本文整理汇总了Python中vtktools.arr函数的典型用法代码示例。如果您正苦于以下问题:Python arr函数的具体用法?Python arr怎么用?Python arr使用的例子?那么恭喜您, 这里精选的函数代码示例或许可以为您提供帮助。
在下文中一共展示了arr函数的20个代码示例,这些例子默认根据受欢迎程度排序。您可以为喜欢或者感觉有用的代码点赞,您的评价将有助于我们的系统推荐出更棒的Python代码示例。
示例1: calc_mld
def calc_mld(files,start,x0=0.0,y0=0.0):
""" Caclulate density-based MLD from a bunch of VTU files
"""
mld = []
times = []
dates = []
for file in files:
try:
os.stat(file)
except:
print("No such file: %s" % file)
sys.exit(1)
# open vtu and derive the field indices of the edge at (x=0,y=0) ordered by depth
u=vtktools.vtu(file)
pos = u.GetLocations()
ind = get_1d_indices(pos, x0, y0)
# from this we can derive the 1D profile of any field like this:
depth = vtktools.arr([-pos[i,2] for i in ind])
# handle time for different types of plots
time = u.GetScalarField('Time')
times.append(time[0]) # seconds
dates.append( date2num(start + timedelta(seconds=time[0])) ) # integer datetime
# grab density profile and calculate MLD_den (using 2 different deviation parameters
d = u.GetScalarField('Density')
den = vtktools.arr( [d[i] * 1000 for i in ind] )
mld.append( calc_mld_den(den, depth) ) #den0 = 0.03 is default
return mld, times, dates
开发者ID:FluidityProject,项目名称:fluidity,代码行数:35,代码来源:gls_ocean_param.py
示例2: calc_mld_tke_files
def calc_mld_tke_files(files,start,x0=0.0,y0=0.0):
""" Caclulate tke-based MLD from a bunch of VTU files
"""
mld = []
times = []
dates = []
for file in files:
try:
os.stat(file)
except:
print "No such file: %s" % file
sys.exit(1)
# open vtu and derive the field indices of the edge at (x=0,y=0) ordered by depth
u=vtktools.vtu(file)
pos = u.GetLocations()
ind = get_1d_indices(pos, x0, y0)
# from this we can derive the 1D profile of any field like this:
depth = vtktools.arr([-pos[i,2] for i in ind])
# handle time for different types of plots
time = u.GetScalarField('Time')
times.append(time[0]) # seconds
dates.append( date2num(start + timedelta(seconds=time[0])) ) # integer datetime
# grab density profile and calculate MLD
d = u.GetScalarField('GLSTurbulentKineticEnergy')
tke = vtktools.arr( [d[i] for i in ind] )
mld.append( calc_mld_tke(tke, depth) )
return mld, times, dates
开发者ID:jhill1,项目名称:python_scripts,代码行数:35,代码来源:mld_util.py
示例3: plot_2d_data
def plot_2d_data(data,depths,time_secs,start_date,file_path,axis_label,finish_date=None,mld_data=None,max_depth=150,interval=3,minimum=None,maximum=None,spacing=None,colour_scale=cm.jet,dates=None):
"""
"""
# turn given 2d-arrays into numpy arrays (in case they are not already)
data = vtktools.arr(data)
time_secs = vtktools.arr(time_secs)
depths = vtktools.arr(depths)
# convert time profiles in seconds into months
start = datetime.strptime(start_date, "%Y-%m-%d %H:%M:%S")
if (dates == None):
dates = time_secs
i = 0
for time in time_secs:
t = float(time[0].item())
dates[i,:] = date2num(start + timedelta(seconds=t))
i += 1
# see if finishing date is given, default to last time given
if (finish_date != None):
finish = datetime.strptime(finish_date, "%Y-%m-%d %H:%M:%S")
else:
finish = dates[-1][0]
# define min/max and spacing of data if not given (so we see all of the data)
if (minimum == None):
minimum = data.min()
minimum = minimum - (0.1*minimum)
if (maximum == None):
maximum = data.max()
maximum = maximum + (0.1*maximum)
if (spacing == None):
spacing = (maximum - minimum) /256.
