one Global Stiffness
return self.k_global,self.strain_global
# get final solution
q1 = getRaw(fh.root.StructGridField, 2, 8, 4)
Xn, Yn, qn_1 = projectOnFinerGrid_f(Xc, Yc, q1)
# get intial solution
fh = tables.openFile("s17-dg-maxwell_q_0.h5")
q0 = getRaw(fh.root.StructGridField, 2, 8, 4)
Xn, Yn, qn_0 = projectOnFinerGrid_f(Xc, Yc, q0)
nx, ny = Xn.shape[0], Yn.shape[0]
# make plot
pylab.figure(1)
im = pylab.pcolormesh(Xn, Yn, pylab.transpose(qn_1))
pylab.axis('tight')
colorbar_adj(im)
pylab.savefig('s17-dg-maxwell-Ez.png')
def calcAverage(fld):
wt = pylab.array([1.0, 1.0, 1.0, 1.0])
return (fld[:, :, 0:4] * wt).sum(axis=-1)
# compute error
q0avg = calcAverage(q0)
q1avg = calcAverage(q1)
vol = dx * dy / 4.0
cells = grid._v_attrs.vsNumCells
dx = (upper[0] - lower[0]) / cells[0]
dy = (upper[1] - lower[1]) / cells[1]
Xc = pylab.linspace(lower[0] + 0.5 * dx, upper[0] - 0.5 * dx, cells[0])
Yc = pylab.linspace(lower[1] + 0.5 * dy, upper[1] - 0.5 * dy, cells[1])
# get final solution
qn_1 = fh.root.StructGridField[:, :, 2]
# get intial solution
fh = tables.openFile("s0-fv-maxwell_q_0.h5")
qn_0 = fh.root.StructGridField[:, :, 2]
nx, ny = Xc.shape[0], Yc.shape[0]
# make plot
pylab.figure(1)
im = pylab.pcolormesh(Xc, Yc, pylab.transpose(qn_1))
pylab.axis('tight')
colorbar_adj(im)
pylab.savefig('s1-fv-maxwell-Ez.png')
# compute error
err = numpy.abs(qn_1 - qn_0).sum() / (nx * ny)
print math.sqrt(dx * dy), err
pylab.show()
def yfit(self):
return pl.dot(pl.transpose(self.M), self.pars)
xup, yup = 10, 10
nx, ny = 64, 64
dx = (xup - xlo) / nx
dy = (yup - ylo) / ny
Xc = pylab.linspace(xlo + 0.5 * dx, xup - 0.5 * dx, nx)
Yc = pylab.linspace(ylo + 0.5 * dy, yup - 0.5 * dy, ny)
tEnd = 100.0
nFrame = 11
T = pylab.linspace(0, tEnd, nFrame)
for i in range(nFrame):
print "Working on ", i
fh = tables.openFile("s141-vortex-waltz_chi_%d.h5" % i)
q = fh.root.StructGridField
Xn, Yn, qn = projectOnFinerGrid_f(Xc, Yc, q)
fig = pylab.figure(1)
pylab.pcolormesh(Xn, Yn, pylab.transpose(qn), vmin=0.0, vmax=1.0)
pylab.axis('image')
pylab.title('T=%f' % T[i])
pylab.savefig('s141-vortex-waltz_%05d.png' % i)
pylab.close()
fh.close()
def ReperageAcc():
ax = (reperageSpeed[1:, 0] - reperageSpeed[0:-1, 0]) / dt[0:-1]
ay = (reperageSpeed[1:, 1] - reperageSpeed[0:-1, 1]) / dt[0:-1]
return pylab.transpose(pylab.array([ax, ay]))
return Eval, Evec
#-------------------------------------------------------------------------------
# End - defining functions -----------------------------------------------------
#-------------------------------------------------------------------------------
h = len(S)
s, U = jacobi(S, h)
iss = pylab.zeros((h,h), dtype = float) # inverse square-root of s
for i in range (h):
for j in range(h):
if j == i :
iss[i,j] = 1.0 / (math.sqrt(s[i]))
V = pylab.dot(U, iss)
# hamiltonian matrix when equation reduced to standard eigenvalue problem
Hbar = pylab.dot(pylab.transpose(V),pylab.dot(H,V))
n1 = len(Hbar)
Eval, Evec = jacobi(Hbar, n1)
# sorting output from Jacobi diagonalization
n2 = len(Eval)
for i in range(n2-1):
index = i
val = Eval[i]
for j in range(i+1, n2):
if Eval[j] < val:
index = j
val = Eval[j]
