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Commit 607aafa8 authored by Michael Kuron's avatar Michael Kuron
Browse files

fix more tests on Ubuntu

parent 01a56d31
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pystencils/astnodes.py
View file @ 607aafa8
......@@ -291,7 +291,10 @@ class Block(Node):
self._nodes = nodes
self.parent = None
for n in self._nodes:
n.parent = self
try:
n.parent = self
except AttributeError:
pass
@property
def args(self):
......
pystencils/backends/cbackend.py
View file @ 607aafa8
......@@ -386,6 +386,13 @@ class CustomSympyPrinter(CCodePrinter):
return self._print(expr.args[0])
elif isinstance(expr, fast_inv_sqrt):
return "({})".format(self._print(1 / sp.sqrt(expr.args[0])))
elif isinstance(expr, sp.Abs):
return "abs({})".format(self._print(expr.args[0]))
elif isinstance(expr, sp.Mod):
if expr.is_integer:
return "({} % {})".format(self._print(expr.args[0]), self._print(expr.args[1]))
else:
return "fmod({}, {})".format(self._print(expr.args[0]), self._print(expr.args[1]))
elif expr.func in infix_functions:
return "(%s %s %s)" % (self._print(expr.args[0]), infix_functions[expr.func], self._print(expr.args[1]))
elif expr.func == int_power_of_2:
......
pystencils_tests/test_boundary.py
View file @ 607aafa8
......@@ -3,6 +3,8 @@ from tempfile import TemporaryDirectory
import numpy as np
import pytest
from pystencils import Assignment, create_kernel
from pystencils.boundaries import BoundaryHandling, Neumann, add_neumann_boundary
from pystencils.datahandling import SerialDataHandling
......@@ -83,5 +85,6 @@ def test_kernel_vs_copy_boundary():
np.testing.assert_almost_equal(python_copy_result, handling_result)
with TemporaryDirectory() as tmp_dir:
pytest.importorskip('pyevtk')
boundary_handling.geometry_to_vtk(file_name=os.path.join(tmp_dir, 'test_output1'), ghost_layers=False)
boundary_handling.geometry_to_vtk(file_name=os.path.join(tmp_dir, 'test_output2'), ghost_layers=True)
pystencils_tests/test_buffer_gpu.py
View file @ 607aafa8
......@@ -22,6 +22,7 @@ FIELD_SIZES = [(4, 3), (9, 3, 7)]
def _generate_fields(dt=np.uint8, stencil_directions=1, layout='numpy'):
pytest.importorskip('pycuda')
field_sizes = FIELD_SIZES
if stencil_directions > 1:
field_sizes = [s + (stencil_directions,) for s in field_sizes]
......@@ -44,7 +45,6 @@ def _generate_fields(dt=np.uint8, stencil_directions=1, layout='numpy'):
return fields
@pytest.mark.gpu
def test_full_scalar_field():
"""Tests fully (un)packing a scalar field (from)to a GPU buffer."""
fields = _generate_fields()
......@@ -73,7 +73,6 @@ def test_full_scalar_field():
np.testing.assert_equal(src_arr, dst_arr)
@pytest.mark.gpu
def test_field_slice():
"""Tests (un)packing slices of a scalar field (from)to a buffer."""
fields = _generate_fields()
......@@ -109,7 +108,6 @@ def test_field_slice():
np.testing.assert_equal(src_arr[pack_slice], dst_arr[unpack_slice])
@pytest.mark.gpu
def test_all_cell_values():
"""Tests (un)packing all cell values of the a field (from)to a buffer."""
num_cell_values = 7
......@@ -148,7 +146,6 @@ def test_all_cell_values():
np.testing.assert_equal(src_arr, dst_arr)
@pytest.mark.gpu
def test_subset_cell_values():
"""Tests (un)packing a subset of cell values of the a field (from)to a buffer."""
num_cell_values = 7
......@@ -190,7 +187,6 @@ def test_subset_cell_values():
np.testing.assert_equal(dst_arr, mask_arr.filled(int(0)))
@pytest.mark.gpu
def test_field_layouts():
num_cell_values = 7
for layout_str in ['numpy', 'fzyx', 'zyxf', 'reverse_numpy']:
......
pystencils_tests/test_complex_numbers.py
View file @ 607aafa8
......@@ -57,6 +57,9 @@ def test_complex_numbers(assignment, scalar_dtypes, target):
print(code)
assert "Not supported" not in code
if target == 'gpu':
pytest.importorskip('pycuda')
kernel = ast.compile()
assert kernel is not None
......@@ -100,6 +103,9 @@ def test_complex_numbers_64(assignment, target):
print(code)
assert "Not supported" not in code
if target == 'gpu':
pytest.importorskip('pycuda')
kernel = ast.compile()
assert kernel is not None
......@@ -125,6 +131,7 @@ def test_complex_execution(dtype, target, with_complex_argument):
})
if target == 'gpu':
pytest.importorskip('pycuda')
from pycuda.gpuarray import zeros
x_arr = zeros((20, 30), complex_dtype)
y_arr = zeros((20, 30), complex_dtype)
......
