Source code for pysph.sph.iisph

"""The basic equations for the IISPH formulation of

    M. Ihmsen, J. Cornelis, B. Solenthaler, C. Horvath, M. Teschner, "Implicit
    Incompressible SPH," IEEE Transactions on Visualization and Computer
    Graphics, vol. 20, no. 3, pp. 426-435, March 2014.
    http://dx.doi.org/10.1109/TVCG.2013.105

"""

from numpy import sqrt, fabs
from compyle.api import declare
from pysph.base.particle_array import get_ghost_tag
from pysph.sph.equation import Equation
from pysph.sph.integrator_step import IntegratorStep
from pysph.base.reduce_array import serial_reduce_array, parallel_reduce_array
from pysph.sph.scheme import Scheme, add_bool_argument


GHOST_TAG = get_ghost_tag()


[docs]class IISPHStep(IntegratorStep): """A straightforward and simple integrator to be used for IISPH. """
[docs] def stage1(self, d_idx, d_x, d_y, d_z, d_u, d_v, d_w, d_uadv, d_vadv, d_wadv, d_au, d_av, d_aw, d_ax, d_ay, d_az, dt): d_u[d_idx] = d_uadv[d_idx] + dt * d_au[d_idx] d_v[d_idx] = d_vadv[d_idx] + dt * d_av[d_idx] d_w[d_idx] = d_wadv[d_idx] + dt * d_aw[d_idx] d_x[d_idx] += dt * d_u[d_idx] d_y[d_idx] += dt * d_v[d_idx] d_z[d_idx] += dt * d_w[d_idx]
[docs]class NumberDensity(Equation):
[docs] def initialize(self, d_idx, d_V): d_V[d_idx] = 0.0
[docs] def loop(self, d_idx, d_V, WIJ): d_V[d_idx] += WIJ
[docs]class SummationDensity(Equation):
[docs] def initialize(self, d_idx, d_rho): d_rho[d_idx] = 0.0
[docs] def loop(self, d_idx, d_rho, s_idx, s_m, WIJ): d_rho[d_idx] += s_m[s_idx]*WIJ
[docs]class SummationDensityBoundary(Equation): def __init__(self, dest, sources, rho0): self.rho0 = rho0 super(SummationDensityBoundary, self).__init__(dest, sources)
[docs] def loop(self, d_idx, d_rho, s_idx, s_V, WIJ): d_rho[d_idx] += self.rho0/s_V[s_idx]*WIJ
[docs]class NormalizedSummationDensity(Equation):
[docs] def initialize(self, d_idx, d_rho, d_rho_adv, d_rho0, d_V): d_rho0[d_idx] = d_rho[d_idx] d_rho[d_idx] = 0.0 d_rho_adv[d_idx] = 0.0 d_V[d_idx] = 0.0
[docs] def loop(self, d_idx, d_rho, d_rho_adv, d_V, s_idx, s_m, s_rho0, WIJ): tmp = s_m[s_idx]*WIJ d_rho[d_idx] += tmp d_rho_adv[d_idx] += tmp/s_rho0[s_idx] d_V[d_idx] += WIJ
[docs] def post_loop(self, d_idx, d_rho, d_rho_adv): d_rho[d_idx] /= d_rho_adv[d_idx]
[docs]class AdvectionAcceleration(Equation): def __init__(self, dest, sources, gx=0.0, gy=0.0, gz=0.0): self.gx = gx self.gy = gy self.gz = gz super(AdvectionAcceleration, self).__init__(dest, sources)
[docs] def initialize(self, d_idx, d_au, d_av, d_aw, d_uadv, d_vadv, d_wadv): d_au[d_idx] = self.gx d_av[d_idx] = self.gy d_aw[d_idx] = self.gz d_uadv[d_idx] = 0.0 d_vadv[d_idx] = 0.0 d_wadv[d_idx] = 0.0
[docs] def post_loop(self, d_idx, d_au, d_av, d_aw, d_uadv, d_vadv, d_wadv, d_u, d_v, d_w, dt=0.0): d_uadv[d_idx] = d_u[d_idx] + dt*d_au[d_idx] d_vadv[d_idx] = d_v[d_idx] + dt*d_av[d_idx] d_wadv[d_idx] = d_w[d_idx] + dt*d_aw[d_idx]
[docs]class ViscosityAcceleration(Equation): def __init__(self, dest, sources, nu): self.nu = nu super(ViscosityAcceleration, self).__init__(dest, sources)
