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.gitignore

+3 −0
Original line number Diff line number Diff line
@@ -21,6 +21,9 @@ doc/bibtex.json 
/src/lbmpy/phasefield/simplex_projection.*.so

/src/lbmpy/phasefield/simplex_projection.c



test-report

report.xml



# macOS

**/.DS_Store

*.uuid

.gitlab-ci.yml

+104 −157
Original line number Diff line number Diff line 
stages:

  - pretest

  - test

  - "Code Quality"

  - "Tests"

  - "Prerelease-Tests"

  - integration

  - nightly

  - docs

  - deploy



# --------------------------  Templates ------------------------------------------------------------------------------------

# --------------------------  Code Quality --------------------------------------------------------------------------------



# Base configuration for jobs meant to run at every commit

.every-commit:

  rules:

    - if: $CI_PIPELINE_SOURCE != "schedule"



# Configuration for jobs meant to run on each commit to pycodegen/pystencils/master

.every-commit-master:

  rules:

    - if: '$CI_PIPELINE_SOURCE != "schedule" && $CI_PROJECT_PATH == "pycodegen/lbmpy" && $CI_COMMIT_BRANCH == "master"'



# Linter for code formatting

flake8-lint:

  stage: "Code Quality"

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/nox:alpine

  script:

    - nox -s lint

  tags:

    - docker



# Base configuration for jobs meant to run at a schedule

.scheduled:

  rules:

    - if: $CI_PIPELINE_SOURCE == "schedule"



# --------------------------  Pre Tests --------------------------------------------------------------------------------

# --------------------------  Tests --------------------------------------------------------------------------------



# Normal test - runs on every commit all but "long run" tests

tests-and-coverage:

  stage: pretest

  extends: .every-commit

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/full

testsuite-cuda-py3.10:

  stage: "Tests"

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/nox:ubuntu24.04-cuda12.6

  needs: []

  script:

    # - pip install sympy --upgrade

    - export NUM_CORES=$(nproc --all)

    - mkdir -p ~/.config/matplotlib

    - echo "backend:template" > ~/.config/matplotlib/matplotlibrc

    - mkdir public

    - pip install git+https://gitlab-ci-token:${CI_JOB_TOKEN}@i10git.cs.fau.de/pycodegen/pystencils.git@master#egg=pystencils

    - env

    - pip list

    - py.test -v -n $NUM_CORES --cov-report html --cov-report xml --cov-report term --cov=. -m "not longrun" --junitxml=report.xml

    - python3 -m coverage xml

    - nox -s "testsuite_gpu-3.10(cupy12)"

  tags:

    - docker

    - cuda11

    - cuda

    - cudaComputeCapability6.1

    - AVX

  coverage: /Total coverage:\s\d+.\d+\%/

  artifacts:

    when: always

    paths:

      - coverage_report

      - test-report

    reports:

      coverage_report:

        coverage_format: cobertura

        path: coverage.xml

      junit: report.xml





testsuite-cpu-py3.13:

  stage: "Tests"

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/nox:alpine

  needs: []

  script:

    - mkdir -p ~/.config/matplotlib

    - echo "backend:template" > ~/.config/matplotlib/matplotlibrc

    - nox -s "testsuite_cpu-3.13"

  tags:

    - docker

    - AVX

  artifacts:

    when: always

    paths:

      - test-report

    reports:

      junit: report.xml





# Normal test with longruns

tests-and-coverage-with-longrun:

  stage: test

  stage: "Tests"

  when: manual

  allow_failure: true

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/full
@@ -74,155 +86,88 @@ tests-and-coverage-with-longrun: 
    - py.test -v -n $NUM_CORES

  tags:

    - docker

    - cuda11

    - cuda

    - cudaComputeCapability6.1

    - AVX



minimal-conda:

  stage: pretest

  extends: .every-commit

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/minimal_conda

  script:

    - pip install git+https://gitlab-ci-token:${CI_JOB_TOKEN}@i10git.cs.fau.de/pycodegen/pystencils.git@master#egg=pystencils

    - pip install -e .

    - python quicktest.py

  tags:

    - docker



# Linter for code formatting

flake8-lint:

  stage: pretest

  extends: .every-commit

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/full

  script:

    - flake8 src/lbmpy

  tags:

    - docker

    - cuda11



# -------------------------- Tests -------------------------------------------------------------------------------------

# --------------------------  Nightly and Pre-Release Tests --------------------------------------------------------------------------------



# pipeline with latest python version

latest-python:

  stage: test

  extends: .every-commit

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/latest_python

  before_script:

    - pip install git+https://gitlab-ci-token:${CI_JOB_TOKEN}@i10git.cs.fau.de/pycodegen/pystencils.git@master#egg=pystencils

# Test against latest pystencils 2.0 development version

pystencils-2.0dev:

  stage: "Prerelease-Tests"

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/nox:ubuntu24.04-cuda12.6

  allow_failure: true

  needs: []

  script:

    - env

    - pip list

    - export NUM_CORES=$(nproc --all)

    - mkdir -p ~/.config/matplotlib

    - echo "backend:template" > ~/.config/matplotlib/matplotlibrc

    - mkdir public

    - py.test -v -n $NUM_CORES -m "not longrun" --junitxml=report.xml

    - nox -s "testsuite_pystencils2(cupy12)"

  tags:

    - docker

    - AVX

    - cuda

    - cudaComputeCapability6.1

  artifacts:

    when: always

    paths:

      - test-report

    reports:

      junit: report.xml



# Minimal tests in windows environment

#minimal-windows:

#  stage: test

#  except:

#    variables:

#      - $ENABLE_NIGHTLY_BUILDS

#  tags:

#    - win

#  script:

#    - export NUM_CORES=$(nproc --all)

#    - export MPLBACKEND=Agg

#    - source /cygdrive/c/Users/build/Miniconda3/Scripts/activate

#    - source activate pystencils

#    - pip install git+https://gitlab-ci-token:${CI_JOB_TOKEN}@i10git.cs.fau.de/pycodegen/pystencils.git@master#egg=pystencils

#    - python -c "import numpy"

#    - pip install sympy==1.9

#    - py.test -v -m "not (notebook or longrun)"



minimal-sympy-master:

  stage: test

  extends: .every-commit

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/minimal_conda

  before_script:

    - pip install -e .

  stage: "Prerelease-Tests"

  needs: []

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/nox:alpine

  script:

    - pip install git+https://gitlab-ci-token:${CI_JOB_TOKEN}@i10git.cs.fau.de/pycodegen/pystencils.git@master#egg=pystencils

    - python -m pip install --upgrade git+https://github.com/sympy/sympy.git

    - pip list

    - python quicktest.py

    - nox -s quicktest -P 3.13 -- --sympy-master

  allow_failure: true

  tags:

    - docker

    - cuda



ubuntu:

  stage: test

  extends: .every-commit

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/ubuntu

  before_script:

    # - apt-get -y remove python3-sympy

    - ln -s /usr/include/locale.h /usr/include/xlocale.h

    # - pip3 install `grep -Eo 'sympy[>=]+[0-9\.]+' setup.py | sed 's/>/=/g'`

    - pip3 install git+https://gitlab-ci-token:${CI_JOB_TOKEN}@i10git.cs.fau.de/pycodegen/pystencils.git@master#egg=pystencils

  script:

    - export NUM_CORES=$(nproc --all)

    - mkdir -p ~/.config/matplotlib

    - echo "backend:template" > ~/.config/matplotlib/matplotlibrc

    - env

    - pip3 list

    - pytest -v -n $NUM_CORES -m "not longrun" --junitxml=report.xml

  tags:

    - docker

    - cuda11

  artifacts:

    when: always

    reports:

      junit: report.xml

# pycodegen-integration:

#   image: i10git.cs.fau.de:5005/pycodegen/pycodegen/full

#   stage: integration

#   when: manual

#   allow_failure: true

#   script:

#     - env

#     - pip list

#     - git clone https://gitlab-ci-token:${CI_JOB_TOKEN}@i10git.cs.fau.de/pycodegen/pycodegen.git

#     - cd pycodegen

#     - git submodule sync --recursive

#     - git submodule update --init --recursive

#     - git submodule foreach git fetch origin   # compare the latest master version!

#     - git submodule foreach git reset --hard origin/master

#     - cd lbmpy

#     - git remote add test $CI_REPOSITORY_URL

#     - git fetch test

#     - git reset --hard $CI_COMMIT_SHA

#     - cd ..

#     - pip install -e pystencils/

#     - pip install -e lbmpy/

#     - ./install_walberla.sh

#     # build all integration tests

#     - cd walberla/build/

#     - make -j $NUM_CORES MicroBenchmarkGpuLbm LbCodeGenerationExample

#     - cd apps/benchmarks/UniformGridGPU

#     - make -j $NUM_CORES

#     - cd ../UniformGridCPU

#     - make -j $NUM_CORES



pycodegen-integration:

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/full

  stage: test

  when: manual

  allow_failure: true

  script:

    - env

    - pip list

    - git clone https://gitlab-ci-token:${CI_JOB_TOKEN}@i10git.cs.fau.de/pycodegen/pycodegen.git

    - cd pycodegen

    - git submodule sync --recursive

    - git submodule update --init --recursive

    - git submodule foreach git fetch origin   # compare the latest master version!

