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Merge pull request #207 from ananyo-work/gas-dynamics-fixes
Gas dynamics fixes
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"""Acoustic wave diffusion in 2-d (2 mins) | ||
Two Dimensional constant pressure accuracy test | ||
particles should simply advect in a periodic domain | ||
""" | ||
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# NumPy and standard library imports | ||
import numpy | ||
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from pysph.base.nnps import DomainManager | ||
from pysph.base.utils import get_particle_array as gpa | ||
from pysph.solver.application import Application | ||
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from pysph.sph.scheme import GasDScheme, ADKEScheme, GSPHScheme, SchemeChooser | ||
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# PySPH tools | ||
from pysph.tools import uniform_distribution as ud | ||
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# Numerical constants | ||
dim = 2 | ||
gamma = 1.4 | ||
gamma1 = gamma - 1.0 | ||
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# solution parameters | ||
dt = 5e-3 | ||
tf = 1. | ||
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# domain size | ||
xmin = 0. | ||
xmax = 1. | ||
ymin = 0. | ||
ymax = 1. | ||
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# scheme constants | ||
alpha1 = 1.0 | ||
alpha2 = 0.1 | ||
beta = 2.0 | ||
kernel_factor = 1.5 | ||
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class AccuracyTest2D(Application): | ||
def initialize(self): | ||
self.xmin = xmin | ||
self.xmax = xmax | ||
self.ymin = ymin | ||
self.ymax = ymax | ||
self.ny = 100 | ||
self.nx = self.ny | ||
self.dx = (self.xmax - self.xmin) / (self.nx) | ||
self.hdx = 2. | ||
self.p = 1. | ||
self.u = 1 | ||
self.v = -1 | ||
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def create_domain(self): | ||
return DomainManager( | ||
xmin=xmin, xmax=xmax, ymin=ymin, ymax=ymax, | ||
periodic_in_x=True, periodic_in_y=True) | ||
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def create_particles(self): | ||
global dx | ||
data = ud.uniform_distribution_cubic2D( | ||
self.dx, xmin, xmax, ymin, ymax | ||
) | ||
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x = data[0].ravel() | ||
y = data[1].ravel() | ||
dx = data[2] | ||
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volume = dx * dx | ||
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rho = 1 + 0.2 * numpy.sin( | ||
numpy.pi * (x + y) | ||
) | ||
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p = numpy.ones_like(x) * self.p | ||
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# const h and mass | ||
h = numpy.ones_like(x) * self.hdx * dx | ||
m = numpy.ones_like(x) * volume * rho | ||
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# u = 1 | ||
u = numpy.ones_like(x) * self.u | ||
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# v = -1 | ||
v = numpy.ones_like(x) * self.v | ||
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# thermal energy from the ideal gas EOS | ||
e = p/(gamma1*rho) | ||
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fluid = gpa(name='fluid', x=x, y=y, rho=rho, p=p, e=e, h=h, m=m, | ||
h0=h.copy(), u=u, v=v) | ||
self.scheme.setup_properties([fluid]) | ||
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print("2D Accuracy Test with %d particles" | ||
% (fluid.get_number_of_particles())) | ||
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return [fluid, ] | ||
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def create_scheme(self): | ||
self.dt = dt | ||
self.tf = tf | ||
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adke = ADKEScheme( | ||
fluids=['fluid'], solids=[], dim=dim, gamma=gamma, | ||
alpha=1, beta=1, k=1.0, eps=0.8, g1=0.5, g2=0.5) | ||
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mpm = GasDScheme( | ||
fluids=['fluid'], solids=[], dim=dim, gamma=gamma, | ||
kernel_factor=kernel_factor, alpha1=alpha1, alpha2=alpha2, | ||
beta=beta | ||
) | ||
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gsph = GSPHScheme( | ||
fluids=['fluid'], solids=[], dim=dim, gamma=gamma, | ||
kernel_factor=1., | ||
g1=0., g2=0., rsolver=2, interpolation=0, monotonicity=0, | ||
interface_zero=True, hybrid=False, blend_alpha=5.0, | ||
niter=40, tol=1e-6 | ||
) | ||
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s = SchemeChooser( | ||
default='gsph', adke=adke, mpm=mpm, gsph=gsph | ||
) | ||
return s | ||