pystencils_tests/test_cuda_known_functions.py
View file @ 607aafa8
import sympy
import pytest
import pystencils
from pystencils.astnodes import get_dummy_symbol
from pystencils.backends.cuda_backend import CudaSympyPrinter
......@@ -19,6 +21,7 @@ def test_cuda_known_functions():
ast = pystencils.create_kernel(assignments, 'gpu')
print(pystencils.show_code(ast))
pytest.importorskip('pycuda')
kernel = ast.compile()
assert(kernel is not None)
......
pystencils_tests/test_datahandling.py
View file @ 607aafa8
......@@ -3,6 +3,8 @@ from tempfile import TemporaryDirectory
import numpy as np
import pytest
import pystencils as ps
from pystencils import create_data_handling, create_kernel
......@@ -128,6 +130,7 @@ def kernel_execution_jacobi(dh, target):
def vtk_output(dh):
pytest.importorskip('pyevtk')
dh.add_array('scalar_field')
dh.add_array('vector_field', values_per_cell=dh.dim)
dh.add_array('multiple_scalar_field', values_per_cell=9)
......@@ -223,6 +226,7 @@ def test_kernel_param(target):
def test_vtk_output():
pytest.importorskip('pyevtk')
for domain_shape in [(4, 5), (3, 4, 5)]:
dh = create_data_handling(domain_size=domain_shape, periodicity=True)
vtk_output(dh)
......
pystencils_tests/test_phasefield_dentritic_3D.ipynb
View file @ 607aafa8
%% Cell type:code id: tags:
``` python
import pytest
pytest.importorskip('pycuda')
```
%% Cell type:code id: tags:
``` python
from pystencils.session import *
sp.init_printing()
frac = sp.Rational
```
%% Cell type:markdown id: tags:
# Phase-field simulation of dentritic solidification in 3D
This notebook tests the model presented in the dentritic growth tutorial in 3D.
%% Cell type:code id: tags:
``` python
target = 'gpu'
gpu = target == 'gpu'
domain_size = (25, 25, 25) if 'is_test_run' in globals() else (300, 300, 300)
dh = ps.create_data_handling(domain_size=domain_size, periodicity=True, default_target=target)
φ_field = dh.add_array('phi', latex_name='φ')
φ_delta_field = dh.add_array('phidelta', latex_name='φ_D')
t_field = dh.add_array('T')
```
%% Cell type:code id: tags:
``` python
ε, m, δ, j, θzero, α, γ, Teq, κ, τ = sp.symbols("ε m δ j θ_0 α γ T_eq κ τ")
εb = sp.Symbol("\\bar{\\epsilon}")
discretize = ps.fd.Discretization2ndOrder(dx=0.03, dt=1e-5)
φ = φ_field.center
T = t_field.center
d = ps.fd.Diff
def f(φ, m):
return φ**4 / 4 - (frac(1, 2) - m/3) * φ**3 + (frac(1,4)-m/2)*φ**2
bulk_free_energy_density = f(φ, m)
interface_free_energy_density = ε ** 2 / 2 * (d(φ, 0) ** 2 + d(φ, 1) ** 2 + d(φ, 2) ** 2)
```
%% Cell type:markdown id: tags:
Here comes the major change, that has to be made for the 3D model: $\epsilon$ depends on the interface normal, which can not be computed simply as atan() as in the 2D case
%% Cell type:code id: tags:
``` python
n = sp.Matrix([d(φ, i) for i in range(3)])
nLen = sp.sqrt(sum(n_i**2 for n_i in n))
n = n / nLen
nVal = sum(n_i**4 for n_i in n)
σ = δ * nVal
εVal = εb * (1 + σ)
εVal
```
%%%% Output: execute_result
$\displaystyle \bar{\epsilon} \left(δ \left(\frac{{\partial_{0} {{φ}_{(0,0,0)}}}^{4}}{\left({\partial_{0} {{φ}_{(0,0,0)}}}^{2} + {\partial_{1} {{φ}_{(0,0,0)}}}^{2} + {\partial_{2} {{φ}_{(0,0,0)}}}^{2}\right)^{2}} + \frac{{\partial_{1} {{φ}_{(0,0,0)}}}^{4}}{\left({\partial_{0} {{φ}_{(0,0,0)}}}^{2} + {\partial_{1} {{φ}_{(0,0,0)}}}^{2} + {\partial_{2} {{φ}_{(0,0,0)}}}^{2}\right)^{2}} + \frac{{\partial_{2} {{φ}_{(0,0,0)}}}^{4}}{\left({\partial_{0} {{φ}_{(0,0,0)}}}^{2} + {\partial_{1} {{φ}_{(0,0,0)}}}^{2} + {\partial_{2} {{φ}_{(0,0,0)}}}^{2}\right)^{2}}\right) + 1\right)$