    - git submodule foreach git reset --hard origin/master

    - cd lbmpy

    - git remote add test $CI_REPOSITORY_URL

    - git fetch test

    - git reset --hard $CI_COMMIT_SHA

    - cd ..

    - pip install -e pystencils/

    - pip install -e lbmpy/

    - ./install_walberla.sh

    # build all integration tests

    - cd walberla/build/

    - make -j $NUM_CORES MicroBenchmarkGpuLbm LbCodeGenerationExample

    - cd apps/benchmarks/UniformGridGPU

    - make -j $NUM_CORES

    - cd ../UniformGridCPU

    - make -j $NUM_CORES

#   tags:

#     - docker

#     - cuda

#     - cudaComputeCapability6.1

#     - AVX



  tags:

    - docker

    - cuda11

    - AVX



# -------------------- Scheduled Tasks --------------------------------------------------------------------------





nightly-sympy:

  stage: nightly

  extends: .scheduled

  rules:

    - if: $CI_PIPELINE_SOURCE == "schedule"

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/latest_python

  before_script:

    - pip install -e .
@@ -240,6 +185,7 @@ nightly-sympy: 
    - docker

    - AVX

    - cuda

    - cudaComputeCapability6.1

  artifacts:

    when: always

    reports:
@@ -251,7 +197,6 @@ nightly-sympy: 
build-documentation:

  stage: docs

  needs: []

  extends: .every-commit

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/documentation

  before_script:

    - pip install -e .
@@ -262,7 +207,8 @@ build-documentation: 
    - sphinx-build -W -b html doc html_doc

  tags:

    - docker

    - cuda11

    - cuda

    - cudaComputeCapability6.1

  artifacts:

    paths:

      - html_doc
@@ -270,9 +216,10 @@ build-documentation: 


pages:

  image: i10git.cs.fau.de:5005/pycodegen/pycodegen/full

  extends: .every-commit-master

  rules:

    - if: '$CI_PIPELINE_SOURCE != "schedule" && $CI_PROJECT_PATH == "pycodegen/lbmpy" && $CI_COMMIT_BRANCH == "master"'

  stage: deploy

  needs: ["tests-and-coverage", "build-documentation"]

  needs: ["testsuite-cuda-py3.10", "build-documentation"]

  script:

    - ls -l

    - mv coverage_report html_doc

AUTHORS.txt

+1 −0
Original line number Diff line number Diff line
@@ -11,3 +11,4 @@ Contributors: 
  - Rudolf Weeber <weeber@icp.uni-stuttgart.de>

  - Christian Godenschwager <christian.godenschwager@fau.de>

  - Jan Hönig <jan.hoenig@fau.de>

  - Philipp Suffa <philipp.suffa@fau.de>

COPYING.txt

+0 −12
Original line number Diff line number Diff line 
------------------------   Important ---------------------------------



lbmpy is under the following GNU AGPLv3 license. 

This license holds for the sources of lbmpy itself as well 

as for all kernels generated with lbmpy i.e. 

the output of lbmpy is also protected by the GNU AGPLv3 license. 



----------------------------------------------------------------------







                    

                    GNU AFFERO GENERAL PUBLIC LICENSE

                       Version 3, 19 November 2007

conftest.py

+15 −4
Original line number Diff line number Diff line
@@ -5,12 +5,17 @@ import runpy 
import sys

import warnings

import platform

import pathlib



import nbformat

from nbconvert import PythonExporter

import nbconvert

import sympy



from lbmpy._compat import IS_PYSTENCILS_2



# Trigger config file reading / creation once - to avoid race conditions when multiple instances are creating it

# at the same time

if not IS_PYSTENCILS_2:

    from pystencils.cpu import cpujit



# trigger cython imports - there seems to be a problem when multiple processes try to compile the same cython file
@@ -19,7 +24,6 @@ try: 
    import pyximport



    pyximport.install(language_level=3)



    from lbmpy.phasefield.simplex_projection import simplex_projection_2d  # NOQA

except ImportError:

    pass
@@ -45,6 +49,13 @@ collect_ignore = [os.path.join(SCRIPT_FOLDER, "doc", "conf.py"), 
                  os.path.join(SCRIPT_FOLDER, "doc", "img", "mb_discretization", "maxwell_boltzmann_stencil_plot.py")]

add_path_to_ignore('_local_tmp')



if IS_PYSTENCILS_2:

    #   TODO: Fix these step-by-step

    collect_ignore += [

        os.path.join(SCRIPT_FOLDER, "doc", "notebooks", "10_tutorial_conservative_allen_cahn_two_phase.ipynb"),

        os.path.join(SCRIPT_FOLDER, "tests", "test_compiled_in_boundaries.ipynb")

    ]



try:

    import cupy

except ImportError:
@@ -129,7 +140,7 @@ class IPyNbTest(pytest.Item): 


class IPyNbFile(pytest.File):

    def collect(self):

        exporter = PythonExporter()

        exporter = nbconvert.PythonExporter()

        exporter.exclude_markdown = True

        exporter.exclude_input_prompt = True

doc/img/lbmpy-logo.svg

0 → 100644
+794 −0

File added.

Preview size limit exceeded, changes collapsed.

doc/img/logo.svg

+27 −31
Original line number Diff line number Diff line
@@ -2,23 +2,23 @@ 
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   version="1.1"

   id="svg834"

   inkscape:version="0.92.3 (2405546, 2018-03-11)"

   inkscape:version="1.4.2 (ebf0e940d0, 2025-05-08)"

   sodipodi:docname="logo.svg"

   inkscape:export-filename="/local/bauer/code/lbmpy/lbmpy/doc/img/logo.png"

   inkscape:export-xdpi="70.669998"

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   xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#"

   xmlns:cc="http://creativecommons.org/ns#"

   xmlns:dc="http://purl.org/dc/elements/1.1/">

  <defs

     id="defs828">

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@@ -688,21 +694,11 @@ 
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doc/notebooks/08_tutorial_shanchen_twophase.ipynb

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%% Cell type:markdown id: tags:



# Shan-Chen Two-Phase Single-Component Lattice Boltzmann



%% Cell type:code id: tags:



``` python

from lbmpy.session import *

from lbmpy.updatekernels import create_stream_pull_with_output_kernel

from lbmpy.macroscopic_value_kernels import macroscopic_values_getter, macroscopic_values_setter

from lbmpy.maxwellian_equilibrium import get_weights

```



%% Cell type:markdown id: tags:



This is based on section 9.3.2 of Krüger et al.'s "The Lattice Boltzmann Method", Springer 2017 (http://www.lbmbook.com).

Sample code is available at [https://github.com/lbm-principles-practice/code/](https://github.com/lbm-principles-practice/code/blob/master/chapter9/shanchen.cpp).



%% Cell type:markdown id: tags:



## Parameters



%% Cell type:code id: tags:



``` python

N = 64

omega_a = 1.

g_aa = -4.7

rho0 = 1.



stencil = LBStencil(Stencil.D2Q9)

weights = get_weights(stencil, c_s_sq=sp.Rational(1,3))

weights = get_weights(stencil)

```



%% Cell type:markdown id: tags:



## Data structures



%% Cell type:code id: tags:



``` python

dh = ps.create_data_handling((N,) * stencil.D, periodicity=True, default_target=ps.Target.CPU)



src = dh.add_array('src', values_per_cell=stencil.Q)

dst = dh.add_array_like('dst', 'src')



ρ = dh.add_array('rho')

```



%% Cell type:markdown id: tags:



## Force & combined velocity



%% Cell type:markdown id: tags:



The force on the fluid is

$\vec{F}_A(\vec{x})=-\psi(\rho_A(\vec{x}))g_{AA}\sum\limits_{i=1}^{q}w_i\psi(\rho_A(\vec{x}+\vec{c}_i))\vec{c}_i$

with

$\psi(\rho)=\rho_0\left[1-\exp(-\rho/\rho_0)\right]$.