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def configure_scheme(self): | ||
s = self.scheme | ||
if self.options.scheme == 'mpm': | ||
s.configure(kernel_factor=kernel_factor) | ||
s.configure_solver(dt=self.dt, tf=self.tf, | ||
adaptive_timestep=True, pfreq=50) | ||
elif self.options.scheme == 'adke': | ||
s.configure_solver(dt=self.dt, tf=self.tf, | ||
adaptive_timestep=False, pfreq=50) | ||
elif self.options.scheme == 'gsph': | ||
s.configure_solver(dt=self.dt, tf=self.tf, | ||
adaptive_timestep=False, pfreq=50) | ||
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def post_process(self): | ||
from pysph.solver.utils import load | ||
if len(self.output_files) < 1: | ||
return | ||
outfile = self.output_files[-1] | ||
data = load(outfile) | ||
pa = data['arrays']['fluid'] | ||
x_c = pa.x | ||
y_c = pa.y | ||
rho_c = pa.rho | ||
rho_e = 1 + 0.2 * numpy.sin( | ||
numpy.pi * (x_c + y_c) | ||
) | ||
num_particles = rho_c.size | ||
l1_norm = numpy.sum( | ||
numpy.abs(rho_c - rho_e) | ||
) / num_particles | ||
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print(l1_norm) | ||
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if __name__ == '__main__': | ||
app = AccuracyTest2D() | ||
app.run() | ||
app.post_process() |
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"""Diffusion of an acoustic wave in 1-d (30 secs) | ||
Propagation of acoustic wave | ||
particles have properties according | ||
to the following distribuion | ||
\rho = \rho_0 + \Delta\rho sin(kx) | ||
p = p_0 + c_0^2\Delta\rho sin(kx) | ||
u = c_0\rho_0^{-1}\Delta\rho sin(kx) | ||
with \Delta\rho = 1e-6 and k = 2\pi/\lambda | ||
where \lambda is the domain length. | ||
\rho_0 = \gamma = 1.4 and p_0 = 1.0 | ||
""" | ||
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# standard library and numpy imports | ||
import numpy | ||
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# pysph imports | ||
from pysph.base.utils import get_particle_array as gpa | ||
from pysph.base.nnps import DomainManager | ||
from pysph.solver.application import Application | ||
from pysph.sph.scheme import \ | ||
GSPHScheme, ADKEScheme, GasDScheme, SchemeChooser | ||
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class AcousticWave(Application): | ||
def initialize(self): | ||
self.xmin = 0. | ||
self.xmax = 1. | ||
self.gamma = 1.4 | ||
self.rho_0 = self.gamma | ||
self.p_0 = 1. | ||
self.c_0 = 1. | ||
self.delta_rho = 1e-6 | ||
self.n_particles = 400 | ||
self.domain_length = self.xmax - self.xmin | ||
self.dx = self.domain_length / (self.n_particles) | ||
self.k = -2 * numpy.pi / self.domain_length | ||
self.hdx = 1. | ||
self.dt = 1e-3 | ||
self.tf = 10 | ||
self.dim = 1 | ||
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def create_domain(self): | ||
return DomainManager( | ||
xmin=0, xmax=1, periodic_in_x=True | ||
) | ||
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def create_particles(self): | ||
x = numpy.arange( | ||
self.xmin + self.dx*0.5, self.xmax, self.dx | ||
) | ||
rho = self.rho_0 + self.delta_rho *\ | ||
numpy.sin(self.k * x) | ||
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p = self.p_0 + self.c_0**2 *\ | ||
self.delta_rho * numpy.sin(self.k * x) | ||
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u = self.c_0 * self.delta_rho * numpy.sin(self.k * x) /\ | ||
self.rho_0 | ||
cs = numpy.sqrt( | ||
self.gamma * p / rho | ||
) | ||
h = numpy.ones_like(x) * self.dx * self.hdx | ||
m = numpy.ones_like(x) * self.dx * rho | ||
e = p / ((self.gamma - 1) * rho) | ||
fluid = gpa( | ||
name='fluid', x=x, p=p, rho=rho, u=u, h=h, m=m, e=e, cs=cs | ||
) | ||
self.scheme.setup_properties([fluid]) | ||
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return [fluid, ] | ||
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def create_scheme(self): | ||
gsph = GSPHScheme( | ||
fluids=['fluid'], solids=[], dim=self.dim, | ||
gamma=self.gamma, kernel_factor=1.0, | ||
g1=0., g2=0., rsolver=7, interpolation=1, monotonicity=1, | ||
interface_zero=True, hybrid=False, blend_alpha=5.0, | ||
niter=40, tol=1e-6 | ||
) | ||
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mpm = GasDScheme( | ||
fluids=['fluid'], solids=[], dim=self.dim, gamma=self.gamma, | ||
kernel_factor=1.2, alpha1=0, alpha2=0, | ||
beta=2.0, update_alpha1=False, update_alpha2=False | ||
) | ||
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s = SchemeChooser( | ||
default='gsph', gsph=gsph, mpm=mpm | ||
) | ||
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return s | ||