if index != i:
swap1(Eval, i, index)
swap2(Evec, i, index)
def fit_emp_prior(id,
param_type,
fast_fit=False,
generate_emp_priors=True,
zero_re=True,
alt_prior=False,
global_heterogeneity='Slightly'):
""" Fit empirical prior of specified type for specified model
Parameters
----------
id : int
The model id number for the job to fit
param_type : str, one of incidence, prevalence, remission, excess-mortality, prevalence_x_excess-mortality
The disease parameter to generate empirical priors for
Example
-------
>>> import fit_emp_prior
>>> fit_emp_prior.fit_emp_prior(2552, 'incidence')
"""
dir = dismod3.settings.JOB_WORKING_DIR % id
## load the model from disk or from web
import simplejson as json
import data
reload(data)
dm = dismod3.load_disease_model(id)
try:
model = data.ModelData.load(dir)
print 'loaded data from new format from %s' % dir
except (IOError, AssertionError):
model = data.ModelData.from_gbd_jsons(json.loads(dm.to_json()))
#model.save(dir)
print 'loaded data from json, saved in new format for next time in %s' % dir
## next block fills in missing covariates with zero
for col in model.input_data.columns:
if col.startswith('x_'):
model.input_data[col] = model.input_data[col].fillna(0.)
# also fill all covariates missing in output template with zeros
model.output_template = model.output_template.fillna(0)
# set all heterogeneity priors to Slightly for the global fit
for t in model.parameters:
if 'heterogeneity' in model.parameters[t]:
model.parameters[t]['heterogeneity'] = global_heterogeneity
t = {
'incidence': 'i',
'prevalence': 'p',
'remission': 'r',
'excess-mortality': 'f',
'prevalence_x_excess-mortality': 'pf'
}[param_type]
model.input_data = model.get_data(t)
if len(model.input_data) == 0:
print 'No data for type %s, exiting' % param_type
return dm
### For testing:
## speed up computation by reducing number of knots
## model.parameters[t]['parameter_age_mesh'] = [0, 10, 20, 40, 60, 100]
## smooth Slightly, Moderately, or Very
## model.parameters[t]['smoothness'] = dict(age_start=0, age_end=100, amount='Very')
## speed up computation be reducing data size
## predict_area = 'super-region_0'
## predict_year=2005
## predict_sex='total'
## subtree = nx.traversal.bfs_tree(model.hierarchy, predict_area)
## relevant_rows = [i for i, r in model.input_data.T.iteritems() \
## if (r['area'] in subtree or r['area'] == 'all')\
## and (r['year_end'] >= 1997) \
## and r['sex'] in [predict_sex, 'total']]
## model.input_data = model.input_data.ix[relevant_rows]
# testing changes
#model.input_data['effective_sample_size'] = pl.minimum(1.e3, model.input_data['effective_sample_size'])
#missing_ess = pl.isnan(model.input_data['effective_sample_size'])
#model.input_data['effective_sample_size'][missing_ess] = 1.
#model.input_data['z_overdisperse'] = 1.
#print model.describe(t)
#model.input_data = model.input_data[model.input_data['area'].map(lambda x: x in nx.bfs_tree(model.hierarchy, 'super-region_5'))]
#model.input_data = model.input_data = model.input_data.drop(['x_LDI_id_Updated_7July2011'], axis=1)
#model.input_data = model.input_data.filter([model.input_data['x_nottroponinuse'] == 0.]