%% Cell type:code id: tags:



``` python

def psi(dens):

    return rho0 * (1. - sp.exp(-dens / rho0));

```



%% Cell type:code id: tags:



``` python

zero_vec = sp.Matrix([0] * stencil.D)



force = sum((psi(ρ[d]) * w_d * sp.Matrix(d)

            for d, w_d in zip(stencil, weights)), zero_vec) * psi(ρ.center) * -1 * g_aa

```



%% Cell type:markdown id: tags:



## Kernels



%% Cell type:code id: tags:



``` python

lbm_config = LBMConfig(stencil=stencil, relaxation_rate=omega_a, compressible=True,

                       force_model=ForceModel.GUO, force=force, kernel_type='collide_only')



collision = create_lb_update_rule(lbm_config=lbm_config,

                                  optimization={'symbolic_field': src})



stream = create_stream_pull_with_output_kernel(collision.method, src, dst, {'density': ρ})





config = ps.CreateKernelConfig(target=dh.default_target, cpu_openmp=False)



stream_kernel = ps.create_kernel(stream, config=config).compile()

collision_kernel = ps.create_kernel(collision, config=config).compile()

```



%% Cell type:markdown id: tags:



## Initialization



%% Cell type:code id: tags:



``` python

method_without_force = create_lb_method(LBMConfig(stencil=stencil, relaxation_rate=omega_a, compressible=True))

init_assignments = macroscopic_values_setter(method_without_force, velocity=(0, 0),

                                             pdfs=src.center_vector, density=ρ.center)





init_kernel = ps.create_kernel(init_assignments, ghost_layers=0, config=config).compile()

```



%% Cell type:code id: tags:



``` python

def init():

    for x in range(N):

        for y in range(N):

            if (x-N/2)**2 + (y-N/2)**2 <= 15**2:

                dh.fill(ρ.name, 2.1, slice_obj=[x,y])

            else:

                dh.fill(ρ.name, 0.15, slice_obj=[x,y])



    dh.run_kernel(init_kernel)

```



%% Cell type:markdown id: tags:



## Timeloop



%% Cell type:code id: tags:



``` python

sync_pdfs = dh.synchronization_function([src.name])

sync_ρs = dh.synchronization_function([ρ.name])



def time_loop(steps):

    dh.all_to_gpu()

    for i in range(steps):

        sync_ρs()

        dh.run_kernel(collision_kernel)



        sync_pdfs()

        dh.run_kernel(stream_kernel)



        dh.swap(src.name, dst.name)

    dh.all_to_cpu()

```



%% Cell type:code id: tags:



``` python

def plot_ρs():

    plt.figure(dpi=200)

    plt.title("$\\rho$")

    plt.scalar_field(dh.gather_array(ρ.name), vmin=0, vmax=2.5)

    plt.colorbar()

```



%% Cell type:markdown id: tags:



## Run the simulation

### Initial state



%% Cell type:code id: tags:



``` python

init()

plot_ρs()

```



%% Output



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


%% Cell type:markdown id: tags:



### Run the simulation until converged



%% Cell type:code id: tags:



``` python

init()

time_loop(1000)

plot_ρs()

```



%% Output



img 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


%% Cell type:code id: tags:



``` python

assert np.isfinite(dh.gather_array(ρ.name)).all()

```

doc/notebooks/09_tutorial_shanchen_twocomponent.ipynb

+1 −1
Original line number Diff line number Diff line 
%% Cell type:markdown id: tags:



# Shan-Chen Two-Component Lattice Boltzmann



%% Cell type:code id: tags:



``` python

from lbmpy.session import *

from lbmpy.updatekernels import create_stream_pull_with_output_kernel

from lbmpy.macroscopic_value_kernels import macroscopic_values_getter, macroscopic_values_setter

from lbmpy.maxwellian_equilibrium import get_weights

```



%% Cell type:markdown id: tags:



This is based on section 9.3.3 of Krüger et al.'s "The Lattice Boltzmann Method", Springer 2017 (http://www.lbmbook.com).

Sample code is available at [https://github.com/lbm-principles-practice/code/](https://github.com/lbm-principles-practice/code/blob/master/chapter9/shanchen.cpp).



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## Parameters



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``` python

N = 64       # domain size

omega_a = 1. # relaxation rate of first component

omega_b = 1. # relaxation rate of second component



# interaction strength

g_aa = 0.

g_ab = g_ba = 6.

g_bb = 0.



rho0 = 1.



stencil = LBStencil(Stencil.D2Q9)

weights = get_weights(stencil, c_s_sq=sp.Rational(1, 3))

weights = get_weights(stencil)

```



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## Data structures



We allocate two sets of PDF's, one for each phase. Additionally, for each phase there is one field to store its density and velocity.



To run the simulation on GPU, change the `default_target` to gpu



%% Cell type:code id: tags:



``` python

dim = stencil.D

dh = ps.create_data_handling((N, ) * dim, periodicity=True, default_target=ps.Target.CPU)



src_a = dh.add_array('src_a', values_per_cell=stencil.Q)

dst_a = dh.add_array_like('dst_a', 'src_a')



src_b = dh.add_array('src_b', values_per_cell=stencil.Q)

dst_b = dh.add_array_like('dst_b', 'src_b')



ρ_a = dh.add_array('rho_a')

ρ_b = dh.add_array('rho_b')

u_a = dh.add_array('u_a', values_per_cell=stencil.D)

u_b = dh.add_array('u_b', values_per_cell=stencil.D)

u_bary = dh.add_array_like('u_bary', u_a.name)



f_a = dh.add_array('f_a', values_per_cell=stencil.D)

f_b = dh.add_array_like('f_b', f_a.name)

```



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## Force & combined velocity



The two LB methods are coupled using a force term. Its symbolic representation is created in the next cells.

The force value is not written to a field, but directly evaluated inside the collision kernel.



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The force between the two components is

$\mathbf{F}_k(\mathbf{x})=-\psi(\rho_k(\mathbf{x}))\sum\limits_{k^\prime\in\{A,B\}}g_{kk^\prime}\sum\limits_{i=1}^{q}w_i\psi(\rho_{k^\prime}(\mathbf{x}+\mathbf{c}_i))\mathbf{c}_i$

for $k\in\{A,B\}$

and with

$\psi(\rho)=\rho_0\left[1-\exp(-\rho/\rho_0)\right]$.



%% Cell type:code id: tags:



``` python

def psi(dens):

    return rho0 * (1. - sp.exp(-dens / rho0));

```



%% Cell type:code id: tags:



``` python

zero_vec = sp.Matrix([0] * dh.dim)



force_a = zero_vec

for factor, ρ in zip([g_aa, g_ab], [ρ_a, ρ_b]):

    force_a += sum((psi(ρ[d]) * w_d * sp.Matrix(d)

                    for d, w_d in zip(stencil, weights)),

                   zero_vec) * psi(ρ_a.center) * -1 * factor



force_b = zero_vec

for factor, ρ in zip([g_ba, g_bb], [ρ_a, ρ_b]):

    force_b += sum((psi(ρ[d]) * w_d * sp.Matrix(d)

                    for d, w_d in zip(stencil, weights)),

                   zero_vec) * psi(ρ_b.center) * -1 * factor



f_expressions = ps.AssignmentCollection([

    ps.Assignment(f_a.center_vector, force_a),

    ps.Assignment(f_b.center_vector, force_b)

])

```



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The barycentric velocity, which is used in place of the individual components' velocities in the equilibrium distribution and Guo force term, is

$\vec{u}=\frac{1}{\rho_a+\rho_b}\left(\rho_a\vec{u}_a+\frac{1}{2}\vec{F}_a+\rho_b\vec{u}_b+\frac{1}{2}\vec{F}_b\right)$.



%% Cell type:code id: tags:



``` python

u_full = list(ps.Assignment(u_bary.center_vector,

                           (ρ_a.center * u_a.center_vector + ρ_b.center * u_b.center_vector) / (ρ_a.center + ρ_b.center)))

```



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## Kernels



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``` python

lbm_config_a = LBMConfig(stencil=stencil, relaxation_rate=omega_a, compressible=True,

                         velocity_input=u_bary, density_input=ρ_a, force_model=ForceModel.GUO,

                         force=f_a, kernel_type='collide_only')



lbm_config_b = LBMConfig(stencil=stencil, relaxation_rate=omega_b, compressible=True,

                         velocity_input=u_bary, density_input=ρ_b, force_model=ForceModel.GUO,

                         force=f_b, kernel_type='collide_only')







collision_a = create_lb_update_rule(lbm_config=lbm_config_a,

                                    optimization={'symbolic_field': src_a})



collision_b = create_lb_update_rule(lbm_config=lbm_config_b,

                                    optimization={'symbolic_field': src_b})

```



%% Cell type:code id: tags:



``` python

stream_a = create_stream_pull_with_output_kernel(collision_a.method, src_a, dst_a,

                                                 {'density': ρ_a, 'velocity': u_a})

stream_b = create_stream_pull_with_output_kernel(collision_b.method, src_b, dst_b,

                                                 {'density': ρ_b, 'velocity': u_b})



config = ps.CreateKernelConfig(target=dh.default_target)



stream_a_kernel = ps.create_kernel(stream_a, config=config).compile()

stream_b_kernel = ps.create_kernel(stream_b, config=config).compile()

collision_a_kernel = ps.create_kernel(collision_a, config=config).compile()

collision_b_kernel = ps.create_kernel(collision_b, config=config).compile()



force_kernel = ps.create_kernel(f_expressions, config=config).compile()

u_kernel = ps.create_kernel(u_full, config=config).compile()