# plot 2d colour graph...
fig = figure(figsize=(15,8),dpi=90)
ax = fig.add_axes([.1,.18,.9,.7])
cs=ax.contour(dates, depths, data, arange(minimum,maximum,spacing),cmap=colour_scale)
cs=ax.contourf(dates, depths, data, arange(minimum,maximum,spacing),cmap=colour_scale)
pp=colorbar(cs,format='%.2f')
if(mld_data!=None):
ax.plot(dates[:,0],mld_data,'w', alpha=0.7)
dateFmt = mpl.dates.DateFormatter('%m/%Y')
ax.xaxis.set_major_formatter(dateFmt)
monthsLoc = mpl.dates.MonthLocator(interval=interval)
ax.xaxis.set_major_locator(monthsLoc)
labels = ax.get_xticklabels()
for label in labels:
label.set_rotation(30)
ax.set_ylim(max_depth, 0)
ax.set_xlim(start,finish)
pp.set_label(axis_label)
xlabel('Date (mm/yyyy)')
ylabel('Depth (m)')
form = file_path.split('.')[-1].strip()
savefig(file_path, dpi=90,format=form)
close(fig)
开发者ID:jhill1,项目名称:python_scripts,代码行数:59,代码来源:mld_util.py
示例4: botella_p1
def botella_p1(NN):
#Botella and Peyret (1998) Table 9.
filelist_not_sorted = glob.glob('driven_cavity-%d/*.vtu'%NN)
vtu_nos_not_sorted = [int(file.split('.vtu')[0].split('_')[-1]) for file in filelist_not_sorted]
filelist = [filelist_not_sorted[i] for i in numpy.argsort(vtu_nos_not_sorted)]
file = filelist[-1]
print file
try:
os.stat(file)
except:
print "No such file: %s" % file
sys.exit(1)
u=vtktools.vtu(file)
pts=vtktools.arr([
[0.5, 0.0000, 0.0, 0.110591],
[0.5, 0.0547, 0.0, 0.109689],
[0.5, 0.0625, 0.0, 0.109200],
[0.5, 0.0703, 0.0, 0.108566],
[0.5, 0.1016, 0.0, 0.104187],
[0.5, 0.1719, 0.0, 0.081925],
[0.5, 0.2813, 0.0, 0.040377],
[0.5, 0.4531, 0.0, 0.004434],
[0.5, 0.5000, 0.0, 0.000000],
[0.5, 0.6172, 0.0, -0.000827],
[0.5, 0.7344, 0.0, 0.012122],
[0.5, 0.8516, 0.0, 0.034910],
[0.5, 0.9531, 0.0, 0.050329],
[0.5, 0.9609, 0.0, 0.050949],
[0.5, 0.9688, 0.0, 0.051514],
[0.5, 0.9766, 0.0, 0.052009],
[0.5, 1.0000, 0.0, 0.052987]])
velocity = u.ProbeData(pts, "Velocity")
(ilen, jlen) = velocity.shape
pressure = u.ProbeData(pts, "Pressure")
pts0=vtktools.arr([[0.5, 0.5, 0.0]]) # We're going to subtract off the pressure at the centre point
press0 = u.ProbeData(pts0, "Pressure")
norm=0.0
for i in range(ilen):
diff = pts[i][3] - (pressure[i][0]-press0[0][0])
norm = norm + diff*diff
norm = math.sqrt(norm/ilen)
print "botella_p1_norm:", norm
return norm
开发者ID:fmilthaler,项目名称:DAKOTA-Fluidity-examples,代码行数:49,代码来源:driven_cavity.py
示例5: botella_p2
def botella_p2(NN):
#Botella and Peyret (1998) Table 10.