#model.input_data = model.input_data[:100]
## speed up output by not making predictions for empirical priors
#generate_emp_priors = False
print 'fitting', t
model.vars += ism.age_specific_rate(model,
t,
reference_area='all',
reference_sex='total',
reference_year='all',
mu_age=None,
mu_age_parent=None,
sigma_age_parent=None,
rate_type=(t == 'rr') and 'log_normal'
or 'neg_binom',
zero_re=zero_re)
# for backwards compatibility, should be removed eventually
dm.model = model
dm.vars = model.vars[t]
vars = dm.vars
if fast_fit:
dm.map, dm.mcmc = dismod3.fit.fit_asr(model,
t,
iter=101,
burn=0,
thin=1,
tune_interval=100)
else:
dm.map, dm.mcmc = dismod3.fit.fit_asr(model,
t,
iter=50000,
burn=10000,
thin=40,
tune_interval=1000,
verbose=True)
stats = dm.vars['p_pred'].stats(batches=5)
dm.vars['data']['mu_pred'] = stats['mean']
dm.vars['data']['sigma_pred'] = stats['standard deviation']
stats = dm.vars['pi'].stats(batches=5)
dm.vars['data']['mc_error'] = stats['mc error']
dm.vars['data'][
'residual'] = dm.vars['data']['value'] - dm.vars['data']['mu_pred']
dm.vars['data']['abs_residual'] = pl.absolute(dm.vars['data']['residual'])
graphics.plot_fit(model,
data_types=[t],
ylab=['PY'],
plot_config=(1, 1),
fig_size=(8, 8))
if generate_emp_priors:
for a in [
dismod3.utils.clean(a) for a in dismod3.settings.gbd_regions
]:
print 'generating empirical prior for %s' % a
for s in dismod3.settings.gbd_sexes:
for y in dismod3.settings.gbd_years:
key = dismod3.utils.gbd_key_for(param_type, a, y, s)
if t in model.parameters and 'level_bounds' in model.parameters[
t]:
lower = model.parameters[t]['level_bounds']['lower']
upper = model.parameters[t]['level_bounds']['upper']
else:
lower = 0
upper = pl.inf
emp_priors = covariate_model.predict_for(
model, model.parameters[t], 'all', 'total', 'all', a,
dismod3.utils.clean(s), int(y), alt_prior, vars, lower,
upper)
dm.set_mcmc('emp_prior_mean', key, emp_priors.mean(0))
if 'eta' in vars:
N, A = emp_priors.shape # N samples, for A age groups
delta_trace = pl.transpose([
pl.exp(vars['eta'].trace()) for _ in range(A)
]) # shape delta matrix to match prediction matrix
emp_prior_std = pl.sqrt(
emp_priors.var(0) +
(emp_priors**2 / delta_trace).mean(0))
else:
emp_prior_std = emp_priors.std(0)
dm.set_mcmc('emp_prior_std', key, emp_prior_std)
pl.plot(model.parameters['ages'],
dm.get_mcmc('emp_prior_mean', key),
color='grey',
label=a,
zorder=-10,
alpha=.5)
pl.savefig(dir + '/prior-%s.png' % param_type)
store_effect_coefficients(dm, vars, param_type)
#graphics.plot_one_ppc(vars, t)
#pl.savefig(dir + '/prior-%s-ppc.png'%param_type)
graphics.plot_acorr(model)
pl.savefig(dir + '/prior-%s-convergence.png' % param_type)
graphics.plot_trace(model)
pl.savefig(dir + '/prior-%s-trace.png' % param_type)
graphics.plot_one_effects(model, t)
pl.savefig(dir + '/prior-%s-effects.png' % param_type)
# save results (do this last, because it removes things from the disease model that plotting function, etc, might need
try:
dm.save('dm-%d-prior-%s.json' % (id, param_type))
except IOError, e:
print e
def main():
import optparse
from numpy import sum
# Parse command line
parser = optparse.OptionParser(usage=USAGE)
parser.add_option("-p",
"--plot",
action="store_true",
help="Generate pdf with IR-spectrum")
parser.add_option("-i",
"--info",
action="store_true",
help="Set up/ Calculate vibrations & quit")
parser.add_option("-s",
"--suffix",
action="store",
help="Call suffix for binary e.g. 'mpirun -n 4 '",
default='')
parser.add_option("-r",
"--run",
action="store",
help="path to FHI-aims binary",
default='')
parser.add_option("-x",
"--relax",
action="store_true",
help="Relax initial geometry")
parser.add_option("-m",
"--molden",
action="store_true",
help="Output in molden format")
parser.add_option("-w",
"--distort",
action="store_true",