```



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## Initialization



%% Cell type:code id: tags:



``` python

init_a = macroscopic_values_setter(collision_a.method, velocity=(0, 0),

                                   pdfs=src_a.center_vector, density=ρ_a.center)

init_b = macroscopic_values_setter(collision_b.method, velocity=(0, 0),

                                   pdfs=src_b.center_vector, density=ρ_b.center)

init_a_kernel = ps.create_kernel(init_a, ghost_layers=0).compile()

init_b_kernel = ps.create_kernel(init_b, ghost_layers=0).compile()





dh.run_kernel(init_a_kernel)

dh.run_kernel(init_b_kernel)

```



%% Cell type:code id: tags:



``` python

def init():

    dh.fill(ρ_a.name, 0.1, slice_obj=ps.make_slice[:, :0.5])

    dh.fill(ρ_a.name, 0.9, slice_obj=ps.make_slice[:, 0.5:])



    dh.fill(ρ_b.name, 0.9, slice_obj=ps.make_slice[:, :0.5])

    dh.fill(ρ_b.name, 0.1, slice_obj=ps.make_slice[:, 0.5:])



    dh.fill(f_a.name, 0.0)

    dh.fill(f_b.name, 0.0)



    dh.run_kernel(init_a_kernel)

    dh.run_kernel(init_b_kernel)



    dh.fill(u_a.name, 0.0)

    dh.fill(u_b.name, 0.0)

```



%% Cell type:markdown id: tags:



## Timeloop



%% Cell type:code id: tags:



``` python

sync_pdfs = dh.synchronization_function([src_a.name, src_b.name])

sync_ρs = dh.synchronization_function([ρ_a.name, ρ_b.name])



def time_loop(steps):

    dh.all_to_gpu()

    for i in range(steps):

        sync_ρs()  # force values depend on neighboring ρ's

        dh.run_kernel(force_kernel)

        dh.run_kernel(u_kernel)

        dh.run_kernel(collision_a_kernel)

        dh.run_kernel(collision_b_kernel)



        sync_pdfs()

        dh.run_kernel(stream_a_kernel)

        dh.run_kernel(stream_b_kernel)



        dh.swap(src_a.name, dst_a.name)

        dh.swap(src_b.name, dst_b.name)

    dh.all_to_cpu()

```



%% Cell type:code id: tags:



``` python

def plot_ρs():

    plt.figure(dpi=200)

    plt.subplot(1,2,1)

    plt.title("$\\rho_A$")

    plt.scalar_field(dh.gather_array(ρ_a.name), vmin=0, vmax=2)

    plt.colorbar()

    plt.subplot(1,2,2)

    plt.title("$\\rho_B$")

    plt.scalar_field(dh.gather_array(ρ_b.name), vmin=0, vmax=2)

    plt.colorbar()

```



%% Cell type:markdown id: tags:



## Run the simulation

### Initial state



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``` python

init()

plot_ρs()

```



%% Output



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


%% Cell type:markdown id: tags:



### Run the simulation until converged



%% Cell type:code id: tags:



``` python

init()

time_loop(10000)

plot_ρs()

```



%% Output



img 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">
 


%% Cell type:code id: tags:



``` python

assert np.isfinite(dh.gather_array(ρ_a.name)).all()

assert np.isfinite(dh.gather_array(ρ_b.name)).all()

```

doc/notebooks/demo_interpolation_boundary_conditions.ipynb

+0 −2
Original line number Diff line number Diff line 
%% Cell type:code id: tags:















``` python















from IPython.display import clear_output















from lbmpy.session import *















from lbmpy.relaxationrates import relaxation_rate_from_lattice_viscosity

























from pystencils.typing import BasicType, TypedSymbol















```





























%% Cell type:markdown id: tags:





























# Demo: Interpolation Bounce Back Boundaries















In this notebook we present how to use interpolation bounce back boundaries. We will show this on a simple flow around sphere in two dimensions using the linearised bounce back boundary by [Bouzidi et. al.](https://doi.org/10.1063/1.1399290) and the `QuadraticBounceBack` boundary condition by [Geier et. al.](https://www.sciencedirect.com/science/article/pii/S0898122115002126)





























The first part of the demo is similar to other demos / tutorials, so we will not go into detail about these parts





























%% Cell type:code id: tags:





























``` python















stencil = LBStencil(Stencil.D2Q9)















reference_length = 30















maximal_velocity = 0.05















reynolds_number = 500















kinematic_vicosity = (reference_length * maximal_velocity) / reynolds_number





























initial_velocity=(maximal_velocity, 0)















omega = relaxation_rate_from_lattice_viscosity(kinematic_vicosity)















```





























%% Cell type:code id: tags:





























``` python















domain_size = (400, 150)















dim = len(domain_size)















circle_mid = np.array((40, 75))















circle_rad = 10















```





























%% Cell type:code id: tags:





























``` python















dh = ps.create_data_handling(domain_size=domain_size)





























src = dh.add_array('pdfs', values_per_cell=len(stencil))















dh.fill(src.name, 0.0, ghost_layers=True)















dst = dh.add_array('pdfs_tmp', values_per_cell=len(stencil))















dh.fill(dst.name, 0.0, ghost_layers=True)





























velField = dh.add_array('velField', values_per_cell=dh.dim)















dh.fill('velField', 0.0, ghost_layers=True)





























densityField = dh.add_array('densityField', values_per_cell=1)















dh.fill('densityField', 1.0, ghost_layers=True)















```





























%% Cell type:code id: tags:





























``` python















lbm_config = LBMConfig(stencil=stencil, method=Method.CUMULANT, relaxation_rate=omega,















                       compressible=True, output={"velocity": velField, "density": densityField})





























method = create_lb_method(lbm_config=lbm_config)















```





























%% Cell type:code id: tags:





























``` python















init = pdf_initialization_assignments(method, 1.0, (0.0, 0.0, 0.0), src.center_vector)





























ast_init = ps.create_kernel(init, target=dh.default_target)















kernel_init = ast_init.compile()





























dh.run_kernel(kernel_init)















```





























%% Cell type:code id: tags:





























``` python















lbm_optimisation = LBMOptimisation(symbolic_field=src, symbolic_temporary_field=dst)















update = create_lb_update_rule(lb_method=method,















                               lbm_config=lbm_config,















                               lbm_optimisation=lbm_optimisation)





























ast_kernel = ps.create_kernel(update, target=dh.default_target)















kernel = ast_kernel.compile()















```





























%% Cell type:code id: tags:





























``` python















def set_sphere(x, y, *_):