filelist_not_sorted = glob.glob('driven_cavity-%d/*.vtu'%NN)
vtu_nos_not_sorted = [int(file.split('.vtu')[0].split('_')[-1]) for file in filelist_not_sorted]
filelist = [filelist_not_sorted[i] for i in numpy.argsort(vtu_nos_not_sorted)]
file = filelist[-1]
print file
try:
os.stat(file)
except:
print "No such file: %s" % file
sys.exit(1)
u=vtktools.vtu(file)
pts=vtktools.arr([
[1.0000, 0.5, 0.0, 0.077455],
[0.9688, 0.5, 0.0, 0.078837],
[0.9609, 0.5, 0.0, 0.078685],
[0.9531, 0.5, 0.0, 0.078148],
[0.9453, 0.5, 0.0, 0.077154],
[0.9063, 0.5, 0.0, 0.065816],
[0.8594, 0.5, 0.0, 0.049029],
[0.8047, 0.5, 0.0, 0.034552],
[0.5000, 0.5, 0.0, 0.000000],
[0.2344, 0.5, 0.0, 0.044848],
[0.2266, 0.5, 0.0, 0.047260],
[0.1563, 0.5, 0.0, 0.069511],
[0.0938, 0.5, 0.0, 0.084386],
[0.0781, 0.5, 0.0, 0.086716],
[0.0703, 0.5, 0.0, 0.087653],
[0.0625, 0.5, 0.0, 0.088445],
[0.0000, 0.5, 0.0, 0.090477]])
velocity = u.ProbeData(pts, "Velocity")
(ilen, jlen) = velocity.shape
pressure = u.ProbeData(pts, "Pressure")
pts0=vtktools.arr([[0.5, 0.5, 0.0]]) # We're going to subtract off the pressure at the centre point
press0 = u.ProbeData(pts0, "Pressure")
norm=0.0
for i in range(ilen):
diff = pts[i][3] - (pressure[i][0]-press0[0][0])
norm = norm + diff*diff
norm = math.sqrt(norm/ilen)
print "botella_p2_norm:", norm
return norm
开发者ID:fmilthaler,项目名称:DAKOTA-Fluidity-examples,代码行数:49,代码来源:driven_cavity.py
示例6: plot_1d_comparison
def plot_1d_comparison(data_dict,style_dict,time_dict,start_date,finish_date,file_path,axis_label,interval=3):
"""
"""
start_time = date2num(datetime.strptime(start_date, "%Y-%m-%d %H:%M:%S"))
finish_time = date2num(datetime.strptime(finish_date, "%Y-%m-%d %H:%M:%S"))
# plot 1d graph...
fig = figure(figsize=(15,8),dpi=90)
ax = fig.add_axes([.05,.12,.9,.85])
max_value = 0.0
for key, data_arr in data_dict.iteritems():
ax.plot(time_dict[key],data_arr,style_dict[key], label=key)
data_arr = vtktools.arr(data_arr)
if data_arr.max() > max_value:
max_value = data_arr.max()
max_value += max_value * 0.1
dateFmt = mpl.dates.DateFormatter('%m/%Y')
ax.xaxis.set_major_formatter(dateFmt)
monthsLoc = mpl.dates.MonthLocator(interval=interval)
ax.xaxis.set_major_locator(monthsLoc)
labels = ax.get_xticklabels()
for label in labels:
label.set_rotation(30)
ax.set_ylim(max_value, 0)
ax.set_xlim(start_time,finish_time)
xlabel('Date (mm/yyyy)')
ylabel(axis_label)
legend(loc=0)
form = file_path.split('.')[-1].strip()
savefig(file_path, dpi=90,format=form)
close(fig)
开发者ID:jhill1,项目名称:python_scripts,代码行数:33,代码来源:mld_util.py
示例7: MLD
def MLD(filelist):
x0 = 0.
tke0 = 1.0e-5
last_mld = 0
times = []
depths = []
Dm = []
for file in filelist:
try:
os.stat(file)
except:
print "No such file: %s" % file
sys.exit(1)
u=vtktools.vtu(file)
time = u.GetScalarField('Time')
tt = time[0]
kk = u.GetScalarField('GLSTurbulentKineticEnergy')
pos = u.GetLocations()
# ignore first 4 hours of simulaiton
if (tt < 14400):
continue
xyzkk = []
for i in range(0,len(kk)):
if( abs(pos[i,0] - x0) < 0.1 ):
xyzkk.append((pos[i,0],-pos[i,1],pos[i,2],(kk[i])))
xyzkkarr = vtktools.arr(xyzkk)
III = argsort(xyzkkarr[:,1])
xyzkkarrsort = xyzkkarr[III,:]
# march down the column, grabbing the last value above tk0 and the first
# one less than tke0. Interpolate between to get the MLD
kea = 1000
keb = 0
zza = 0
zzb = 0
for values in xyzkkarrsort:
if (values[3] > tke0):
kea = values[3]
zza = -values[1]
if (values[3] < tke0):
keb = values[3]
zzb = -values[1]
break
# the MLD is somewhere between these two values - let's estimate half way!
mld = (zzb+zza)/2.