[docs] def loop(self, d_idx, d_au, d_av, d_aw, s_idx, s_m, EPS, VIJ, XIJ, RHOIJ1, R2IJ, DWIJ): dwijdotxij = DWIJ[0]*XIJ[0] + DWIJ[1]*XIJ[1] + DWIJ[2]*XIJ[2] fac = 2.0*self.nu*s_m[s_idx]*RHOIJ1*dwijdotxij/(R2IJ + EPS) d_au[d_idx] += fac*VIJ[0] d_av[d_idx] += fac*VIJ[1] d_aw[d_idx] += fac*VIJ[2]
[docs]class ViscosityAccelerationBoundary(Equation): """The acceleration on the fluid due to a boundary. """ def __init__(self, dest, sources, rho0, nu): self.nu = nu self.rho0 = rho0 super(ViscosityAccelerationBoundary, self).__init__(dest, sources)
[docs] def loop(self, d_idx, d_au, d_av, d_aw, d_rho, s_idx, s_V, EPS, VIJ, XIJ, R2IJ, DWIJ): phi_b = self.rho0/(s_V[s_idx]*d_rho[d_idx]) dwijdotxij = DWIJ[0]*XIJ[0] + DWIJ[1]*XIJ[1] + DWIJ[2]*XIJ[2] fac = 2.0*self.nu*phi_b*dwijdotxij/(R2IJ + EPS) d_au[d_idx] += fac*VIJ[0] d_av[d_idx] += fac*VIJ[1] d_aw[d_idx] += fac*VIJ[2]
[docs]class ComputeDII(Equation):
[docs] def initialize(self, d_idx, d_dii0, d_dii1, d_dii2): d_dii0[d_idx] = 0.0 d_dii1[d_idx] = 0.0 d_dii2[d_idx] = 0.0
[docs] def loop(self, d_idx, d_rho, d_dii0, d_dii1, d_dii2, s_idx, s_m, DWIJ): rho_1 = 1.0/d_rho[d_idx] fac = -s_m[s_idx]*rho_1*rho_1 d_dii0[d_idx] += fac*DWIJ[0] d_dii1[d_idx] += fac*DWIJ[1] d_dii2[d_idx] += fac*DWIJ[2]
[docs]class ComputeDIIBoundary(Equation): def __init__(self, dest, sources, rho0): self.rho0 = rho0 super(ComputeDIIBoundary, self).__init__(dest, sources)
[docs] def loop(self, d_idx, d_dii0, d_dii1, d_dii2, d_rho, s_idx, s_m, s_V, DWIJ): rhoi1 = 1.0/d_rho[d_idx] fac = -rhoi1*rhoi1*self.rho0/s_V[s_idx] d_dii0[d_idx] += fac*DWIJ[0] d_dii1[d_idx] += fac*DWIJ[1] d_dii2[d_idx] += fac*DWIJ[2]
[docs]class ComputeRhoAdvection(Equation):
[docs] def initialize(self, d_idx, d_rho_adv, d_rho, d_p0, d_p, d_piter, d_aii): d_rho_adv[d_idx] = d_rho[d_idx] d_p0[d_idx] = d_p[d_idx] d_piter[d_idx] = 0.5*d_p[d_idx]
[docs] def loop(self, d_idx, d_rho, d_rho_adv, d_uadv, d_vadv, d_wadv, d_u, d_v, d_w, s_idx, s_m, s_uadv, s_vadv, s_wadv, DWIJ, dt=0.0): vijdotdwij = (d_uadv[d_idx] - s_uadv[s_idx])*DWIJ[0] + \ (d_vadv[d_idx] - s_vadv[s_idx])*DWIJ[1] + \ (d_wadv[d_idx] - s_wadv[s_idx])*DWIJ[2] d_rho_adv[d_idx] += dt*s_m[s_idx]*vijdotdwij
[docs]class ComputeRhoBoundary(Equation): def __init__(self, dest, sources, rho0): self.rho0 = rho0 super(ComputeRhoBoundary, self).__init__(dest, sources)
[docs] def loop(self, d_idx, d_rho, d_rho_adv, d_uadv, d_vadv, d_wadv, s_idx, s_u, s_v, s_w, s_V, WIJ, DWIJ, dt=0.0): phi_b = self.rho0/s_V[s_idx] vijdotdwij = (d_uadv[d_idx] - s_u[s_idx])*DWIJ[0] + \ (d_vadv[d_idx] - s_v[s_idx])*DWIJ[1] + \ (d_wadv[d_idx] - s_w[s_idx])*DWIJ[2] d_rho_adv[d_idx] += dt*phi_b*vijdotdwij
[docs]class ComputeAII(Equation):
[docs] def initialize(self, d_idx, d_aii): d_aii[d_idx] = 0.0
[docs] def loop(self, d_idx, d_aii, d_dii0, d_dii1, d_dii2, d_m, d_rho, s_idx, s_m, s_rho, DWIJ): rho1 = 1.0/d_rho[d_idx] fac = d_m[d_idx]*rho1*rho1 # The following is m_j (d_ii - d_ji) . DWIJ # DWIJ = -DWJI dijdotdwij = (d_dii0[d_idx] - fac*DWIJ[0])*DWIJ[0] + \ (d_dii1[d_idx] - fac*DWIJ[1])*DWIJ[1] + \ (d_dii2[d_idx] - fac*DWIJ[2])*DWIJ[2] d_aii[d_idx] += s_m[s_idx]*dijdotdwij