    return (x-circle_mid[0])**2 + (y-circle_mid[1])**2 < circle_rad**2















```





























%% Cell type:markdown id: tags:





























# Interpolation Boundary Conditions implementation details





























The most important part of the interpolation bounce back boundary is, that we need to define the distance to the wall for each boundary cell. Thus, we need to provide a Python CallBack function to the boundary that calculates the normalised wall distance `q` for each cell and stores the value in `boundary_data`. The normalised wall distance is defined as:





























$$















\begin{align}















q = \frac{|\boldsymbol{x}_{F} - \boldsymbol{x}_{w}|}{|\boldsymbol{x}_{F} - \boldsymbol{x}_{b}|}.















\end{align}















$$





























 The variable `boundary_data` is an index vector that every boundary condition holds internally. For simple boundaries it stores the `x`- and `y`- (and `z` in 3D) coordinate to represent a fluid cell that is next to a boundary cell and the lattice direction `dir` to get from the fluid cell to the boundary cell.





























In the case of the interpolation boundaries we have an additional value `q` that needs to be stored in each cell. This value needs to be between 0 and 1, otherwise the boundary condition would fall back to a simple bounce back boundary without interpolation.





























<center>















<img src="../img/Boundary.svg" alt="Boundary.svg" width="400" height="400">















</center>





























Two dimensional representation of the boundary nodes with the normalised wall distance `q`. The figure was inspired by [Directional lattice Boltzmann boundary conditions](https://doi.org/10.13097/archive-ouverte/unige:160770).





























The linear Bouzidi boundary condition is implemented using the following equation















$$















\begin{align}















    f_{\bar{i}}^{t + 1}(\boldsymbol{x}_b) =















\begin{cases}















    \frac{1}{2q} f_{i}(\boldsymbol{x}_F) + \frac{2q-1}{2q} f_{\bar{i}}(\boldsymbol{x}_{F}), & \text{if } q \geq 0.5\\















    2 q f_{i}(\boldsymbol{x}_F) + (1 - 2q) f_{i}(\boldsymbol{x}_{FF}),              & q > 0 \land q < 0.5 \\















    f_{i}(\boldsymbol{x}_F),              & q = -1















\end{cases}















\end{align}















$$





























where $f_{\bar{i}}^{t + 1}(\boldsymbol{x}_b)$ is the missing lattice link that will be needed in the next streaming step. Furthermore, $f_{i}(\boldsymbol{x}_F)$ represents the lattice link flowing in wall direction at $\boldsymbol{x}_{F}$, $f_{\bar{i}}(\boldsymbol{x}_{F})$ is the inverse direction at $\boldsymbol{x}_{F}$ and $f_{i}(\boldsymbol{x}_{FF})$ is the lattice link at the next cell.





























**The linearised bounce back boundary by [Bouzidi et. al.](https://doi.org/10.1063/1.1399290) needs a second fluid node for the interpolation. This fluid node is not guaranteed to exist. In this case, we implemented a fallback scenario to a simple bounce back scheme with interpolation by setting `q` to -1.**





























To overcome this problem, we can use the `QuadraticBounceBack` boundary condition by [Geier et. al.](https://www.sciencedirect.com/science/article/pii/S0898122115002126). It uses the following rule:





























$$















\begin{align}















f_{\bar{i}}^{\mathrm{p}}(\boldsymbol{x}_F) &= \frac{f_{\bar{i}}(\boldsymbol{x}_F) - f_{i}(\boldsymbol{x}_F)}{2} + \frac{f_{\bar{i}}(\boldsymbol{x}_F) + f_{i}(\boldsymbol{x}_F)- \omega(f_{\bar{i}}^{\mathrm{eq}}(\boldsymbol{x}_F) + f_{i}^{\mathrm{eq}}(\boldsymbol{x}_F))}{2 - 2\omega} \\















f_{\bar{i}}^{\mathrm{wall}}(\boldsymbol{x}_F) &= (1 - q)f_{\bar{i}}^{\mathrm{p}}(\boldsymbol{x}_F) + q f_{\bar{i}}(\boldsymbol{x}_F) \\















f_{\bar{i}}^{t + 1}(\boldsymbol{x}_b) &= \frac{1}{q+1} f_{\bar{i}}^{\mathrm{wall}}(\boldsymbol{x}_F) + \frac{q}{q+1}f_{i}(\boldsymbol{x}_F)















\end{align}















$$





























In this BC the idea is to realise the interpolation with the pre collision PDF value (marked with the subscript p). Since the pre collision PDF value is not available a simple reconstruction needs to be done. This happens via the BGK rule and the relaxation rate for the fluid viscosity. Thus, this boundary condition needs the equilibrium at the wall. However, the equilibrium at the wall can be calculated inplace from the PDFs. Thus, this BC does not need any further information and can be applied in all cases. Furthermore, we have no more branches with the subgrid distance `q`





























%% Cell type:code id: tags:





























``` python















def init_wall_distance(boundary_data, **_):















    dim = boundary_data.dim















    coords = [coord for coord, _ in zip(['x', 'y', 'z'], range(dim))]





























    for cell in boundary_data.index_array:















        direction = np.array(stencil[cell['dir']])















        fluid_cell = np.array(tuple([cell[coord] for coord in coords])) - np.array([0.5] * dim)















        boundary_cell = fluid_cell + direction





























        f = fluid_cell - circle_mid















        d = (boundary_cell - circle_mid) - f





























        a = d.dot(d)















        b = 2.0 * ( d.dot(f))















        c = f.dot(f) - circle_rad**2





























        bb4ac = b * b - ( 4.0 * a * c )















        assert bb4ac > 0





























        sqrtbb4ac = np.sqrt(bb4ac)















        q = np.min( [( -b + sqrtbb4ac ) / ( 2.0 * a ), ( -b - sqrtbb4ac ) / ( 2.0 * a )] )





























        assert q > 0 and q < 1





























        cell['q'] = q















```





























%% Cell type:code id: tags:





























``` python















bh = LatticeBoltzmannBoundaryHandling(method, dh, src.name, name="bh")





























inflow = UBB(initial_velocity)















outflow = ExtrapolationOutflow(stencil[4], method)















wall = NoSlip("wall")















# obstacle = NoSlip("obstacle")















# obstacle = NoSlipLinearBouzidi("obstacle", init_wall_distance=init_wall_distance)















obstacle = QuadraticBounceBack(omega, "obstacle", init_wall_distance=init_wall_distance)





























bh.set_boundary(inflow, slice_from_direction('W', dim))















bh.set_boundary(outflow, slice_from_direction('E', dim))















for direction in ('N', 'S'):















    bh.set_boundary(wall, slice_from_direction(direction, dim))





























bh.set_boundary(obstacle, mask_callback=set_sphere)





























plt.figure(dpi=200)















plt.boundary_handling(bh)















```





























%% Output





























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%% Cell type:code id: tags:





























``` python















def timeloop(timeSteps):















    for i in range(timeSteps):















        bh()















        dh.run_kernel(kernel)















        dh.swap(src.name, dst.name)















```





























%% Cell type:code id: tags:





























``` python















mask = np.fromfunction(set_sphere, (domain_size[0], domain_size[1], len(domain_size)))















if 'is_test_run' not in globals():















    timeloop(50000)  # initial steps





























    def run():















        timeloop(50)















        return np.ma.array(dh.gather_array('velField'), mask=mask)





























    animation = plt.vector_field_magnitude_animation(run, frames=600, rescale=True)















    set_display_mode('video')















    res = display_animation(animation)















else:















    timeloop(10)