if (last_mld == mld):
continue
times.append(tt/3600)
depths.append(-1.0*mld)
last_mld = mld
Dm.append(1.05*0.00988211768*(1.0/sqrt(0.01))*sqrt(tt))
return times, depths, Dm
开发者ID:Nasrollah,项目名称:fluidity,代码行数:59,代码来源:mld_calc.py
示例8: plot_tracer
def plot_tracer(vtu_file, line=None):
u=vtktools.vtu(vtu_file)
pos = u.GetLocations()
time = u.GetScalarField('Time')[0]
t = u.GetScalarField('Tracer')
ind = get_1d_indices(pos)
distance = vtktools.arr([pos[i,0] for i in ind])
tracer = vtktools.arr( [t[i] for i in ind] )
if (line):
line.set_ydata(tracer) # update the data
draw()
else:
line, = plot(distance,tracer,color='k')
return line
开发者ID:FluidityProject,项目名称:training,代码行数:17,代码来源:visualise.py
示例9: MLD
def MLD(filelist):
x0 = 0.
tke0 = 1.0e-5
last_mld = 0
times = []
depths = []
for file in filelist:
try:
os.stat(file)
except:
print("No such file: %s" % file)
sys.exit(1)
u=vtktools.vtu(file)
time = u.GetScalarField('Time')
tt = time[0]
kk = u.GetScalarField('GLSTurbulentKineticEnergy')
pos = u.GetLocations()
if (tt < 100):
continue
xyzkk = []
for i in range(0,len(kk)):
if( abs(pos[i,0] - x0) < 0.1 ):
xyzkk.append((pos[i,0],-pos[i,1],pos[i,2],(kk[i])))
xyzkkarr = vtktools.arr(xyzkk)
III = argsort(xyzkkarr[:,1])
xyzkkarrsort = xyzkkarr[III,:]
# march down the column, grabbing the last value above tk0 and the first
# one less than tke0. Interpolate between to get the MLD
kea = 1000
keb = 0
zza = 0
zzb = 0
for values in xyzkkarrsort:
if (values[3] > tke0):
kea = values[3]
zza = -values[1]
if (values[3] < tke0):
keb = values[3]
zzb = -values[1]
break
mld = zza
if (last_mld == mld):
continue
times.append(tt/3600)
depths.append(-1.0*mld)
last_mld = mld
return times, depths
开发者ID:FluidityProject,项目名称:fluidity,代码行数:54,代码来源:mixed_layer_depth_all.py
示例10: getDistanceMeshDensity
def getDistanceMeshDensity(file):
v = vtktools.vtu(file)
l = [0.0] * v.ugrid.GetNumberOfPoints()
a = vtktools.arr(l)
for i in range(v.ugrid.GetNumberOfPoints()):
neighbours = v.GetPointPoints(i)
sum = 0.0
for neighbour in neighbours:
sum = sum + v.GetDistance(i, neighbour)
a[i] = sum / len(neighbours)
return a
开发者ID:FluidityProject,项目名称:multifluids,代码行数:11,代码来源:fluidity_tools.py
示例11: getData
def getData(file, xmin=float('nan'), xmax=float('nan'), ymin=float('nan'), ymax=float('nan'), step_x=1,step_y=1):
u=vtktools.vtu(file)
print numpy.isnan(xmin), numpy.isnan(xmax), numpy.isnan(ymin), numpy.isnan(ymax)
if numpy.isnan(xmin):
xmin=u.ugrid.GetBounds()[0]
print 'xmin = ', xmin
if numpy.isnan(ymin):
ymin=u.ugrid.GetBounds()[2]
print 'ymin = ', ymin
if numpy.isnan(xmax):
xmax=u.ugrid.GetBounds()[1]
print 'xmax = ', xmax
if numpy.isnan(ymax):
ymax=u.ugrid.GetBounds()[3]
print 'ymax = ', ymax
Xlist = numpy.arange(xmin,xmax,step_x)# x coordinates
Ylist = numpy.arange(ymin,ymax,step_y)# y coordinates
[X0,Y0] = scipy.meshgrid(Xlist,Ylist)
X0=X0.transpose()
Y0=Y0.transpose()
print Xlist.shape, Ylist.shape, X0.shape, Y0.shape
Z0 = 0.0*Y0 # This is 2d so z is an array of zeros.