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def configure_scheme(self): | ||
s = self.scheme | ||
if self.options.scheme == 'gsph': | ||
s.configure_solver( | ||
dt=self.dt, tf=self.tf, | ||
adaptive_timestep=True, pfreq=50 | ||
) | ||
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if self.options.scheme == 'mpm': | ||
s.configure(kernel_factor=1.2) | ||
s.configure_solver(dt=self.dt, tf=self.tf, | ||
adaptive_timestep=True, pfreq=50) | ||
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def post_process(self): | ||
from pysph.solver.utils import load | ||
if len(self.output_files) < 1: | ||
return | ||
outfile = self.output_files[-1] | ||
data = load(outfile) | ||
pa = data['arrays']['fluid'] | ||
x_c = pa.x | ||
u = self.c_0 * self.delta_rho * numpy.sin(self.k * x_c) /\ | ||
self.rho_0 | ||
u_c = pa.u | ||
l_inf = numpy.max( | ||
numpy.abs(u_c - u) | ||
) | ||
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print("L_inf norm for the problem: %s" % (l_inf)) | ||
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if __name__ == "__main__": | ||
app = AcousticWave() | ||
app.run() | ||
app.post_process() |
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@@ -0,0 +1,99 @@ | ||
"""Cheng and Shu's 1d acoustic wave propagation in 1d (1 min) | ||
particles have properties according | ||
to the following distribuion | ||
\rho = \rho_0 + \Delta\rho sin(kx) | ||
p = 1.0 | ||
u = 1 + 0.1sin(kx) | ||
with \Delta\rho = 1 and k = 2\pi/\lambda | ||
where \lambda is the domain length. | ||
\rho_0 = 2, \gamma = 1.4 and p_0 = 1.0 | ||
""" | ||
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# standard library and numpy imports | ||
import numpy | ||
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# pysph imports | ||
from pysph.base.utils import get_particle_array as gpa | ||
from pysph.base.nnps import DomainManager | ||
from pysph.solver.application import Application | ||
from pysph.sph.scheme import \ | ||
GSPHScheme, ADKEScheme, GasDScheme, SchemeChooser | ||
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class ChengShu(Application): | ||
def initialize(self): | ||
self.xmin = 0. | ||
self.xmax = 1. | ||
self.gamma = 1.4 | ||
self.p_0 = 1. | ||
self.c_0 = 1. | ||
self.delta_rho = 1 | ||
self.n_particles = 1000 | ||
self.domain_length = self.xmax - self.xmin | ||
self.dx = self.domain_length / (self.n_particles - 1) | ||
self.k = 2 * numpy.pi / self.domain_length | ||
self.hdx = 2. | ||
self.dt = 1e-4 | ||
self.tf = 1.0 | ||
self.dim = 1 | ||
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def create_domain(self): | ||
return DomainManager( | ||
xmin=self.xmin, xmax=self.xmax, periodic_in_x=True | ||
) | ||
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def create_particles(self): | ||
x = numpy.linspace( | ||
self.xmin, self.xmax, self.n_particles | ||
) | ||
rho = 2 + numpy.sin(2 * numpy.pi * x)*self.delta_rho | ||
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p = numpy.ones_like(x) | ||
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u = 1 + 0.1 * numpy.sin(2 * numpy.pi * x) | ||
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cs = numpy.sqrt( | ||
self.gamma * p / rho | ||
) | ||
h = numpy.ones_like(x) * self.dx * self.hdx | ||
m = numpy.ones_like(x) * self.dx * rho | ||
e = p / ((self.gamma - 1) * rho) | ||
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fluid = gpa( | ||
name='fluid', x=x, p=p, rho=rho, u=u, h=h, m=m, e=e, cs=cs | ||
) | ||
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self.scheme.setup_properties([fluid]) | ||
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return [fluid, ] | ||
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def create_scheme(self): | ||
gsph = GSPHScheme( | ||
fluids=['fluid'], solids=[], dim=self.dim, | ||
gamma=self.gamma, kernel_factor=1., | ||
g1=0., g2=0., rsolver=3, interpolation=1, monotonicity=1, | ||
interface_zero=True, hybrid=False, blend_alpha=5.0, | ||
niter=200, tol=1e-6 | ||
) | ||
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s = SchemeChooser( | ||
default='gsph', gsph=gsph | ||
) | ||
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return s | ||
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def configure_scheme(self): | ||
s = self.scheme | ||
if self.options.scheme == 'gsph': | ||
s.configure_solver( | ||
dt=self.dt, tf=self.tf, | ||
adaptive_timestep=False, pfreq=1000 | ||
) | ||
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if __name__ == "__main__": | ||
app = ChengShu() | ||
app.run() |
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