    res = None















res















```





























%% Output





























    <IPython.core.display.HTML object>





























noxfile.py
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+170
−0
















Original line number
Diff line number
Diff line













from __future__ import annotations













from typing import Sequence













from argparse import ArgumentParser



























import os













import nox













import subprocess













import re



























nox.options.sessions = ["lint", "typecheck"]









































def get_cuda_version(session: nox.Session) -> None | tuple[int, ...]:













    query_args = ["nvcc", "--version"]



























    try:













        query_result = subprocess.run(query_args, capture_output=True)













    except FileNotFoundError:













        return None



























    matches = re.findall(r"release \d+\.\d+", str(query_result.stdout))













    if matches:













        match = matches[0]













        version_string = match.split()[-1]













        try:













            return tuple(int(v) for v in version_string.split("."))













        except ValueError:













            pass



























    session.warn("nvcc was found, but I am unable to determine the CUDA version.")













    return None









































def install_cupy(













    session: nox.Session, cupy_version: str, skip_if_no_cuda: bool = False













):













    if cupy_version is not None:













        cuda_version = get_cuda_version(session)













        if cuda_version is None or cuda_version[0] not in (11, 12):













            if skip_if_no_cuda:













                session.skip(













                    "No compatible installation of CUDA found - Need either CUDA 11 or 12"













                )













            else:













                session.warn(













                    "Running without cupy: no compatbile installation of CUDA found. Need either CUDA 11 or 12."













                )













                return



























        cuda_major = cuda_version[0]













        cupy_package = f"cupy-cuda{cuda_major}x=={cupy_version}"













        session.install(cupy_package)









































def check_external_doc_dependencies(session: nox.Session):













    dot_args = ["dot", "--version"]













    try:













        _ = subprocess.run(dot_args, capture_output=True)













    except FileNotFoundError:













        session.error(













            "Unable to build documentation: "













            "Command `dot` from the `graphviz` package (https://www.graphviz.org/) is not available"













        )









































def editable_install(session: nox.Session, opts: Sequence[str] = ()):













    if opts:













        opts_str = "[" + ",".join(opts) + "]"













    else:













        opts_str = ""













    session.install("-e", f".{opts_str}")









































def install_pystencils_master(session: nox.Session):













    session.install("git+https://i10git.cs.fau.de/pycodegen/pystencils.git@master")









































def install_sympy_master(session: nox.Session):













    session.install("--upgrade", "git+https://github.com/sympy/sympy.git@master")









































@nox.session(python="3.10", tags=["qa", "code-quality"])













def lint(session: nox.Session):













    """Lint code using flake8"""



























    session.install("flake8")













    session.run("flake8", "src/lbmpy")









































@nox.session(python="3.10", tags=["qa", "code-quality"])













def typecheck(session: nox.Session):













    """Run MyPy for static type checking"""













    editable_install(session)













    session.install("mypy")













    session.run("mypy", "src/lbmpy")









































def run_testsuite(session: nox.Session, coverage: bool = True):













    num_cores = os.cpu_count()



























    args = [













        "pytest",













        "-v",













        "-n",













        str(num_cores),













        "-m",













        "not longrun",













        "--html",













        "test-report/index.html",













        "--junitxml=report.xml",













    ]



























    if coverage:













        args += [













            "--cov-report=term",













            "--cov=.",













        ]



























    session.run(*args)



























    if coverage:













        session.run("coverage", "html")













        session.run("coverage", "xml")









































@nox.session(python=["3.10", "3.11", "3.12", "3.13"])













def testsuite_cpu(session: nox.Session):













    install_pystencils_master(session)













    editable_install(session, ["alltrafos", "use_cython", "interactive", "tests"])













    run_testsuite(session, coverage=False)









































@nox.session(python=["3.10", "3.11", "3.12", "3.13"])













@nox.parametrize("cupy_version", ["12", "13"], ids=["cupy12", "cupy13"])













def testsuite_gpu(session: nox.Session, cupy_version: str | None):













    install_cupy(session, cupy_version, skip_if_no_cuda=True)













    install_pystencils_master(session)













    editable_install(session, ["alltrafos", "use_cython", "interactive", "tests"])













    run_testsuite(session)









































@nox.parametrize("cupy_version", [None, "12", "13"], ids=["cpu", "cupy12", "cupy13"])













@nox.session(python="3.10", tags=["test"])













def testsuite_pystencils2(session: nox.Session, cupy_version: str | None):













    if cupy_version is not None:













        install_cupy(session, cupy_version, skip_if_no_cuda=True)



























    session.install(













        "git+https://i10git.cs.fau.de/pycodegen/pystencils.git@v2.0-dev"













    )













    editable_install(session, ["alltrafos", "use_cython", "interactive", "tests"])



























    run_testsuite(session)









































@nox.session













def quicktest(session: nox.Session):













    parser = ArgumentParser()













    parser.add_argument(













        "--sympy-master", action="store_true", help="Use latest SymPy master revision"













    )













    args = parser.parse_args(session.posargs)



























    install_pystencils_master(session)













    editable_install(session)



























    if args.sympy_master:













        install_sympy_master(session)



























    session.run("python", "quicktest.py")
























pyproject.toml



+1
−1
















Original line number
Diff line number
Diff line








@@ -11,7 +11,7 @@ authors = [













]















license = { file = "COPYING.txt" }















requires-python = ">=3.10"













dependencies = ["pystencils>=1.3", "sympy>=1.9,<=1.12.1", "numpy>=1.8.0", "appdirs", "joblib"]













dependencies = ["pystencils>=1.3", "sympy>=1.12", "numpy>=1.8.0", "appdirs", "joblib", "packaging"]















classifiers = [















    "Development Status :: 4 - Beta",















    "Framework :: Jupyter",

































pytest.ini



+9
−1
















Original line number
Diff line number
Diff line








@@ -3,7 +3,12 @@ testpaths = src tests doc/notebooks













pythonpath = src















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













addopts = 













       --doctest-modules --durations=20













       --cov-config pytest.ini













       --ignore=src/lbmpy/custom_code_nodes.py













       --ignore=src/lbmpy/lookup_tables.py













       --ignore=src/lbmpy/phasefield_allen_cahn/contact_angle.py















markers =















       longrun: tests only run at night since they have large execution time















       notebook: mark for notebooks









@@ -24,7 +29,10 @@ omit = doc/*













       setup.py















       conftest.py















       versioneer.py













       quicktest.py













       noxfile.py















       src/lbmpy/_version.py













       src/lbmpy/_compat.py















       venv/































[report]

































src/lbmpy/_compat.py
0 → 100644



+42
−0
















Original line number
Diff line number
Diff line













from pystencils import __version__ as ps_version



























#   Determine if we're running pystencils 1.x or 2.x













version_tokes = ps_version.split(".")



























PYSTENCILS_VERSION_MAJOR = int(version_tokes[0])













IS_PYSTENCILS_2 = PYSTENCILS_VERSION_MAJOR == 2



























if IS_PYSTENCILS_2:













    from pystencils.defaults import DEFAULTS



























    def get_loop_counter_symbol(coord: int):













        return DEFAULTS.spatial_counters[coord]



























    def get_supported_instruction_sets():













        from pystencils import Target













        vector_targets = Target.available_vector_cpu_targets()













        isas = []













        for target in vector_targets:













            tokens = target.name.split("_")













            isas.append(tokens[-1].lower())













        return isas



























else:













    from pystencils.backends.simd_instruction_sets import (













        get_supported_instruction_sets as get_supported_instruction_sets_,













    )



























    get_supported_instruction_sets = get_supported_instruction_sets_



























    def get_loop_counter_symbol(coord: int):













        from pystencils.astnodes import LoopOverCoordinate



























        return LoopOverCoordinate.get_loop_counter_symbol(coord)









































def import_guard_pystencils1(feature):













    if IS_PYSTENCILS_2:













        raise ImportError(













            f"The following feature is not yet available when running pystencils 2.x: {feature}"













        )













    return True
























src/lbmpy/advanced_streaming/communication.py



+1
−2
















Original line number
Diff line number
Diff line















import itertools













from pystencils import CreateKernelConfig, Field, Assignment, AssignmentCollection













from pystencils import CreateKernelConfig, Field, Assignment, AssignmentCollection, Target















from pystencils.slicing import (















    shift_slice,















    get_slice_before_ghost_layer,









@@ -14,7 +14,6 @@ from lbmpy.advanced_streaming.utility import (













    numeric_offsets,















)















from pystencils.datahandling import SerialDataHandling













from pystencils.enums import Target















from itertools import chain

































































src/lbmpy/advanced_streaming/indexing.py



+33
−8
















Original line number
Diff line number
Diff line








@@ -2,10 +2,17 @@ import numpy as np













import sympy as sp















import pystencils as ps





























from .._compat import IS_PYSTENCILS_2



























if IS_PYSTENCILS_2:













    from pystencils import TypedSymbol, create_type













    from pystencils.types.quick import Arr













    from lbmpy.lookup_tables import TranslationArraysNode