X = numpy.reshape(X0,(numpy.size(X0),))
Y = numpy.reshape(Y0,(numpy.size(Y0),))
Z = numpy.reshape(Z0,(numpy.size(Z0),))
pts = zip(X,Y,Z)
pts = vtktools.arr(pts)
# create arrays of velocity and temperature values at the desired points
sol = u.ProbeData(pts, 'solution')
print sol.shape, Xlist.shape, Ylist.shape
#temperature_structured = u.ProbeData(pts, 'Temperature')
numpy.savetxt("pts.dat", zip(X,Y,sol))
sol = sol.reshape((numpy.size(Xlist),numpy.size(Ylist)))
x=[]
y=[]
z=[]
for i in range(len(Xlist)):
for j in range(len(Ylist)):
#print i,j
x.append(X0[i,j])
y.append(Y0[i,j])
z.append(sol[i,j])
numpy.savetxt("pts2.dat", numpy.array(zip(x, y, z)))
#data = scipy.interpolate.RectBivariateSpline(Xlist,Ylist,sol)
# return Xlist, Ylist, sol
return Xlist,Ylist,sol
开发者ID:ipbs,项目名称:ipbs,代码行数:52,代码来源:getData.py
示例12: erturk_v
def erturk_v(NN):
#Erturk et al 2005. Table VII
filelist_not_sorted = glob.glob('driven_cavity-%d/*.vtu'%NN)
vtu_nos_not_sorted = [int(file.split('.vtu')[0].split('_')[-1]) for file in filelist_not_sorted]
filelist = [filelist_not_sorted[i] for i in numpy.argsort(vtu_nos_not_sorted)]
file = filelist[-1]
print file
try:
os.stat(file)
except:
print "No such file: %s" % file
sys.exit(1)
u=vtktools.vtu(file)
pts=vtktools.arr([
[0.000, 0.5, 0.0, 0.0000],
[0.015, 0.5, 0.0, 0.1019],
[0.030, 0.5, 0.0, 0.1792],
[0.045, 0.5, 0.0, 0.2349],
[0.060, 0.5, 0.0, 0.2746],
[0.075, 0.5, 0.0, 0.3041],
[0.090, 0.5, 0.0, 0.3273],
[0.105, 0.5, 0.0, 0.3460],
[0.120, 0.5, 0.0, 0.3605],
[0.135, 0.5, 0.0, 0.3705],
[0.150, 0.5, 0.0, 0.3756],
[0.500, 0.5, 0.0, 0.0258],
[0.850, 0.5, 0.0, -0.4028],
[0.865, 0.5, 0.0, -0.4407],
[0.880, 0.5, 0.0, -0.4803],
[0.895, 0.5, 0.0, -0.5132],
[0.910, 0.5, 0.0, -0.5263],
[0.925, 0.5, 0.0, -0.5052],
[0.940, 0.5, 0.0, -0.4417],
[0.955, 0.5, 0.0, -0.3400],
[0.970, 0.5, 0.0, -0.2173],
[0.985, 0.5, 0.0, -0.0973],
[1.000, 0.5, 0.0, 0.0000]])
velocity = u.ProbeData(pts, "Velocity")
(ilen, jlen) = velocity.shape
norm=0.0
for i in range(ilen):
diff = pts[i][3] - velocity[i][1]
norm = norm + diff*diff
norm = math.sqrt(norm/ilen)
print "erturk_v_norm:", norm
return norm
开发者ID:fmilthaler,项目名称:DAKOTA-Fluidity-examples,代码行数:50,代码来源:driven_cavity.py
示例13: erturk_u
def erturk_u(NN):
#Erturk et al 2005. Table VI
filelist_not_sorted = glob.glob('driven_cavity-%d/*.vtu'%NN)
vtu_nos_not_sorted = [int(file.split('.vtu')[0].split('_')[-1]) for file in filelist_not_sorted]
filelist = [filelist_not_sorted[i] for i in numpy.argsort(vtu_nos_not_sorted)]
file = filelist[-1]
print file
try:
os.stat(file)
except:
print "No such file: %s" % file
sys.exit(1)
u=vtktools.vtu(file)
pts=vtktools.arr([[0.5, 0.000, 0.000, 0.0000],
[0.5, 0.000, 0.000, 0.0000],
[0.5, 0.020, 0.000, -0.0757],
[0.5, 0.040, 0.000, -0.1392],
[0.5, 0.060, 0.000, -0.1951],
[0.5, 0.080, 0.000, -0.2472],