⎛ ⎛ 4
⎜ ⎜ D(φ[0,0,0])
\bar{\epsilon}⋅⎜δ⋅⎜───────────────────────────────────────────── + ───────────
⎜ ⎜ 2
⎜ ⎜⎛ 2 2 2⎞ ⎛
⎝ ⎝⎝D(φ[0,0,0]) + D(φ[0,0,0]) + D(φ[0,0,0]) ⎠ ⎝D(φ[0,0,0]
4 4
D(φ[0,0,0]) D(φ[0,0,0])
────────────────────────────────── + ─────────────────────────────────────────
2
2 2 2⎞ ⎛ 2 2
) + D(φ[0,0,0]) + D(φ[0,0,0]) ⎠ ⎝D(φ[0,0,0]) + D(φ[0,0,0]) + D(φ[0,0,0]
⎞ ⎞
⎟ ⎟
────⎟ + 1⎟
2⎟ ⎟
2⎞ ⎟ ⎟
) ⎠ ⎠ ⎠
%% Cell type:code id: tags:
``` python
def m_func(temperature):
return (α / sp.pi) * sp.atan(γ * (Teq - temperature))
```
%% Cell type:code id: tags:
``` python
substitutions = {m: m_func(T),
ε: εVal}
fe_i = interface_free_energy_density.subs(substitutions)
fe_b = bulk_free_energy_density.subs(substitutions)
μ_if = ps.fd.expand_diff_full(ps.fd.functional_derivative(fe_i, φ), functions=[φ])
μ_b = ps.fd.expand_diff_full(ps.fd.functional_derivative(fe_b, φ), functions=[φ])
```
%% Cell type:code id: tags:
``` python
dF_dφ = μ_b + sp.Piecewise((μ_if, nLen**2 > 1e-10), (0, True))
```
%% Cell type:code id: tags:
``` python
parameters = {
τ: 0.0003,
κ: 1.8,
εb: 0.01,
δ: 0.3,
γ: 10,
j: 6,
α: 0.9,
Teq: 1.0,
θzero: 0.2,
sp.pi: sp.pi.evalf()
}
parameters
```
%%%% Output: execute_result
![](data:image/png;base64,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)
$\displaystyle \left\{ \pi : 3.14159265358979, \ T_{eq} : 1.0, \ \bar{\epsilon} : 0.01, \ j : 6, \ α : 0.9, \ γ : 10, \ δ : 0.3, \ θ_{0} : 0.2, \ κ : 1.8, \ τ : 0.0003\right\}$
{π: 3.14159265358979, T_eq: 1.0, \bar{\epsilon}: 0.01, j: 6, α: 0.9, γ: 10, δ:
0.3, θ₀: 0.2, κ: 1.8, τ: 0.0003}
%% Cell type:code id: tags:
``` python
dφ_dt = - dF_dφ / τ
assignments = [
ps.Assignment(φ_delta_field.center, discretize(dφ_dt.subs(parameters))),
]
φEqs = ps.simp.sympy_cse_on_assignment_list(assignments)
φEqs.append(ps.Assignment(φ, discretize(ps.fd.transient(φ) - φ_delta_field.center)))
temperatureEvolution = -ps.fd.transient(T) + ps.fd.diffusion(T, 1) + κ * φ_delta_field.center
temperatureEqs = [
ps.Assignment(T, discretize(temperatureEvolution.subs(parameters)))
]
```
%% Cell type:code id: tags:
``` python
temperatureEqs
```
%%%% Output: execute_result
$\displaystyle \left[ {{T}_{(0,0,0)}} \leftarrow 0.0111111111111111 {{T}_{(-1,0,0)}} + 0.0111111111111111 {{T}_{(0,-1,0)}} + 0.0111111111111111 {{T}_{(0,0,-1)}} + 0.933333333333333 {{T}_{(0,0,0)}} + 0.0111111111111111 {{T}_{(0,0,1)}} + 0.0111111111111111 {{T}_{(0,1,0)}} + 0.0111111111111111 {{T}_{(1,0,0)}} + 1.8 \cdot 10^{-5} {{φ_D}_{(0,0,0)}}\right]$
[T_C := 0.0111111111111111⋅T_W + 0.0111111111111111⋅T_S + 0.0111111111111111⋅T
_B + 0.933333333333333⋅T_C + 0.0111111111111111⋅T_T + 0.0111111111111111⋅T_N +
0.0111111111111111⋅T_E + 1.8e-5⋅phidelta_C]
%% Cell type:code id: tags:
``` python
φ_kernel = ps.create_kernel(φEqs, cpu_openmp=4, target=target).compile()
temperatureKernel = ps.create_kernel(temperatureEqs, cpu_openmp=4, target=target).compile()
```
%% Cell type:code id: tags:
``` python
def time_loop(steps):