else:















    from pystencils.typing import TypedSymbol, create_type













from lbmpy.advanced_streaming.utility import get_accessor, inverse_dir_index, is_inplace, Timestep













from lbmpy.custom_code_nodes import TranslationArraysNode













    from ..custom_code_nodes import TranslationArraysNode





























from lbmpy.advanced_streaming.utility import get_accessor, inverse_dir_index, is_inplace, Timestep















from itertools import product










































@@ -64,13 +71,21 @@ class BetweenTimestepsIndexing:













        assert f_dir in ['in', 'out']















        inv = '_inv' if inverse else ''















        name = f"f_{f_dir}{inv}_dir_idx"













        if IS_PYSTENCILS_2:













            return TypedSymbol(name, Arr(self._index_dtype, self._q))













        else:















            return TypedSymbol(name, self._index_dtype)































    def _offset_array_symbols(self, f_dir, inverse):















        assert f_dir in ['in', 'out']















        inv = '_inv' if inverse else ''















        name_base = f"f_{f_dir}{inv}_offsets_"



























        if IS_PYSTENCILS_2:













            symbols = [TypedSymbol(name_base + d, Arr(self._index_dtype, self._q)) for d in self._coordinate_names]













        else:















            symbols = [TypedSymbol(name_base + d, self._index_dtype) for d in self._coordinate_names]













        















        return symbols































    def _array_symbols(self, f_dir, inverse, index):










@@ -169,6 +184,10 @@ class BetweenTimestepsIndexing:













            indices, offsets = self._get_translated_indices_and_offsets(f_dir, inv)















            index_array_symbol = self._index_array_symbol(f_dir, inv)















            symbols_defined.add(index_array_symbol)



























            if IS_PYSTENCILS_2:













                array_content.append((index_array_symbol, indices))













            else:















                array_content.append((self._index_dtype, index_array_symbol.name, indices))































        for f_dir, inv in self._required_offset_arrays:









@@ -176,8 +195,14 @@ class BetweenTimestepsIndexing:













            offset_array_symbols = self._offset_array_symbols(f_dir, inv)















            symbols_defined |= set(offset_array_symbols)















            for d, arrsymb in enumerate(offset_array_symbols):













                if IS_PYSTENCILS_2:













                    array_content.append((arrsymb, offsets[d]))













                else:















                    array_content.append((self._offsets_dtype, arrsymb.name, offsets[d]))





























        if IS_PYSTENCILS_2:













            return TranslationArraysNode(array_content)













        else:















            return TranslationArraysNode(array_content, symbols_defined)































#   end class AdvancedStreamingIndexing
























src/lbmpy/boundaries/boundaries_in_kernel.py



+13
−5
















Original line number
Diff line number
Diff line















import sympy as sp





























from .._compat import IS_PYSTENCILS_2





























from lbmpy.advanced_streaming.indexing import BetweenTimestepsIndexing















from lbmpy.advanced_streaming.utility import Timestep, get_accessor













from lbmpy.custom_code_nodes import LbmWeightInfo















from pystencils.boundaries.boundaryhandling import BoundaryOffsetInfo













from pystencils.assignment import Assignment













from pystencils.astnodes import Block, Conditional, LoopOverCoordinate, SympyAssignment













from pystencils.simp.assignment_collection import AssignmentCollection













from pystencils.simp.simplifications import sympy_cse_on_assignment_list













from pystencils import Assignment













from pystencils.simp import AssignmentCollection, sympy_cse_on_assignment_list















from pystencils.stencil import inverse_direction















from pystencils.sympyextensions import fast_subs





























if IS_PYSTENCILS_2:













    from lbmpy.lookup_tables import LbmWeightInfo













else:













    from lbmpy.custom_code_nodes import LbmWeightInfo













    from pystencils.astnodes import Block, Conditional, LoopOverCoordinate, SympyAssignment  # TODO replace













































def direction_indices_in_direction(direction, stencil):















    for i, offset in enumerate(stencil):










@@ -58,6 +63,9 @@ def border_conditions(direction, field, ghost_layers=1):













































def boundary_conditional(boundary, direction, streaming_pattern, prev_timestep, lb_method, output_field, cse=False):













    if IS_PYSTENCILS_2:













        raise NotImplementedError("In-Kernel Boundaries are not yet available on pystencils 2.0")





























    stencil = lb_method.stencil































    dir_indices = direction_indices_in_direction(direction, stencil)

































src/lbmpy/boundaries/boundaryconditions.py



+72
−18
















Original line number
Diff line number
Diff line








@@ -2,21 +2,38 @@ import abc













from enum import Enum, auto















from warnings import warn





























from pystencils import Assignment, Field













from pystencils.simp.assignment_collection import AssignmentCollection













from pystencils import Assignment, AssignmentCollection, Field, TypedSymbol















from pystencils.stencil import offset_to_direction_string, direction_string_to_offset, inverse_direction















from pystencils.sympyextensions import get_symmetric_part, simplify_by_equality, scalar_product













from pystencils.typing import create_type, TypedSymbol































from lbmpy.advanced_streaming.utility import AccessPdfValues, Timestep













from lbmpy.custom_code_nodes import (NeighbourOffsetArrays, MirroredStencilDirections, LbmWeightInfo,













                                     TranslationArraysNode)















from lbmpy.maxwellian_equilibrium import discrete_equilibrium















from lbmpy.simplificationfactory import create_simplification_strategy































import sympy as sp















import numpy as np





























from .._compat import IS_PYSTENCILS_2



























if IS_PYSTENCILS_2:













    from pystencils import create_type













    from pystencils.sympyextensions.typed_sympy import CastFunc













    from pystencils.types.quick import Arr













    from lbmpy.lookup_tables import (













        NeighbourOffsetArrays,













        MirroredStencilDirections,













        LbmWeightInfo,













        TranslationArraysNode













    )













else:













    from pystencils.typing import create_type, CastFunc













    from lbmpy.custom_code_nodes import (













        NeighbourOffsetArrays,













        MirroredStencilDirections,













        LbmWeightInfo,













        TranslationArraysNode













    )













































class LbBoundary(abc.ABC):















    """Base class that all boundaries should derive from.










@@ -130,6 +147,8 @@ class NoSlip(LbBoundary):













            force = sp.Symbol("f")















            subexpressions = [Assignment(force, sp.Float(2.0) * f_out(dir_symbol))]















            offset = NeighbourOffsetArrays.neighbour_offset(dir_symbol, lb_method.stencil)













            if IS_PYSTENCILS_2:













                offset = [CastFunc.as_numeric(o) for o in offset]















            for i in range(lb_method.stencil.D):















                subexpressions.append(Assignment(force_vector[0](f'F_{i}'), force * offset[i]))















        else:










@@ -211,6 +230,8 @@ class NoSlipLinearBouzidi(LbBoundary):













            force = sp.Symbol("f")















            subexpressions.append(Assignment(force, f_xf + rhs))















            offset = NeighbourOffsetArrays.neighbour_offset(dir_symbol, lb_method.stencil)













            if IS_PYSTENCILS_2:













                offset = [CastFunc.as_numeric(o) for o in offset]















            for i in range(lb_method.stencil.D):















                subexpressions.append(Assignment(force_vector[0](f'F_{i}'), force * offset[i]))


























@@ -239,10 +260,15 @@ class QuadraticBounceBack(LbBoundary):













        self.data_type = data_type















        self.init_wall_distance = init_wall_distance















        self.equilibrium_values_name = "f_eq"













        self.inv_dir_symbol = TypedSymbol("inv_dir", create_type("int32"))































        super(QuadraticBounceBack, self).__init__(name, calculate_force_on_boundary)





























    def inv_dir_symbol(self, stencil):













        if IS_PYSTENCILS_2:













            return TypedSymbol("inv_dir", Arr(create_type("int32"), stencil.Q))













        else:













            return TypedSymbol("inv_dir", create_type("int32"))





























    @property















    def additional_data(self):















        """Used internally only. For the NoSlipLinearBouzidi boundary the distance to the obstacle of every










@@ -273,9 +299,15 @@ class QuadraticBounceBack(LbBoundary):













        """















        stencil = lb_method.stencil















        inv_directions = [str(stencil.index(inverse_direction(direction))) for direction in stencil]













        dtype = self.inv_dir_symbol.dtype













        name = self.inv_dir_symbol.name













        inverse_dir_node = TranslationArraysNode([(dtype, name, inv_directions), ], {self.inv_dir_symbol})













        













        if IS_PYSTENCILS_2:













            inverse_dir_node = TranslationArraysNode([(self.inv_dir_symbol(stencil), inv_directions), ])













        else:













            inv_dir_symbol = self.inv_dir_symbol(stencil)













            dtype = inv_dir_symbol.dtype













            name = inv_dir_symbol.name













            inverse_dir_node = TranslationArraysNode([(dtype, name, inv_directions), ], {inv_dir_symbol})













        















        return [LbmWeightInfo(lb_method, self.data_type), inverse_dir_node, NeighbourOffsetArrays(lb_method.stencil)]































    @staticmethod









@@ -293,7 +325,7 @@ class QuadraticBounceBack(LbBoundary):





























    def __call__(self, f_out, f_in, dir_symbol, inv_dir, lb_method, index_field, force_vector):















        omega = self.relaxation_rate













        inv = sp.IndexedBase(self.inv_dir_symbol, shape=(1,))[dir_symbol]













        inv = sp.IndexedBase(self.inv_dir_symbol(lb_method.stencil), shape=(1,))[dir_symbol]















        weight_info = LbmWeightInfo(lb_method, data_type=self.data_type)















        weight_of_direction = weight_info.weight_of_direction















        pdf_field_accesses = [f_out(i) for i in range(len(lb_method.stencil))]









@@ -317,13 +349,19 @@ class QuadraticBounceBack(LbBoundary):













        subexpressions.append(Assignment(weight, weight_of_direction(dir_symbol, lb_method)))















        subexpressions.append(Assignment(weight_inv, weight_of_direction(inv, lb_method)))





























        if IS_PYSTENCILS_2:













            cast_offset = CastFunc.as_numeric













        else:













            def cast_offset(x):













                return x





























        for i in range(lb_method.stencil.D):















            offset = NeighbourOffsetArrays.neighbour_offset(dir_symbol, lb_method.stencil)