[0.5, 0.100, 0.000, -0.2960],
[0.5, 0.120, 0.000, -0.3381],
[0.5, 0.140, 0.000, -0.3690],
[0.5, 0.160, 0.000, -0.3854],
[0.5, 0.180, 0.000, -0.3869],
[0.5, 0.200, 0.000, -0.3756],
[0.5, 0.500, 0.000, -0.0620],
[0.5, 0.900, 0.000, 0.3838],
[0.5, 0.910, 0.000, 0.3913],
[0.5, 0.920, 0.000, 0.3993],
[0.5, 0.930, 0.000, 0.4101],
[0.5, 0.940, 0.000, 0.4276],
[0.5, 0.950, 0.000, 0.4582],
[0.5, 0.960, 0.000, 0.5102],
[0.5, 0.970, 0.000, 0.5917],
[0.5, 0.980, 0.000, 0.7065],
[0.5, 0.990, 0.000, 0.8486],
[0.5, 1.000, 0.000, 1.0000]])
velocity = u.ProbeData(pts, "Velocity")
(ilen, jlen) = velocity.shape
norm=0.0
for i in range(ilen):
diff = pts[i][3] - velocity[i][0]
norm = norm + diff*diff
norm = math.sqrt(norm/ilen)
print "erturk_u_norm:", norm
return norm
开发者ID:fmilthaler,项目名称:DAKOTA-Fluidity-examples,代码行数:50,代码来源:driven_cavity.py
示例14: getElementMeshDensity
def getElementMeshDensity(file):
v = vtktools.vtu(file)
l = [0.0] * v.ugrid.GetNumberOfPoints()
a = vtktools.arr(l)
c = v.ugrid.GetCell(1)
for i in range(v.ugrid.GetNumberOfPoints()):
eles = v.GetPointCells(i)
sum = 0.0
for ele in eles:
points = v.ugrid.GetCell(ele).GetPoints().GetData()
sum = sum + c.ComputeVolume(points.GetTuple3(1), points.GetTuple3(2),
points.GetTuple3(3), points.GetTuple3(4))
a[i] = sum / len(eles)
return a
开发者ID:FluidityProject,项目名称:multifluids,代码行数:15,代码来源:fluidity_tools.py
示例15: calc_mld
def calc_mld(files,mld_depths):
for file in files:
try:
os.stat(file)
except:
print "No such file: %s" % file
sys.exit(1)
num = int(file.split(".vtu")[0].split('_')[-1])
u=vtktools.vtu(file)
pos = u.GetLocations()
time = u.GetScalarField('Time')
tt = time[0]
# grab the data e need from the VTUs and shove in an array
den = u.GetScalarField('Density')
xyz_data = []
for i in range(0,len(den)):
if (x0-0.1 < pos[i,0] < x0+0.1 and y0-0.1 < pos[i,1] < y0+0.1):
xyz_data.append((pos[i,0],pos[i,1],-pos[i,2]+z0,1000*den[i]))
# sorted the array based on depth
xyz_data = vtktools.arr(xyz_data)
III = argsort(xyz_data[:,2])
xyz_data_sorted = xyz_data[III,:]
# Surface values
sden = xyz_data_sorted[0,3]
# grab any values where the UML condition is met for temperature, density and TKE
uml_den = ((xyz_data_sorted[:,3]) <= (sden+den0)).nonzero()
# ...on density
if( (size(uml_den) > 0 ) ):
LL = uml_den[-1][-1]
zz = xyz_data_sorted[:,2]
if (LL+1 < size(zz)):
zza = zz[LL+1]
kea = xyz_data_sorted[LL+1,3]
else:
zza = zz[LL]
kea = xyz_data_sorted[LL,3]
zzb = zz[LL]
keb = xyz_data_sorted[LL,3]
tt = tt/(24*60*60)
time = start_datetime + timedelta(days=tt)
key = '%04d/%02d/%02d' % (time.year, time.month, time.day)
mld_depths[key] = (zza-(zzb-zza)*(((sden+den0)-kea)/(kea-keb)))
开发者ID:FluidityProject,项目名称:longtests,代码行数:48,代码来源:estimate_error.py
示例16: botella_v
def botella_v(NN):
#Botella and Peyret (1998) Table 10.