[docs]class ComputeAIIBoundary(Equation): """ This is important and not really discussed in the original IISPH paper. """ def __init__(self, dest, sources, rho0): self.rho0 = rho0 super(ComputeAIIBoundary, self).__init__(dest, sources)
[docs] def loop(self, d_idx, d_m, d_aii, d_dii0, d_dii1, d_dii2, d_rho, s_idx, s_m, s_V, DWIJ): phi_b = self.rho0/s_V[s_idx] rho1 = 1.0/d_rho[d_idx] fac = d_m[d_idx]*rho1*rho1 dijdotdwij = ((d_dii0[d_idx] - fac*DWIJ[0])*DWIJ[0] + (d_dii1[d_idx] - fac*DWIJ[1])*DWIJ[1] + (d_dii2[d_idx] - fac*DWIJ[2])*DWIJ[2]) d_aii[d_idx] += phi_b*dijdotdwij
[docs]class ComputeDIJPJ(Equation):
[docs] def initialize(self, d_idx, d_dijpj0, d_dijpj1, d_dijpj2): d_dijpj0[d_idx] = 0.0 d_dijpj1[d_idx] = 0.0 d_dijpj2[d_idx] = 0.0
[docs] def loop(self, d_idx, d_dijpj0, d_dijpj1, d_dijpj2, s_idx, s_m, s_rho, s_piter, DWIJ): rho1 = 1.0/s_rho[s_idx] fac = -s_m[s_idx]*rho1*rho1*s_piter[s_idx] d_dijpj0[d_idx] += fac*DWIJ[0] d_dijpj1[d_idx] += fac*DWIJ[1] d_dijpj2[d_idx] += fac*DWIJ[2]
[docs]class UpdateGhostProps(Equation): def __init__(self, dest, sources=None): super(UpdateGhostProps, self).__init__(dest, sources) # We do this to ensure that the ghost tag is indeed 2. # If not the initialize method will never work. assert GHOST_TAG == 2
[docs] def initialize(self, d_idx, d_tag, d_orig_idx, d_dijpj0, d_dijpj1, d_dijpj2, d_dii0, d_dii1, d_dii2, d_piter): idx = declare('int') if d_tag[d_idx] == 2: idx = d_orig_idx[d_idx] d_dijpj0[d_idx] = d_dijpj0[idx] d_dijpj1[d_idx] = d_dijpj1[idx] d_dijpj2[d_idx] = d_dijpj2[idx] d_dii0[d_idx] = d_dii0[idx] d_dii1[d_idx] = d_dii1[idx] d_dii2[d_idx] = d_dii2[idx] d_piter[d_idx] = d_piter[idx]
[docs]class PressureSolve(Equation): def __init__(self, dest, sources, rho0, omega=0.5, tolerance=1e-2, debug=False): self.rho0 = rho0 self.omega = omega self.compression = 0.0 self.debug = debug self.tolerance = tolerance super(PressureSolve, self).__init__(dest, sources)
[docs] def initialize(self, d_idx, d_p, d_compression): d_p[d_idx] = 0.0 d_compression[d_idx] = 0.0
[docs] def loop(self, d_idx, d_p, d_piter, d_rho, d_m, d_dijpj0, d_dijpj1, d_dijpj2, s_idx, s_m, s_dii0, s_dii1, s_dii2, s_piter, s_dijpj0, s_dijpj1, s_dijpj2, DWIJ): # Note that a good way to check this is to see that when # d_idx == s_idx the contribution is zero, as is expected. rho1 = 1.0/d_rho[d_idx] fac = d_m[d_idx]*rho1*rho1*d_piter[d_idx] djkpk0 = s_dijpj0[s_idx] - fac*DWIJ[0] djkpk1 = s_dijpj1[s_idx] - fac*DWIJ[1] djkpk2 = s_dijpj2[s_idx] - fac*DWIJ[2] tmp0 = d_dijpj0[d_idx] - s_dii0[s_idx]*s_piter[s_idx] - djkpk0 tmp1 = d_dijpj1[d_idx] - s_dii1[s_idx]*s_piter[s_idx] - djkpk1 tmp2 = d_dijpj2[d_idx] - s_dii2[s_idx]*s_piter[s_idx] - djkpk2 tmpdotdwij = tmp0*DWIJ[0] + tmp1*DWIJ[1] + tmp2*DWIJ[2] # This is corrected in the post_loop. d_p[d_idx] += s_m[s_idx]*tmpdotdwij