φ_sync = dh.synchronization_function(['phi'], target=target)
temperature_sync = dh.synchronization_function(['T'], target=target)
dh.all_to_gpu()
for t in range(steps):
φ_sync()
dh.run_kernel(φ_kernel)
temperature_sync()
dh.run_kernel(temperatureKernel)
dh.all_to_cpu()
def init(nucleus_size=np.sqrt(5)):
for b in dh.iterate():
x, y, z = b.cell_index_arrays
x, y, z = x - b.shape[0] // 2, y - b.shape[1] // 2, z - b.shape[2] // 2
b['phi'].fill(0)
b['phi'][(x ** 2 + y ** 2 + z ** 2) < nucleus_size ** 2] = 1.0
b['T'].fill(0.0)
def plot(slice_obj=ps.make_slice[:, :, 0.5]):
plt.subplot(1, 3, 1)
plt.scalar_field(dh.gather_array('phi', slice_obj).squeeze())
plt.title("φ")
plt.colorbar()
plt.subplot(1, 3, 2)
plt.title("T")
plt.scalar_field(dh.gather_array('T', slice_obj).squeeze())
plt.colorbar()
plt.subplot(1, 3, 3)
plt.title("∂φ")
plt.scalar_field(dh.gather_array('phidelta', slice_obj).squeeze())
plt.colorbar()
```
%% Cell type:code id: tags:
``` python
init()
plot()
print(dh)
```
%%%% Output: stream
Name| Inner (min/max)| WithGl (min/max)
----------------------------------------------------
T| ( 0, 0)| ( 0, 0)
phi| ( 0, 1)| ( 0, 1)
phidelta| ( 0, 0)| ( 0, 0)
%%%% Output: display_data
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)
%% Cell type:code id: tags:
``` python
if 'is_test_run' in globals():
time_loop(2)
assert np.isfinite(dh.max('phi'))
assert np.isfinite(dh.max('T'))
assert np.isfinite(dh.max('phidelta'))
else:
from time import perf_counter
vtk_writer = dh.create_vtk_writer('dentritic_growth_large', ['phi'])
last = perf_counter()
for i in range(300):
time_loop(100)
vtk_writer(i)
print("Step ", i, perf_counter() - last, dh.max('phi'))
last = perf_counter()
```
......
pystencils_tests/test_print_infinity.py
View file @ 607aafa8
......@@ -17,6 +17,9 @@ def test_print_infinity(type, negative, target):
assignment = pystencils.Assignment(x.center, oo)
ast = pystencils.create_kernel(assignment, data_type=type, target=target)
if target == 'gpu':
pytest.importorskip('pycuda')
ast.compile()
print(ast.compile().code)
pystencils_tests/test_random.py
View file @ 607aafa8
import numpy as np
import pytest
import pystencils as ps
from pystencils.rng import PhiloxFourFloats, PhiloxTwoDoubles, AESNIFourFloats, AESNITwoDoubles
......@@ -12,6 +14,9 @@ philox_reference = np.array([[[3576608082, 1252663339, 1987745383, 348040302],
def test_philox_double():
for target in ('cpu', 'gpu'):
if target == 'gpu':
pytest.importorskip('pycuda')
dh = ps.create_data_handling((2, 2), default_ghost_layers=0, default_target=target)
f = dh.add_array("f", values_per_cell=2)
......@@ -39,6 +44,9 @@ def test_philox_double():
def test_philox_float():
for target in ('cpu', 'gpu'):
if target == 'gpu':
pytest.importorskip('pycuda')
dh = ps.create_data_handling((2, 2), default_ghost_layers=0, default_target=target)
f = dh.add_array("f", values_per_cell=4)
......
pytest.ini
View file @ 607aafa8
......@@ -3,7 +3,6 @@ python_files = test_*.py *_test.py scenario_*.py
norecursedirs = *.egg-info .git .cache .ipynb_checkpoints htmlcov
addopts = --doctest-modules --durations=20 --cov-config pytest.ini
markers =
gpu: test that require a gpu
kerncraft: tests depending on kerncraft
[run]
......
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