filelist_not_sorted = glob.glob('driven_cavity-%d/*.vtu'%NN)
vtu_nos_not_sorted = [int(file.split('.vtu')[0].split('_')[-1]) for file in filelist_not_sorted]
filelist = [filelist_not_sorted[i] for i in numpy.argsort(vtu_nos_not_sorted)]
file = filelist[-1]
print file
try:
os.stat(file)
except:
print "No such file: %s" % file
sys.exit(1)
u=vtktools.vtu(file)
pts=vtktools.arr([
[1.0000, 0.5, 0.0, 0.0000000],
[0.9688, 0.5, 0.0, -0.2279225],
[0.9609, 0.5, 0.0, -0.2936869],
[0.9531, 0.5, 0.0, -0.3553213],
[0.9453, 0.5, 0.0, -0.4103754],
[0.9063, 0.5, 0.0, -0.5264392],
[0.8594, 0.5, 0.0, -0.4264545],
[0.8047, 0.5, 0.0, -0.3202137],
[0.5000, 0.5, 0.0, 0.0257995],
[0.2344, 0.5, 0.0, 0.3253592],
[0.2266, 0.5, 0.0, 0.3339924],
[0.1563, 0.5, 0.0, 0.3769189],
[0.0938, 0.5, 0.0, 0.3330442],
[0.0781, 0.5, 0.0, 0.3099097],
[0.0703, 0.5, 0.0, 0.2962703],
[0.0625, 0.5, 0.0, 0.2807056],
[0.0000, 0.5, 0.0, 0.0000000]])
velocity = u.ProbeData(pts, "Velocity")
(ilen, jlen) = velocity.shape
norm=0.0
for i in range(ilen):
diff = pts[i][3] - velocity[i][1]
norm = norm + diff*diff
norm = math.sqrt(norm/ilen)
print "botella_v_norm:", norm
return norm
开发者ID:fmilthaler,项目名称:DAKOTA-Fluidity-examples,代码行数:45,代码来源:driven_cavity.py
示例17: botella_u
def botella_u(NN):
#Botella and Peyret (1998) Table 9. NB.our velocity at the lid is reverse theirs therefore minus signs in u below
filelist_not_sorted = glob.glob('driven_cavity-%d/*.vtu'%NN)
vtu_nos_not_sorted = [int(file.split('.vtu')[0].split('_')[-1]) for file in filelist_not_sorted]
filelist = [filelist_not_sorted[i] for i in numpy.argsort(vtu_nos_not_sorted)]
file = filelist[-1]
print file
try:
os.stat(file)
except:
print "No such file: %s" % file
sys.exit(1)
u=vtktools.vtu(file)
pts=vtktools.arr([
[0.5, 0.0000, 0.0, 0.0000000],
[0.5, 0.0547, 0.0, -0.1812881],
[0.5, 0.0625, 0.0, -0.2023300],
[0.5, 0.0703, 0.0, -0.2228955],
[0.5, 0.1016, 0.0, -0.3004561],
[0.5, 0.1719, 0.0, -0.3885691],
[0.5, 0.2813, 0.0, -0.2803696],
[0.5, 0.4531, 0.0, -0.1081999],
[0.5, 0.5000, 0.0, -0.0620561],
[0.5, 0.6172, 0.0, 0.0570178],
[0.5, 0.7344, 0.0, 0.1886747],
[0.5, 0.8516, 0.0, 0.3372212],
[0.5, 0.9531, 0.0, 0.4723329],
[0.5, 0.9609, 0.0, 0.5169277],
[0.5, 0.9688, 0.0, 0.5808359],
[0.5, 0.9766, 0.0, 0.6644227],
[0.5, 1.0000, 0.0, 1.0000000]])
velocity = u.ProbeData(pts, "Velocity")
(ilen, jlen) = velocity.shape
norm=0.0
for i in range(ilen):
diff = pts[i][3] - velocity[i][0]
norm = norm + diff*diff
norm = math.sqrt(norm/ilen)
print "botella_u_norm:", norm
return norm
开发者ID:fmilthaler,项目名称:DAKOTA-Fluidity-examples,代码行数:44,代码来源:driven_cavity.py
示例18: csv_reader
def csv_reader(filename, coords, t):
import sys
import vtktools
vtu=vtktools.vtu(filename[:-10]+'_'+str(t)+'.pvtu')
vtu.ApplyProjection('x', 'y', '0') # Set the third component to zero.