[docs] def post_loop(self, d_idx, d_piter, d_p0, d_p, d_aii, d_rho_adv, d_rho, d_compression, dt=0.0): dt2 = dt*dt # Recall that d_p now has \sum_{j\neq i} a_ij p_j tmp = self.rho0 - d_rho_adv[d_idx] - d_p[d_idx]*dt2 dnr = d_aii[d_idx]*dt2 if fabs(dnr) > 1e-9: # Clamp pressure to positive values. p = max((1.0 - self.omega)*d_piter[d_idx] + self.omega/dnr*tmp, 0.0) else: p = 0.0 if p != 0.0: d_compression[d_idx] = fabs(p*dnr - tmp) + self.rho0 else: d_compression[d_idx] = self.rho0 d_piter[d_idx] = p d_p[d_idx] = p
[docs] def reduce(self, dst, t, dt): dst.tmp_comp[0] = serial_reduce_array(dst.compression > 0.0, 'sum') dst.tmp_comp[1] = serial_reduce_array(dst.compression, 'sum') dst.tmp_comp[:] = parallel_reduce_array(dst.tmp_comp, 'sum') if dst.tmp_comp[0] > 0: avg_rho = dst.tmp_comp[1]/dst.tmp_comp[0] else: avg_rho = self.rho0 self.compression = fabs(avg_rho - self.rho0)/self.rho0
[docs] def converged(self): debug = self.debug compression = self.compression if compression > self.tolerance: if debug: print("Not converged:", compression) return -1.0 else: if debug: print("Converged:", compression) return 1.0
[docs]class PressureSolveBoundary(Equation): def __init__(self, dest, sources, rho0): self.rho0 = rho0 super(PressureSolveBoundary, self).__init__(dest, sources)
[docs] def loop(self, d_idx, d_p, d_rho, d_dijpj0, d_dijpj1, d_dijpj2, s_idx, s_V, DWIJ): phi_b = self.rho0/s_V[s_idx] dijdotwij = (d_dijpj0[d_idx]*DWIJ[0] + d_dijpj1[d_idx]*DWIJ[1] + d_dijpj2[d_idx]*DWIJ[2]) d_p[d_idx] += phi_b*dijdotwij
[docs]class UpdateGhostPressure(Equation):
[docs] def initialize(self, d_idx, d_tag, d_orig_idx, d_p, d_piter): idx = declare('int') if d_tag[d_idx] == 2: idx = d_orig_idx[d_idx] d_piter[d_idx] = d_piter[idx] d_p[d_idx] = d_p[idx]
[docs]class PressureForce(Equation):
[docs] def initialize(self, d_idx, d_au, d_av, d_aw): d_au[d_idx] = 0.0 d_av[d_idx] = 0.0 d_aw[d_idx] = 0.0
[docs] def loop(self, d_idx, d_rho, d_p, d_au, d_av, d_aw, s_idx, s_m, s_rho, s_p, DWIJ): rhoi1 = 1.0/d_rho[d_idx] rhoj1 = 1.0/s_rho[s_idx] fac = -s_m[s_idx]*(d_p[d_idx]*rhoi1*rhoi1 + s_p[s_idx]*rhoj1*rhoj1) d_au[d_idx] += fac*DWIJ[0] d_av[d_idx] += fac*DWIJ[1] d_aw[d_idx] += fac*DWIJ[2]
[docs] def post_loop(self, d_idx, d_au, d_av, d_aw, d_uadv, d_vadv, d_wadv, d_dt_cfl, d_dt_force): fac = d_au[d_idx]*d_au[d_idx] + d_av[d_idx]*d_av[d_idx] +\ d_aw[d_idx]*d_aw[d_idx] vmag = sqrt(d_uadv[d_idx]*d_uadv[d_idx] + d_vadv[d_idx]*d_vadv[d_idx] + d_wadv[d_idx]*d_wadv[d_idx]) d_dt_cfl[d_idx] = 2.0*vmag d_dt_force[d_idx] = 2.0*fac
[docs]class PressureForceBoundary(Equation): def __init__(self, dest, sources, rho0): self.rho0 = rho0 super(PressureForceBoundary, self).__init__(dest, sources)
[docs] def loop(self, d_idx, d_rho, d_au, d_av, d_aw, d_p, s_idx, s_V, DWIJ): rho1 = 1.0/d_rho[d_idx] fac = -d_p[d_idx]*rho1*rho1*self.rho0/s_V[s_idx] d_au[d_idx] += fac*DWIJ[0] d_av[d_idx] += fac*DWIJ[1] d_aw[d_idx] += fac*DWIJ[2]