help="Output geometry distorted along imaginary modes")
parser.add_option("-t",
"--submit",
action="store",
help="""\
Path to submission script, string <jobname>
will be replaced by name + counter, string
<outfile> will be replaced by filename""")
parser.add_option("-d",
"--delta",
action="store",
type="float",
help="Displacement",
default=0.0025)
options, args = parser.parse_args()
if options.info:
print __doc__
sys.exit(0)
if len(args) != 2:
parser.error("Need exactly two arguments")
AIMS_CALL = options.suffix + ' ' + options.run
hessian_thresh = -1
name = args[0]
mode = args[1]
delta = options.delta
run_aims = False
if options.run != '': run_aims = True
submit_script = options.submit is not None
if options.plot:
import matplotlib as mpl
mpl.use('Agg')
from pylab import figure
if options.plot or mode == '1':
from pylab import savetxt, transpose, eig, argsort, sort,\
sign, pi, dot, sum, linspace, argmin, r_, convolve
# Constant from scipy.constants
bohr = constants.value('Bohr radius') * 1.e10
hartree = constants.value('Hartree energy in eV')
at_u = constants.value('atomic mass unit-kilogram relationship')
eV = constants.value('electron volt-joule relationship')
c = constants.value('speed of light in vacuum')
Ang = 1.0e-10
hbar = constants.value('Planck constant over 2 pi')
Avo = constants.value('Avogadro constant')
kb = constants.value('Boltzmann constant in eV/K')
hessian_factor = eV / (at_u * Ang * Ang)
grad_dipole_factor = (eV / (1. / (10 * c))) / Ang #(eV/Ang -> D/Ang)
ir_factor = 1
# Asign all filenames
inputgeomerty = 'geometry.in.' + name
inputcontrol = 'control.in.' + name
atomicmasses = 'masses.' + name + '.dat'
xyzfile = name + '.xyz'
moldenname = name + '.molden'
hessianname = 'hessian.' + name + '.dat'
graddipolename = 'grad_dipole.' + name + '.dat'
irname = 'ir.' + name + '.dat'
deltas = array([-delta, delta])
coeff = array([-1, 1])
c_zero = -1. / (2. * delta)
f = open('control.in', 'r') # read control.in template
template_control = f.read()
f.close
if submit_script:
f = open(options.submit, 'r') # read submission script template
template_job = f.read()
f.close
folder = '' # Dummy
########### Central Point ##################################################
if options.relax and mode == '0':
# First relax input geometry
filename = name + '.out'
folder = name + '_relaxation'
if not os.path.exists(folder): os.mkdir(folder) # Create folder
shutil.copy('geometry.in', folder + '/geometry.in') # Copy geometry
new_control = open(folder + '/control.in', 'w')
new_control.write(template_control +
'relax_geometry trm 1E-3\n') # Relax!
new_control.close()
os.chdir(folder) # Change directoy
print 'Central Point'
if run_aims:
os.system(AIMS_CALL + ' > ' +
filename) # Run aims and pipe the output
# into a file named 'filename'
if submit_script: replace_submission(template_job, name, 0, filename)
os.chdir('..')
############################################################################
# Check for relaxed geometry
if os.path.exists(folder + '/geometry.in.next_step'):
geometry = open(folder + '/geometry.in.next_step', 'r')
else:
geometry = open('geometry.in', 'r')
# Read input geometry
n_line = 0
struc = structure()
lines = geometry.readlines()
for line in lines:
n_line = n_line + 1
if line.rfind('set_vacuum_level') != -1: # Vacuum Level
struc.vacuum_level = float(split_line(line)[-1])
if line.rfind('lattice_vector') != -1: # Lattice vectors and periodic
lat = split_line(line)[1:]
struc.lattic_vector = append(struc.lattic_vector,
float64(array(lat))[newaxis, :],
axis=0)
struc.periodic = True
if line.rfind('atom') != -1: # Set atoms
line_vals = split_line(line)
at = Atom(line_vals[-1], line_vals[1:-1])
if n_line < len(lines):
nextline = lines[n_line]
if nextline.rfind(
'constrain_relaxation') != -1: # constrained?
