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import os
import warp as wp
import numpy as np
from warp.sim import Model, State
import warp.sim.render
import warp.fem as fem
from warp.fem import integrand, lookup, normal, grad, at_node, div
from warp.fem import Field, Sample, Domain
from warp.sparse import bsr_mv, bsr_copy, bsr_mm, bsr_transposed, bsr_zeros, BsrMatrix
try:
from .bsr_utils import bsr_cg
except ImportError:
from bsr_utils import bsr_cg
@integrand
def integrate_fraction(s: Sample, phi: Field):
return phi(s)
@integrand
def integrate_velocity(
s: Sample,
domain: Domain,
u: Field,
velocities: wp.array(dtype=wp.vec3),
velocity_gradients: wp.array(dtype=wp.mat33),
dt: float,
gravity: wp.vec3,
):
"""Transfer particle velocities to grid"""
node_offset = domain(at_node(u, s)) - domain(s)
vel_apic = velocities[s.qp_index] + velocity_gradients[s.qp_index] * node_offset
vel_adv = vel_apic + dt * gravity
return wp.dot(u(s), vel_adv)
@integrand
def update_particles(
s: Sample,
domain: Domain,
grid_vel: Field,
dt: float,
pos: wp.array(dtype=wp.vec3),
pos_prev: wp.array(dtype=wp.vec3),
vel: wp.array(dtype=wp.vec3),
vel_grad: wp.array(dtype=wp.mat33),
):
"""Read particle velocity from grid and advect positions"""
vel[s.qp_index] = grid_vel(s)
vel_grad[s.qp_index] = grad(grid_vel, s)
pos_adv = pos_prev[s.qp_index] + dt * vel[s.qp_index]
# Project onto domain
pos_proj = domain(lookup(domain, pos_adv))
pos[s.qp_index] = pos_proj
@integrand
def velocity_boundary_projector_form(s: Sample, domain: Domain, u: Field, v: Field):
"""Projector for velocity-Dirichlet boundary conditions"""
n = normal(domain, s)
if n[1] > 0.0:
# Neuman on top
return 0.0
# Free-slip on other sides
return wp.dot(u(s), n) * wp.dot(v(s), n)
@integrand
def divergence_form(s: Sample, u: Field, psi: Field):
return div(u, s) * psi(s)
@wp.kernel
def invert_volume_kernel(values: wp.array(dtype=float)):
i = wp.tid()
m = values[i]
if m <= 1.0e-8:
values[i] = 0.0
else:
values[i] = 1.0 / m
@wp.kernel
def scalar_vector_multiply(
alpha: wp.array(dtype=float),
x: wp.array(dtype=wp.vec3),
y: wp.array(dtype=wp.vec3),
):
i = wp.tid()
y[i] = alpha[i] * x[i]
@wp.kernel
def scale_transposed_divergence_mat(
tr_divergence_mat_offsets: wp.array(dtype=int),
tr_divergence_mat_values: wp.array(dtype=wp.mat(shape=(3, 1), dtype=float)),
inv_fraction_int: wp.array(dtype=float),
):
u_i = wp.tid()
block_beg = tr_divergence_mat_offsets[u_i]
block_end = tr_divergence_mat_offsets[u_i + 1]
for b in range(block_beg, block_end):
tr_divergence_mat_values[b] = tr_divergence_mat_values[b] * inv_fraction_int[u_i]
def solve_incompressibility(divergence_mat: BsrMatrix, inv_volume, pressure, velocity, quiet: bool = False):
"""Solve for divergence-free velocity delta:
delta_velocity = inv_volume * transpose(divergence_mat) * pressure
divergence_mat * (velocity + delta_velocity) = 0
"""
# Build transposed gradient matrix, scale with inverse fraction
transposed_divergence_mat = bsr_transposed(divergence_mat)
wp.launch(
kernel=scale_transposed_divergence_mat,
dim=inv_volume.shape[0],
inputs=[
transposed_divergence_mat.offsets,
transposed_divergence_mat.values,
inv_volume,
],
)
# For simplicity, assemble schur complement and solve with CG
schur = bsr_mm(divergence_mat, transposed_divergence_mat)
rhs = wp.zeros_like(pressure)
bsr_mv(A=divergence_mat, x=velocity, y=rhs, alpha=-1.0, beta=0.0)