[docs]class IISPHScheme(Scheme): def __init__(self, fluids, solids, dim, rho0, nu=0.0, gx=0.0, gy=0.0, gz=0.0, omega=0.5, tolerance=1e-2, debug=False, has_ghosts=False): '''The IISPH scheme Parameters ---------- fluids : list(str) List of names of fluid particle arrays. solids : list(str) List of names of solid particle arrays. dim: int Dimensionality of the problem. rho0 : float Density of fluid. nu : float Kinematic viscosity. gx, gy, gz : float Componenents of body acceleration (gravity, external forcing etc.) omega : float Relaxation parameter for relaxed-Jacobi iterations. tolerance: float Tolerance for the convergence of pressure iterations as a fraction. debug: bool Produce some debugging output on iterations. has_ghosts: bool The problem has ghost particles so add equations for those. ''' self.fluids = fluids self.solids = solids self.dim = dim self.rho0 = rho0 self.nu = nu self.gx = gx self.gy = gy self.gz = gz self.omega = omega self.tolerance = tolerance self.debug = debug self.has_ghosts = has_ghosts
[docs] def add_user_options(self, group): group.add_argument( '--omega', action="store", type=float, dest="omega", default=None, help="Relaxation parameter for Jacobi iterations." ) group.add_argument( '--tolerance', action='store', type=float, dest='tolerance', default=None, help='Tolerance for convergence of iterations as a fraction' ) add_bool_argument( group, 'iisph-debug', dest='debug', default=None, help="Produce some debugging output on convergence of iterations." )
[docs] def consume_user_options(self, options): vars = ['omega', 'tolerance', 'debug'] data = dict((var, self._smart_getattr(options, var)) for var in vars) self.configure(**data)
[docs] def configure_solver(self, kernel=None, integrator_cls=None, extra_steppers=None, **kw): """Configure the solver to be generated. This is to be called before `get_solver` is called. Parameters ---------- dim : int Number of dimensions. kernel : Kernel instance. Kernel to use, if none is passed a default one is used. integrator_cls : pysph.sph.integrator.Integrator Integrator class to use, use sensible default if none is passed. extra_steppers : dict Additional integration stepper instances as a dict. **kw : extra arguments Any additional keyword args are passed to the solver instance. """ from pysph.base.kernels import CubicSpline from pysph.sph.integrator import EulerIntegrator from pysph.solver.solver import Solver if kernel is None: kernel = CubicSpline(dim=self.dim) steppers = {} if extra_steppers is not None: steppers.update(extra_steppers) for fluid in self.fluids: if fluid not in steppers: steppers[fluid] = IISPHStep() cls = integrator_cls if integrator_cls is not None else EulerIntegrator integrator = cls(**steppers) self.solver = Solver( dim=self.dim, integrator=integrator, kernel=kernel, **kw )