#Xlist = arange(0.0,4.001,0.01)# x co-ordinates of the desired array shape
#Ylist = arange(0.0,2.001,0.01)# y co-ordinates of the desired array shape
#[X,Y] = meshgrid(Xlist,Ylist)
#Z = 0.0*X # This is 2d so z is an array of zeros.
#X = reshape(X,(size(X),))
#Y = reshape(Y,(size(Y),))
#Z = reshape(Z,(size(Z),))
#zip(X,Y,Z)
#pts = zip(X,Y,Z)
print "coords: ", coords
pts = vtktools.arr([coords])
# create arrays of velocity and temperature values at the desired points
fs = vtu.ProbeData(pts, 'FreeSurface')
return fs[0]
开发者ID:FluidityProject,项目名称:longtests,代码行数:19,代码来源:plotfs_detec.py
示例19: find_sub_arc_isotherm_depth
def find_sub_arc_isotherm_depth(u,temp,a_t_dist):#Take in vtu, temp, arc-trench distance, return isotherm depth
import vtktools
import numpy as np
import matplotlib.pyplot as plt
from scipy.interpolate import interp1d
max_x=301000#maximum x distance from trench to be considered
wedge_pts=[]
X=np.array([i for i in np.arange(0,max_x,1000)])
Y=np.array([i for i in np.arange(0,-201000,-1000)])
for i in np.arange(0,max_x,1000):
for j in np.arange(0,-201000,-1000):
wedge_pts.append([i,j,0.0])
dom=vtktools.arr(np.array(wedge_pts))
temp_struct=u.ProbeData(dom,'Temperature')
CS=plt.contour(X,Y,np.reshape(temp_struct,(301,201)).T,[temp],colors="w",linewidth=200)
plt.clf()
x=[]
y=[]
for i in range(2):
p=CS.collections[0].get_paths()[i]
v=p.vertices
x.extend(v[:,0])
y.extend(v[:,1])
x_new=[]
y_new=[]
for i in range(len(y)):
if y[i] >-100000:
x_new.append(x[i])
y_new.append(y[i])
f=interp1d(x_new,y_new)
return f(a_t_dist)
开发者ID:ap4909,项目名称:geochemistry_data,代码行数:38,代码来源:find_sub_arc_isotherm_depth.py
示例20: range
timeee = u.GetScalarField('Time')
Time = timeee[0]
temp = u.GetScalarField("Temperature")
vert_diff = u.GetScalarField("GLSVerticalDiffusivity")
vert_visc = u.GetScalarField("GLSVerticalViscosity")
uvw = u.GetVectorField("Velocity")
kk = u.GetScalarField('GLSTurbulentKineticEnergy')
pos = u.GetLocations()
xyzkk = []
for i in range(0,len(kk)):
if( abs(pos[i,0] - x0) < 0.1 ):
xyzkk.append((pos[i,0],-pos[i,1],pos[i,2],kk[i],temp[i],uvw[i,0],vert_diff[i],vert_visc[i]))
xyzkkarr = vtktools.arr(xyzkk)
III = argsort(xyzkkarr[:,1])
xyzkkarrsort = xyzkkarr[III,:]
zzz = -xyzkkarrsort[:,1]
kkk = xyzkkarrsort[:,3]
ttt = xyzkkarrsort[:,4]
uuu = xyzkkarrsort[:,5]
diff = xyzkkarrsort[:,6]
visc = xyzkkarrsort[:,7]
fig = figure()
开发者ID:FluidityProject,项目名称:fluidity,代码行数:30,代码来源:line_plot.py
注:本文中的vtktools.arr函数示例由纯净天空整理自Github/MSDocs等源码及文档管理平台,相关代码片段筛选自各路编程大神贡献的开源项目,源码版权归原作者所有,传播和使用请参考对应项目的License;未经允许,请勿转载。 |
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