at = Atom(line_vals[-1], line_vals[1:-1], True)
else:
at = Atom(line_vals[-1], line_vals[1:-1])
struc.join(at)
geometry.close()
n_atoms = struc.n()
n_constrained = n_atoms - sum(struc.constrained)
# Atomic mass file
mass_file = open(atomicmasses, 'w')
mass_vector = zeros([0])
for at_unconstrained in struc.atoms[struc.constrained == False]:
mass_vector = append(mass_vector,
ones(3) * 1. / sqrt(at_unconstrained.mass()))
line = '{0:10.5f}'.format(at_unconstrained.mass())
for i in range(3):
line = line + '{0:11.4f}'.format(at_unconstrained.coord[i])
line = line + '{0:}\n'.format(at_unconstrained.kind)
mass_file.writelines(line)
mass_file.close()
# Init
dip = zeros([n_constrained * 3, 3])
hessian = zeros([n_constrained * 3, n_constrained * 3])
index = 0
counter = 1
# Set up / Read folders for displaced atoms
for atom in arange(n_atoms)[struc.constrained == False]:
for coord in arange(3):
for delta in deltas:
filename=name+'.i_atom_'+str(atom)+'.i_coord_'+str(coord)+'.displ_'+\
str(delta)+'.out'
folder=name+'.i_atom_'+str(atom)+'.i_coord_'+str(coord)+'.displ_'+\
str(delta)
if mode == '0': # Put new geometry and control.in into folder
struc_new = copy.deepcopy(struc)
struc_new.atoms[atom].coord[coord]=\
struc_new.atoms[atom].coord[coord]+delta
geoname='geometry.i_atom_'+str(atom)+'.i_coord_'+str(coord)+\
'.displ_'+str(delta)+'.in'
if not os.path.exists(folder): os.mkdir(folder)
new_geo = open(folder + '/geometry.in', 'w')
newline='#\n# temporary structure-file for finite-difference '+\
'calculation of forces\n'
newline=newline+'# displacement {0:8.4f} of \# atom '.format(delta)+\
'{0:5} direction {1:5}\n#\n'.format(atom,coord)
new_geo.writelines(newline + struc_new.to_str())
new_geo.close()
new_control = open(folder + '/control.in', 'w')
template_control = template_control.replace(
'relax_geometry', '#relax_geometry')
new_control.write(template_control+'compute_forces .true. \n'+\
'final_forces_cleaned '+\
'.true. \noutput dipole \n')
new_control.close()
os.chdir(folder) # Change directoy
print 'Processing atom: '+str(atom+1)+'/'+str(n_atoms)+', coord.: '+\
str(coord+1)+'/'+str(3)+', delta: '+str(delta)
if run_aims:
os.system(AIMS_CALL + ' > ' +
filename) # Run aims and pipe the output
# into a file named 'filename'
if submit_script:
replace_submission(template_job, name, counter,
filename)
# os.system('qsub job.sh') # Mind the environment variables
os.chdir('..')
if mode == '1': # Read output
forces_reached = False
atom_count = 0
data = open(folder + '/' + filename)
for line in data.readlines():
if line.rfind(
'Dipole correction potential jump') != -1:
dip_jump = float(split_line(line)[-2]) # Periodic
if line.rfind('| Total dipole moment [eAng]') != -1:
dip_jump = float64(
split_line(line)[-3:]) # Cluster
if forces_reached and atom_count < n_atoms: # Read Forces
struc.atoms[atom_count].force = float64(
split_line(line)[2:])
atom_count = atom_count + 1
if atom_count == n_atoms:
forces_reached = False
if line.rfind('Total atomic forces') != -1:
forces_reached = True
data.close()
if struc.periodic:
dip[index, 2] = dip[
index,
2] + dip_jump * coeff[deltas == delta] * c_zero
else:
dip[index, :] = dip[index, :] + dip_jump * coeff[
deltas == delta] * c_zero
forces = array([])
for at_unconstrained in struc.atoms[struc.constrained ==
False]:
forces = append(
forces,
coeff[deltas == delta] * at_unconstrained.force)
hessian[index, :] = hessian[index, :] + forces * c_zero
counter = counter + 1
index = index + 1
if mode == '1': # Calculate vibrations
print 'Entering hessian diagonalization'
print 'Number of atoms = ' + str(n_atoms)
print 'Name of Hessian input file = ' + hessianname
print 'Name of grad dipole input file = ' + graddipolename
print 'Name of Masses input file = ' + atomicmasses
print 'Name of XYZ output file = ' + xyzfile
print 'Threshold for Matrix elements = ' + str(hessian_thresh)
if (hessian_thresh < 0.0): print ' All matrix elements are taken'+\
' into account by default\n'
savetxt(hessianname, hessian)
savetxt(graddipolename, dip)
mass_mat = mass_vector[:, newaxis] * mass_vector[newaxis, :]
hessian[abs(hessian) < hessian_thresh] = 0.0
hessian = hessian * mass_mat * hessian_factor
hessian = (hessian + transpose(hessian)) / 2.
