def determineRotation():
if 'rotated' in os.getcwd():
if 'stillwater' in os.getcwd():
angle = np.pi/18
tx=0.5
tz = -0.5
else:
a = pproc.determineAmplitude()
angle = np.pi/18 #10 degrees rotation of the domain
tx=0.0
tz = 4.22
return angle,tx,tz
else:
return 0,0,0
def initialize(a=None, solitonPosition=15):
print 'Initialization of a solitary wave from numerical data'
sys.stdout.flush()
solver = pproc.determineSolver()
a = a or pproc.determineAmplitude()
refDir = os.path.join(referenceDirectoryMain,str(a))
if not os.path.exists(refDir):
print 'No data for given amplitude found. Amplitude provided:',a,', available data:'
for d in sorted(glob.glob(os.path.join(refDir,'../0.*'))):
print d
sys.exit()
surf = np.loadtxt(os.path.join(refDir,'surf'))
surf[:,0] = surf[:,0] + solitonPosition
surf = np.vstack((np.array([-200,0.]),surf,np.array([200,0]))) #if the left side is inside the domain, vofOfManyPolygons has problems
np.savetxt('interface.ini',surf,fmt='%10.6f')
if solver == 'Gerris':
initializeGerris(refDir)
elif solver == 'OpenFOAM':
initializeOpenFOAM(refDir)
elif solver == 'Truchas':
initializeTruchas(refDir)
elif solver == 'Thetis':
initializeThetis(refDir)
def plotCrossSections(path, time=None, a=None, solver=None, x_c=25, bw=0, suffix='', difference=False):
"""
Plots the velocity profiles along vertical crossections of a solitary wave, for a single time step.
In previous versions multiple timesteps were supported, but is not any more.
:param difference: Take a difference between the reference solution and numerical results
:type difference: bool
"""
solver = solver or postprocess.determineSolver(path)
a = a or postprocess.determineAmplitude(path)
path=os.path.abspath(path)
dirs = glob.glob(path + '/case[1-4]/*postprocessed.dat') + glob.glob(path + '/*-[1-4]/*postprocessed.dat')
dirs = [os.path.split(dir)[0] for dir in dirs]
dirs.sort()
if not (dirs):
print 'Empty directory:', path
return 1
else:
print dirs
#correct time:
dt = postprocess.findDt(path)
time_step = int(round(time/dt))
time = time_step*dt
ref_line, u_ref = get_reference(a, time, x_c)
y_ref = ref_line[:, 1]
ux_ref = u_ref[:, 0]
ux_num_list, sample_line_z_list = [], []
for path in dirs:
vtk_file = postprocess.globFiles(path, ext='.vtk', verbose=False)[time_step]
if difference:
p1 = [x_c, np.min(y_ref)]
p2 = [x_c, np.max(y_ref)]
line, vel = sample_vtk(vtk_file, p1=p1, p2=p2, N_points=len(y_ref))
vel[:, 0] = vel[:, 0] - ux_ref
else:
line, vel = sample_vtk(vtk_file, x_c=x_c)
ux_num_list.append(vel[:, 0]) #x component
sample_line_z_list.append(line[:, 2]) #vertical component
print "Plotting..."
gravity = 'sourceGrav' if 'sourceGrav' in path else ''
results = ['VelCross', "A0{0:g}".format(a*10), solver, gravity, suffix]
results = [p for p in results if p] #remove empty strings
results = '_'.join(results)
xlim = {0.1: [-0.03, 0.45], 0.3: [-0.3, 1.3]}
plt.clf()
fig = plt.figure()
fig.subplots_adjust(0.15, 0.15, 0.95, None)
#plt.title('Propagation of a {2:.1f} soliton, t={0:.2f} s, $\Delta x$={1:.2f}m, {3}'.format(t, x_c-15, a, solver))
ls = ['-.', '--', '-']
for j in range(len(ux_num_list)):
case = dirs[j][-1:]
u = ux_num_list[j]
sample_line_z = sample_line_z_list[j]
if bw:
plt.plot(u, sample_line_z, label='Resolution ' + case, ls=ls[j], color='k')
else:
plt.plot(u, sample_line_z, label='Resolution ' + case, ls=ls[j])
if not difference:
plt.plot(ux_ref, y_ref, label='Reference', color='k', ls='-', lw=2)
plt.legend(loc='best')
plt.ylabel('z $[m]$')
plt.xlabel('Velocity $[\\frac{m}{s}]$')
plt.ylim(-1, np.max(sample_line_z))
plt.xlim(xlim[a])
if bw:
results = results+'_bw'
plt.savefig(results+'.png'.format(time))
plt.savefig(results+'.pdf'.format(time))
def plotCrossSections(path,
time=None,
a=None,
solver=None,
x_c=25,
bw=0,
suffix='',
difference=False):
"""
Plots the velocity profiles along vertical crossections of a solitary wave, for a single time step.
In previous versions multiple timesteps were supported, but is not any more.
:param difference: Take a difference between the reference solution and numerical results
:type difference: bool
"""
solver = solver or postprocess.determineSolver(path)
a = a or postprocess.determineAmplitude(path)
path = os.path.abspath(path)
dirs = glob.glob(path + '/case[1-4]/*postprocessed.dat') + glob.glob(
path + '/*-[1-4]/*postprocessed.dat')
dirs = [os.path.split(dir)[0] for dir in dirs]
dirs.sort()
if not (dirs):
print 'Empty directory:', path
return 1
else:
print dirs
#correct time:
dt = postprocess.findDt(path)
time_step = int(round(time / dt))
time = time_step * dt
ref_line, u_ref = get_reference(a, time, x_c)
y_ref = ref_line[:, 1]
ux_ref = u_ref[:, 0]
ux_num_list, sample_line_z_list = [], []
for path in dirs:
vtk_file = postprocess.globFiles(path, ext='.vtk',
verbose=False)[time_step]
if difference:
p1 = [x_c, np.min(y_ref)]
p2 = [x_c, np.max(y_ref)]
line, vel = sample_vtk(vtk_file, p1=p1, p2=p2, N_points=len(y_ref))
vel[:, 0] = vel[:, 0] - ux_ref
else:
line, vel = sample_vtk(vtk_file, x_c=x_c)
ux_num_list.append(vel[:, 0]) #x component
sample_line_z_list.append(line[:, 2]) #vertical component
print "Plotting..."
gravity = 'sourceGrav' if 'sourceGrav' in path else ''
results = ['VelCross', "A0{0:g}".format(a * 10), solver, gravity, suffix]
results = [p for p in results if p] #remove empty strings
results = '_'.join(results)
xlim = {0.1: [-0.03, 0.45], 0.3: [-0.3, 1.3]}
plt.clf()
fig = plt.figure()
fig.subplots_adjust(0.15, 0.15, 0.95, None)
#plt.title('Propagation of a {2:.1f} soliton, t={0:.2f} s, $\Delta x$={1:.2f}m, {3}'.format(t, x_c-15, a, solver))
ls = ['-.', '--', '-']
for j in range(len(ux_num_list)):
case = dirs[j][-1:]
u = ux_num_list[j]
sample_line_z = sample_line_z_list[j]
if bw:
plt.plot(u,
sample_line_z,
label='Resolution ' + case,
ls=ls[j],
color='k')
else:
plt.plot(u, sample_line_z, label='Resolution ' + case, ls=ls[j])