bsr_cg(schur, b=rhs, x=pressure, quiet=quiet)
# Apply pressure to velocity
bsr_mv(A=transposed_divergence_mat, x=pressure, y=velocity, alpha=1.0, beta=1.0)
class Example:
def __init__(self, stage, num_frames=1000, res=[32, 64, 16], quiet=False):
self.frame_dt = 1.0 / 60
self.num_frames = num_frames
self.current_frame = 0
self.sim_substeps = 1
self.sim_dt = self.frame_dt / self.sim_substeps
self.sim_steps = self.num_frames * self.sim_substeps
self._quiet = quiet
# grid dimensions and particle emission
grid_res = np.array(res, dtype=int)
particle_fill_frac = np.array([0.5, 0.5, 1.0])
grid_lo = wp.vec3(0.0)
grid_hi = wp.vec3(50, 100, 25)
grid_cell_size = np.array(grid_hi - grid_lo) / grid_res
grid_cell_volume = np.prod(grid_cell_size)
PARTICLES_PER_CELL_DIM = 3
self.radius = float(np.max(grid_cell_size) / (2 * PARTICLES_PER_CELL_DIM))
particle_grid_res = np.array(particle_fill_frac * grid_res * PARTICLES_PER_CELL_DIM, dtype=int)
particle_grid_offset = wp.vec3(self.radius, self.radius, self.radius)
np.random.seed(0)
builder = wp.sim.ModelBuilder()
builder.add_particle_grid(
dim_x=particle_grid_res[0],
dim_y=particle_grid_res[1],
dim_z=particle_grid_res[2],
cell_x=self.radius * 2.0,
cell_y=self.radius * 2.0,
cell_z=self.radius * 2.0,
pos=wp.vec3(0.0, 0.0, 0.0) + particle_grid_offset,
rot=wp.quat_identity(),
vel=wp.vec3(0.0, 0.0, 0.0),
mass=grid_cell_volume / PARTICLES_PER_CELL_DIM**3,
jitter=self.radius * 1.0,
radius_mean=self.radius,
)
self.grid = fem.Grid3D(wp.vec3i(grid_res), grid_lo, grid_hi)
# Function spaces
self.velocity_space = fem.make_polynomial_space(self.grid, dtype=wp.vec3, degree=1)
self.fraction_space = fem.make_polynomial_space(self.grid, dtype=float, degree=1)
self.strain_space = fem.make_polynomial_space(
self.grid,
dtype=float,
degree=0,
)
self.pressure_field = self.strain_space.make_field()
self.velocity_field = self.velocity_space.make_field()
# Test and trial functions
self.domain = fem.Cells(self.grid)
self.velocity_test = fem.make_test(self.velocity_space, domain=self.domain)
self.velocity_trial = fem.make_trial(self.velocity_space, domain=self.domain)
self.fraction_test = fem.make_test(self.fraction_space, domain=self.domain)
self.strain_test = fem.make_test(self.strain_space, domain=self.domain)
self.strain_trial = fem.make_trial(self.strain_space, domain=self.domain)
# Enforcing the Dirichlet boundary condition the hard way;
# build projector for velocity left- and right-hand-sides
boundary = fem.BoundarySides(self.grid)
u_bd_test = fem.make_test(space=self.velocity_space, domain=boundary)
u_bd_trial = fem.make_trial(space=self.velocity_space, domain=boundary)
u_bd_projector = fem.integrate(
velocity_boundary_projector_form, fields={"u": u_bd_trial, "v": u_bd_test}, nodal=True, output_dtype=float
)
fem.normalize_dirichlet_projector(u_bd_projector)
self.vel_bd_projector = u_bd_projector
# Storage for temporary variables
self.temporary_store = fem.TemporaryStore()
self._divergence_matrix = bsr_zeros(
self.strain_space.node_count(),
self.velocity_space.node_count(),
block_type=wp.mat(shape=(1, 3), dtype=float),
)
# Warp.sim model
self.model: Model = builder.finalize()
if not self._quiet:
print("Particle count:", self.model.particle_count)
self.state_0: State = self.model.state()
self.state_0.particle_qd_grad = wp.zeros(shape=(self.model.particle_count), dtype=wp.mat33)
self.state_1: State = self.model.state()