# Diagonalize hessian (scipy)
print 'Solving eigenvalue system for Hessian Matrix'
freq, eig_vec = eig(hessian)
print 'Done ... '
eig_vec = eig_vec[:, argsort(freq)]
freq = sort(sign(freq) * sqrt(abs(freq)))
ZPE = hbar * (freq) / (2.0 * eV)
freq = (freq) / (200. * pi * c)
grad_dipole = dip * grad_dipole_factor
eig_vec = eig_vec * mass_vector[:, newaxis] * ones(
len(mass_vector))[newaxis, :]
infrared_intensity = sum(dot(transpose(grad_dipole),eig_vec)**2,axis=0)*\
ir_factor
reduced_mass = sum(eig_vec**2, axis=0)
norm = sqrt(reduced_mass)
eig_vec = eig_vec / norm
# The rest is output, xyz, IR,...
print 'Results\n'
print 'List of all frequencies found:'
print 'Mode number Frequency [cm^(-1)] Zero point energy [eV] '+\
'IR-intensity [D^2/Ang^2]'
for i in range(len(freq)):
print '{0:11}{1:25.8f}{2:25.8f}{3:25.8f}'.format(
i + 1, freq[i], ZPE[i], infrared_intensity[i])
print '\n'
print 'Summary of zero point energy for entire system:'
print '| Cumulative ZPE = {0:15.8f} eV'.format(sum(ZPE))
print '| without first six eigenmodes = {0:15.8f} eV\n'.format(
sum(ZPE) - sum(ZPE[:6]))
print 'Stability checking - eigenvalues should all be positive for a '+\
'stable structure. '
print 'The six smallest frequencies should be (almost) zero:'
string = ''
for zz in ZPE[:6]:
string = string + '{0:25.8f}'.format(zz)
print string
print 'Compare this with the largest eigenvalue, '
print '{0:25.8f}'.format(freq[-1])
nums = arange(n_atoms)[struc.constrained == False]
nums2 = arange(n_atoms)[struc.constrained]
newline = ''
newline_ir = '[INT]\n'
if options.molden:
newline_molden = '[Molden Format]\n[GEOMETRIES] XYZ\n'
newline_molden = newline_molden + '{0:6}\n'.format(n_atoms) + '\n'
for i_atoms in range(n_constrained):
newline_molden = newline_molden + '{0:6}'.format(
struc.atoms[nums[i_atoms]].kind)
for i_coord in range(3):
newline_molden = newline_molden + '{0:10.4f}'.format(
struc.atoms[nums[i_atoms]].coord[i_coord])
newline_molden = newline_molden + '\n'
newline_molden = newline_molden + '[FREQ]\n'
for i in range(len(freq)):
newline_molden = newline_molden + '{0:10.3f}\n'.format(freq[i])
newline_molden = newline_molden + '[INT]\n'
for i in range(len(freq)):
newline_molden = newline_molden + '{0:17.6e}\n'.format(
infrared_intensity[i])
newline_molden = newline_molden + '[FR-COORD]\n'
newline_molden = newline_molden + '{0:6}\n'.format(n_atoms) + '\n'
for i_atoms in range(n_constrained):
newline_molden = newline_molden + '{0:6}'.format(
struc.atoms[nums[i_atoms]].kind)
for i_coord in range(3):
newline_molden = newline_molden + '{0:10.4f}'.format(
struc.atoms[nums[i_atoms]].coord[i_coord] / bohr)
newline_molden = newline_molden + '\n'
newline_molden = newline_molden + '[FR-NORM-COORD]\n'
for i in range(len(freq)):
newline = newline + '{0:6}\n'.format(n_atoms)
if freq[i] > 0:
newline = newline + 'stable frequency at '
elif freq[i] < 0:
newline = newline + 'unstable frequency at '
if options.distort and freq[i] < -50:
struc_new = copy.deepcopy(struc)
for i_atoms in range(n_constrained):
for i_coord in range(3):
struc_new.atoms[i_atoms].coord[i_coord]=\
struc_new.atoms[i_atoms].coord[i_coord]+\
eig_vec[(i_atoms)*3+i_coord,i]
geoname = name + '.distorted.vibration_' + str(
i + 1) + '.geometry.in'
new_geo = open(geoname, 'w')
newline_geo = '#\n# distorted structure-file for based on eigenmodes\n'
newline_geo=newline_geo+\