[docs] def get_equations(self): from pysph.sph.equation import Group has_ghosts = self.has_ghosts equations = [] if self.solids: g1 = Group( equations=[NumberDensity(dest=x, sources=[x]) for x in self.solids] ) equations.append(g1) g2 = Group( equations=[SummationDensity(dest=x, sources=self.fluids) for x in self.fluids], real=False ) equations.append(g2) if self.solids: g3 = Group( equations=[ SummationDensityBoundary( dest=x, sources=self.solids, rho0=self.rho0 ) for x in self.fluids], real=False ) equations.append(g3) eq = [] for fluid in self.fluids: eq.extend([ AdvectionAcceleration( dest=fluid, sources=None, gx=self.gx, gy=self.gy, gz=self.gz ), ComputeDII(dest=fluid, sources=self.fluids) ]) if self.nu > 0.0: eq.append( ViscosityAcceleration( dest=fluid, sources=self.fluids, nu=self.nu ) ) if self.solids: if self.nu > 0.0: eq.append( ViscosityAccelerationBoundary( dest=fluid, sources=self.solids, nu=self.nu, rho0=self.rho0, ) ) eq.append( ComputeDIIBoundary(dest=fluid, sources=self.solids, rho0=self.rho0) ) g4 = Group(equations=eq, real=False) equations.append(g4) eq = [] for fluid in self.fluids: eq.extend([ ComputeRhoAdvection(dest=fluid, sources=self.fluids), ComputeAII(dest=fluid, sources=self.fluids), ]) if self.solids: eq.extend([ ComputeRhoBoundary(dest=fluid, sources=self.solids, rho0=self.rho0), ComputeAIIBoundary(dest=fluid, sources=self.solids, rho0=self.rho0), ]) g5 = Group(equations=eq) equations.append(g5) sg1 = Group( equations=[ ComputeDIJPJ(dest=x, sources=self.fluids) for x in self.fluids ] ) eq = [] for fluid in self.fluids: eq.append( PressureSolve(dest=fluid, sources=self.fluids, rho0=self.rho0, tolerance=self.tolerance, debug=self.debug) ) if self.solids: eq.append( PressureSolveBoundary( dest=fluid, sources=self.solids, rho0=self.rho0, ) ) sg2 = Group(equations=eq) if has_ghosts: ghost1 = Group( equations=[UpdateGhostProps(dest=x, sources=None) for x in self.fluids], real=False ) ghost2 = Group( equations=[UpdateGhostPressure(dest=x, sources=None) for x in self.fluids], real=False ) solver_eqs = [sg1, ghost1, sg2, ghost2] else: solver_eqs = [sg1, sg2] g6 = Group( equations=solver_eqs, iterate=True, max_iterations=30, min_iterations=2 ) equations.append(g6) eq = [] for fluid in self.fluids: eq.append( PressureForce(dest=fluid, sources=self.fluids) ) if self.solids: eq.append( PressureForceBoundary( dest=fluid, sources=self.solids, rho0=self.rho0 ) ) g7 = Group(equations=eq) equations.append(g7) return equations
[docs] def setup_properties(self, particles, clean=True): """Setup the particle arrays so they have the right set of properties for this scheme. Parameters ---------- particles : list List of particle arrays. clean : bool If True, removes any unnecessary properties. """ from pysph.base.utils import get_particle_array_iisph dummy = get_particle_array_iisph() props = set(dummy.properties.keys()) for pa in particles: self._ensure_properties(pa, props, clean) for c, v in dummy.constants.items(): if c not in pa.constants: pa.add_constant(c, v) pa.set_output_arrays(dummy.output_property_arrays) if self.has_ghosts: particle_arrays = dict([(p.name, p) for p in particles]) for fluid in self.fluids: pa = particle_arrays[fluid] pa.add_property('orig_idx', type='int')