self.state_1.particle_qd_grad = wp.zeros(shape=(self.model.particle_count), dtype=wp.mat33)
self.renderer = warp.sim.render.SimRenderer(self.model, stage, scaling=20.0)
def update(self):
fem.set_default_temporary_store(self.temporary_store)
self.current_frame = self.current_frame + 1
with wp.ScopedTimer(f"simulate frame {self.current_frame}", active=True):
for s in range(self.sim_substeps):
# Bin particles to grid cells
pic = fem.PicQuadrature(
domain=fem.Cells(self.grid), positions=self.state_0.particle_q, measures=self.model.particle_mass
)
# Borrow some temporary arrays for storing integration results
inv_volume_temporary = fem.borrow_temporary(
self.temporary_store, shape=(self.fraction_space.node_count()), dtype=float
)
velocity_int_temporary = fem.borrow_temporary(
self.temporary_store, shape=(self.velocity_space.node_count()), dtype=wp.vec3
)
inv_volume = inv_volume_temporary.array
velocity_int = velocity_int_temporary.array
# Inverse volume fraction
fem.integrate(
integrate_fraction,
quadrature=pic,
fields={"phi": self.fraction_test},
accumulate_dtype=float,
output=inv_volume,
)
wp.launch(kernel=invert_volume_kernel, dim=inv_volume.shape, inputs=[inv_volume])
# Velocity right-hand side
fem.integrate(
integrate_velocity,
quadrature=pic,
fields={"u": self.velocity_test},
values={
"velocities": self.state_0.particle_qd,
"velocity_gradients": self.state_0.particle_qd_grad,
"dt": self.sim_dt,
"gravity": self.model.gravity,
},
accumulate_dtype=float,
output=velocity_int,
)
# Compute constraint-free velocity
wp.launch(
kernel=scalar_vector_multiply,
dim=inv_volume.shape[0],
inputs=[inv_volume, velocity_int, self.velocity_field.dof_values],
)
# Apply velocity boundary conditions:
# velocity -= vel_bd_projector * velocity
wp.copy(src=self.velocity_field.dof_values, dest=velocity_int)
bsr_mv(A=self.vel_bd_projector, x=velocity_int, y=self.velocity_field.dof_values, alpha=-1.0, beta=1.0)
# Divergence matrix
fem.integrate(
divergence_form,
quadrature=pic,
fields={"u": self.velocity_trial, "psi": self.strain_test},
accumulate_dtype=float,
output=self._divergence_matrix,
)
# Project matrix to enforce boundary conditions
divergence_mat_tmp = bsr_copy(self._divergence_matrix)
bsr_mm(alpha=-1.0, x=divergence_mat_tmp, y=self.vel_bd_projector, z=self._divergence_matrix, beta=1.0)
# Solve unilateral incompressibility
solve_incompressibility(
self._divergence_matrix,
inv_volume,
self.pressure_field.dof_values,
self.velocity_field.dof_values,
quiet=self._quiet,
)
# (A)PIC advection
fem.interpolate(
update_particles,
quadrature=pic,
values={
"pos": self.state_1.particle_q,
"pos_prev": self.state_0.particle_q,
"vel": self.state_1.particle_qd,
"vel_grad": self.state_1.particle_qd_grad,
"dt": self.sim_dt,
},
fields={"grid_vel": self.velocity_field},
)
# swap states
(self.state_0, self.state_1) = (self.state_1, self.state_0)
fem.set_default_temporary_store(None)
def render(self, is_live=False):
with wp.ScopedTimer("render", active=True):
time = self.current_frame * self.frame_dt
self.renderer.begin_frame(time)
self.renderer.render(self.state_0)
self.renderer.end_frame()
if __name__ == "__main__":
wp.set_module_options({"enable_backward": False})
wp.init()
stage_path = os.path.join(os.path.dirname(__file__), "outputs/example_sim_apic.usd")
example = Example(stage_path)
for i in range(example.num_frames):
example.update()
example.render()
example.renderer.save()