'# vibration {0:5} :{1:10.3f} 1/cm\n#\n'.format(i+1,freq[i])
new_geo.writelines(newline_geo + struc_new.to_str())
new_geo.close()
elif freq[i] == 0:
newline = newline + 'translation or rotation '
newline = newline + '{0:10.3f} 1/cm IR int. is '.format(freq[i])
newline = newline + '{0:10.4e} D^2/Ang^2; red. mass is '.format(
infrared_intensity[i])
newline = newline + '{0:5.3f} a.m.u.; force const. is '.format(
1.0 / reduced_mass[i])
newline = newline + '{0:5.3f} mDyne/Ang.\n'.format(
((freq[i] *
(200 * pi * c))**2) * (1.0 / reduced_mass[i]) * at_u * 1.e-2)
if options.molden: newline_molden=newline_molden+\
'vibration {0:6}\n'.format(i+1)
for i_atoms in range(n_constrained):
newline = newline + '{0:6}'.format(
struc.atoms[nums[i_atoms]].kind)
for i_coord in range(3):
newline = newline + '{0:10.4f}'.format(
struc.atoms[nums[i_atoms]].coord[i_coord])
for i_coord in range(3):
newline = newline + '{0:10.4f}'.format(
eig_vec[(i_atoms) * 3 + i_coord, i])
if options.molden:
newline_molden = newline_molden + '{0:10.4f}'.format(
eig_vec[(i_atoms) * 3 + i_coord, i] / bohr)
newline = newline + '\n'
if options.molden: newline_molden = newline_molden + '\n'
for i_atoms in range(n_atoms - n_constrained):
newline = newline + '{0:6}'.format(
struc.atoms[nums2[i_atoms]].kind)
for i_coord in range(3):
newline = newline + '{0:10.4f}'.format(
struc.atoms[nums2[i_atoms]].coord[i_coord])
for i_coord in range(3):
newline = newline + '{0:10.4f}'.format(0.0)
newline = newline + '\n'
newline_ir = newline_ir + '{0:10.4e}\n'.format(
infrared_intensity[i])
xyz = open(xyzfile, 'w')
xyz.writelines(newline)
xyz.close()
ir = open(irname, 'w')
ir.writelines(newline_ir)
ir.close()
if options.molden:
molden = open(moldenname, 'w')
molden.writelines(newline_molden)
molden.close()
if mode == '1' and options.plot:
x = linspace(freq.min() - 500, freq.max() + 500, 1000)
z = zeros(len(x))
for i in range(len(freq)):
z[argmin(abs(x - freq[i]))] = infrared_intensity[i]
window_len = 150
gauss = signal.gaussian(window_len, 10)
s = r_[z[window_len - 1:0:-1], z, z[-1:-window_len:-1]]
z_convolve = convolve(gauss / gauss.sum(), s,
mode='same')[window_len - 1:-window_len + 1]
fig = figure(0)
ax = fig.add_subplot(111)
ax.plot(x, z_convolve, 'r', lw=2)
ax.set_xlim([freq.min() - 500, freq.max() + 500])
ax.set_ylim([-0.01, ax.get_ylim()[1]])
ax.set_yticks([])
ax.set_xlabel('Frequency [1/cm]', size=20)
ax.set_ylabel('Intensity [a.u.]', size=20)
fig.savefig(name + '_IR_spectrum.pdf')
print '\n Done. '
frames = [100]
sims = [215, 217, 218, 219]
alpha = [0.1, 0.3, 1.0, 2.0]
fig = pylab.figure(1)
count = 1
for s in sims:
print "Working on sim %s (count %d)" % (s, count)
f = 100
fh = tables.openFile("../s%d/s%d-hw_phi_%d.h5" % (s, s, f))
q = fh.root.StructGridField
Xn, Yn, qn = projectOnFinerGrid_f39(Xc, Yc, q)
pylab.subplot(2, 2, count)
pylab.title('Adiabacity %g' % alpha[count - 1])
pylab.pcolormesh(Xn, Yn, -pylab.transpose(qn))
pylab.axis('image')
count = count + 1
pylab.savefig("hw-cmp-phi_%d.png" % s, dpi=400)
pylab.close()
fig = pylab.figure(2)
count = 1
for s in sims:
print "Working on sim %s (count %d)" % (s, count)
f = 100
fh = tables.openFile("../s%d/s%d-hw_chi_%d.h5" % (s, s, f))
q = fh.root.StructGridField
Xn, Yn, qn = projectOnFinerGrid_f39(Xc, Yc, q)
fi = FiltFiltOctave(source=t, band=freq, fraction='Third octave')
bt = BeamformerTimeSq(source=fi, grid=g, mpos=m, r_diag=True, c=c0)
avgt = TimeAverage(source=bt,
naverage=int(sfreq * tmax / 16)) # 16 single images
cacht = TimeCache(source=avgt) # cache to prevent recalculation
map2 = zeros(g.shape) # accumulator for average
# plot single frames
figure(1, (8, 7))
i = 1
for res in cacht.result(1):
res0 = res[0].reshape(g.shape)
map2 += res0 # average
i += 1
subplot(4, 4, i)
mx = L_p(res0.max())
imshow(L_p(transpose(res0)), vmax=mx, vmin=mx-10, interpolation='nearest',\
extent=g.extend(), origin='lower')
colorbar()
map2 /= i
subplot(4, 4, 1)
text(0.4, 0.25, 'fixed\nfocus', fontsize=15, ha='center')
axis('off')
tight_layout()
#===============================================================================
# moving focus time domain beamforming
#===============================================================================
# new grid needed, the trajectory starts at origin and is oriented towards +x
# thus, with the circular movement assumed, the center of rotation is at (0,2.5)
Xf_8 = pylab.linspace(0, 1, nx)
Yf_8 = pylab.linspace(0.5 * dy, 1 - 0.5 * dy, ny - 1)
q_8 = q[:, :-1, 2]
Xhr = pylab.linspace(0, 1, 101)
Yhr = pylab.linspace(0, 1, 101)
fhr = exactSol(2, 5, Xhr, Yhr)
vmin, vmax = fhr.min(), fhr.max()
# make plots
f1 = pylab.figure(1)
pylab.subplot(1, 2, 1)
cax = pylab.pcolormesh(Xf,
Yf,
pylab.transpose(q[:, :, 0]),
vmin=vmin,
vmax=vmax)
pylab.axis('image')
pylab.subplot(1, 2, 2)
cax = pylab.pcolormesh(Xhr, Yhr, fhr)
pylab.axis('image')
# compute error
fex = exactSol(2, 5, Xf, Yf)
error = numpy.abs(fex - pylab.transpose(q_1)).sum()
fex = exactSol(2, 5, Xf_5, Yf_5)
error = error + numpy.abs(fex - pylab.transpose(q_5)).sum()
def yfit(self): return pl.dot(pl.transpose(self.M),self.pars)
d = gkedata.GkeData("s1-em-landau_distfElc_0.h5")
dg1_0 = gkedgbasis.GkeDgSerendipNorm2DPolyOrder2Basis(d)
d = gkedata.GkeData("s1-em-landau_distfElc_1.h5")
dg1_1 = gkedgbasis.GkeDgSerendipNorm2DPolyOrder2Basis(d)
d = gkedata.GkeData("s1-em-landau_distfElc_2.h5")
dg1_2 = gkedgbasis.GkeDgSerendipNorm2DPolyOrder2Basis(d)
Xc, Yc, fve_0 = dg1_0.project(0)
Xc, Yc, fve_1 = dg1_1.project(0)
Xc, Yc, fve_2 = dg1_2.project(0)
figure(1)
subplot(2, 1, 1)
im = pcolormesh(Xc, Yc, pylab.transpose(fve_1 - fve_0))
axis('tight')
colorbar_adj(im)
subplot(2, 1, 2)
im = pcolormesh(Xc, Yc, pylab.transpose(fve_2 - fve_0))
axis('tight')
colorbar_adj(im)
savefig('s1-em-landau-deltaF.png')
figure(2)
im = pcolormesh(Xc, Yc, pylab.transpose(fve_2))
axis('tight')
colorbar_adj(im)
savefig('s1-em-landau-deltaF.png')
X, V = getXv(Xc, Yc)
figure(1)
plot(V, fve[fve.shape[0]/2, :], 'r-')
ylo, yup = gca().get_ylim()
plot([1.0, 1.0], [ylo, yup], '--k')
plot([2.0, 2.0], [ylo, yup], '--k')
gca().set_ylim([0, 0.4])
title('Time %g' % d.time)
xlabel('V')
ylabel('f(V)')
savefig('r3-es-resonance-fve1_%05d.png' % i)
close()
figure(2)
subplot(2,1,1)
im = pcolormesh(Xc, Yc, pylab.transpose(fve))
plot([-2*pi,2*pi], [1.0, 1.0], 'k--', linewidth=2.0)
plot([-2*pi,2*pi], [2.0, 2.0], 'k--', linewidth=2.0)
axis('tight')
colorbar_adj(im)
subplot(2,1,2)
im = pcolormesh(Xc, Yc, pylab.transpose(fve-fve0))
plot([-2*pi,2*pi], [1.0, 1.0], 'k--', linewidth=2.0)
plot([-2*pi,2*pi], [2.0, 2.0], 'k--', linewidth=2.0)
#axis('tight')
gca().set_ylim([0.0, 4.0])
gca().set_xlim([-2*pi, 2*pi])
colorbar_adj(im)
suptitle('Time %g' % d.time)