            subexpressions.append(Assignment(v[i], offset[i]))













            subexpressions.append(Assignment(v[i], cast_offset(offset[i])))































        for i in range(lb_method.stencil.D):















            offset = NeighbourOffsetArrays.neighbour_offset(inv, lb_method.stencil)













            subexpressions.append(Assignment(v_inv[i], offset[i]))













            subexpressions.append(Assignment(v_inv[i], cast_offset(offset[i])))































        cqc = lb_method.conserved_quantity_computation















        rho = cqc.density_symbol









@@ -348,6 +386,8 @@ class QuadraticBounceBack(LbBoundary):













            force = sp.Symbol("f")















            subexpressions.append(Assignment(force, f_xf + result))















            offset = NeighbourOffsetArrays.neighbour_offset(dir_symbol, lb_method.stencil)













            if IS_PYSTENCILS_2:













                offset = [CastFunc.as_numeric(o) for o in offset]















            for i in range(lb_method.stencil.D):















                subexpressions.append(Assignment(force_vector[0](f'F_{i}'), force * offset[i]))


























@@ -469,7 +509,7 @@ class FreeSlip(LbBoundary):













        neighbor_offset = NeighbourOffsetArrays.neighbour_offset(dir_symbol, lb_method.stencil)















        if self.normal_direction:















            tangential_offset = tuple(offset + normal for offset, normal in zip(neighbor_offset, self.normal_direction))













            mirrored_stencil_symbol = MirroredStencilDirections._mirrored_symbol(self.mirror_axis)













            mirrored_stencil_symbol = MirroredStencilDirections._mirrored_symbol(self.mirror_axis, self.stencil)















            mirrored_direction = inv_dir[sp.IndexedBase(mirrored_stencil_symbol, shape=(1,))[dir_symbol]]















        else:















            normal_direction = list()










@@ -610,7 +650,7 @@ class WallFunctionBounce(LbBoundary):













        # neighbour offset symbols are basically the stencil directions defined in stencils.py:L130ff.















        neighbor_offset = NeighbourOffsetArrays.neighbour_offset(dir_symbol, lb_method.stencil)















        tangential_offset = tuple(offset + normal for offset, normal in zip(neighbor_offset, self.normal_direction))













        mirrored_stencil_symbol = MirroredStencilDirections._mirrored_symbol(self.mirror_axis)













        mirrored_stencil_symbol = MirroredStencilDirections._mirrored_symbol(self.mirror_axis, self.stencil)















        mirrored_direction = inv_dir[sp.IndexedBase(mirrored_stencil_symbol, shape=(1,))[dir_symbol]]































        name_base = "f_in_inv_offsets_"










@@ -696,7 +736,12 @@ class WallFunctionBounce(LbBoundary):













        if self.stencil.Q == 19:















            result.append(Assignment(weight, sp.Rational(1, 2)))















        elif self.stencil.Q == 27:













            result.append(Assignment(inv_weight_sq, sum([neighbor_offset[i]**2 for i in self.tangential_axis])))













            result.append(













                Assignment(













                    inv_weight_sq,













                    sum([CastFunc(neighbor_offset[i], self.data_type)**2 for i in self.tangential_axis])













                )













            )















            a, b = sp.symbols("wfb_a wfb_b")































            if self.weight_method == self.WeightMethod.LATTICE_WEIGHT:









@@ -712,7 +757,12 @@ class WallFunctionBounce(LbBoundary):













                                                          (res_ab[b], True))))































        factor = self.dt / self.dy * weight













        drag = sum([neighbor_offset[i] * factor * wall_stress[i] for i in self.tangential_axis])













        drag = sum(













            [













                CastFunc(neighbor_offset[i], self.data_type) * factor * wall_stress[i]













                for i in self.tangential_axis













            ]













        )































        result.append(Assignment(f_in.center(inv_dir[dir_symbol]), f_out[tangential_offset](mirrored_direction) - drag))


























@@ -792,6 +842,7 @@ class UBB(LbBoundary):













        return callable(self._velocity)































    def __call__(self, f_out, f_in, dir_symbol, inv_dir, lb_method, index_field, force_vector):













        dtype = create_type(self.data_type)















        vel_from_idx_field = callable(self._velocity)















        vel = [index_field(f'vel_{i}') for i in range(self.dim)] if vel_from_idx_field else self._velocity

























@@ -814,8 +865,11 @@ class UBB(LbBoundary):













        c_s_sq = sp.Rational(1, 3)















        weight_info = LbmWeightInfo(lb_method, data_type=self.data_type)















        weight_of_direction = weight_info.weight_of_direction













        vel_term = 2 / c_s_sq * sum([d_i * v_i for d_i, v_i in zip(neighbor_offset, velocity)]) * weight_of_direction(













            dir_symbol, lb_method)













        vel_term = (













            2 / c_s_sq













            * sum([CastFunc(d_i, dtype) * v_i for d_i, v_i in zip(neighbor_offset, velocity)]) 













            * weight_of_direction(dir_symbol, lb_method)













        )































        # Better alternative: in conserved value computation















        # rename what is currently called density to "virtual_density"

































src/lbmpy/boundaries/boundaryhandling.py



+78
−28
















Original line number
Diff line number
Diff line















from dataclasses import replace















import numpy as np





























from pystencils import Assignment, CreateKernelConfig, create_kernel, Field, Target













from pystencils import Assignment, CreateKernelConfig, create_kernel, Field, Target, FieldType















from pystencils.boundaries import BoundaryHandling















from pystencils.boundaries.createindexlist import numpy_data_type_for_boundary_object













from pystencils.field import FieldType















from pystencils.simp import add_subexpressions_for_field_reads















from pystencils.stencil import inverse_direction































from lbmpy.advanced_streaming.indexing import BetweenTimestepsIndexing















from lbmpy.advanced_streaming.utility import is_inplace, Timestep, AccessPdfValues





























from .._compat import IS_PYSTENCILS_2



























if IS_PYSTENCILS_2:













    from pystencils.types import PsNumericType













































class LatticeBoltzmannBoundaryHandling(BoundaryHandling):















    """









@@ -20,13 +24,16 @@ class LatticeBoltzmannBoundaryHandling(BoundaryHandling):













    """































    def __init__(self, lb_method, data_handling, pdf_field_name, streaming_pattern='pull',













                 name="boundary_handling", flag_interface=None, target=Target.CPU, openmp=False):













                 name="boundary_handling", flag_interface=None, target=Target.CPU, openmp=False, **kwargs):















        self._lb_method = lb_method















        self._streaming_pattern = streaming_pattern















        self._inplace = is_inplace(streaming_pattern)















        self._prev_timestep = None













        super(LatticeBoltzmannBoundaryHandling, self).__init__(data_handling, pdf_field_name, lb_method.stencil,













                                                               name, flag_interface, target, openmp)













        super(LatticeBoltzmannBoundaryHandling, self).__init__(













            data_handling, pdf_field_name, lb_method.stencil,













            name, flag_interface, target=target, openmp=openmp,













            **kwargs













        )































    #   ------------------------- Overridden methods of pystencils.BoundaryHandling -------------------------

























@@ -52,7 +59,7 @@ class LatticeBoltzmannBoundaryHandling(BoundaryHandling):





























    def _add_inplace_boundary(self, boundary_obj, flag=None):















        if boundary_obj not in self._boundary_object_to_boundary_info:













            sym_index_field = Field.create_generic('indexField', spatial_dimensions=1,













            sym_index_field = Field.create_generic('indexField', spatial_dimensions=1, field_type=FieldType.INDEXED,















                                                   dtype=numpy_data_type_for_boundary_object(boundary_obj, self.dim))































            ast_even = self._create_boundary_kernel(self._data_handling.fields[self._field_name], sym_index_field,









@@ -67,10 +74,15 @@ class LatticeBoltzmannBoundaryHandling(BoundaryHandling):













        return self._boundary_object_to_boundary_info[boundary_obj].flag































    def _create_boundary_kernel(self, symbolic_field, symbolic_index_field, boundary_obj, prev_timestep=Timestep.BOTH):













        if IS_PYSTENCILS_2:













            additional_args = {"default_dtype": self._default_dtype}













        else:













            additional_args = dict()













            















        return create_lattice_boltzmann_boundary_kernel(















            symbolic_field, symbolic_index_field, self._lb_method, boundary_obj,















            prev_timestep=prev_timestep, streaming_pattern=self._streaming_pattern,













            target=self._target, cpu_openmp=self._openmp)













            target=self._target, cpu_openmp=self._openmp, **additional_args)































    class InplaceStreamingBoundaryInfo(object):


























@@ -159,6 +171,7 @@ class LatticeBoltzmannBoundaryHandling(BoundaryHandling):













def create_lattice_boltzmann_boundary_kernel(pdf_field, index_field, lb_method, boundary_functor,















                                             prev_timestep=Timestep.BOTH, streaming_pattern='pull',















                                             target=Target.CPU, force_vector=None, **kernel_creation_args):













    from .._compat import IS_PYSTENCILS_2































    indexing = BetweenTimestepsIndexing(















        pdf_field, lb_method.stencil, prev_timestep, streaming_pattern, np.int32, np.int32)









@@ -168,7 +181,44 @@ def create_lattice_boltzmann_boundary_kernel(pdf_field, index_field, lb_method,













    dir_symbol = indexing.dir_symbol















    inv_dir = indexing.inverse_dir_symbol





























    config = CreateKernelConfig(target=target, default_number_int="int32",













    if IS_PYSTENCILS_2:













        from pystencils.types.quick import SInt













        config = CreateKernelConfig(













            index_field=index_field,













            target=target,













            index_dtype=SInt(32),













            skip_independence_check=True,













            **kernel_creation_args













        )



























        default_data_type: PsNumericType = config.get_option("default_dtype")



























        if force_vector is None:













            force_vector_type = np.dtype([(f"F_{i}", default_data_type.numpy_dtype) for i in range(dim)], align=True)













            force_vector = Field.create_generic('force_vector', spatial_dimensions=1,













                                                dtype=force_vector_type, field_type=FieldType.INDEXED)



























        boundary_assignments = boundary_functor(f_out, f_in, dir_symbol, inv_dir, lb_method, index_field, force_vector)













        boundary_assignments = indexing.substitute_proxies(boundary_assignments)



























        if pdf_field.dtype != default_data_type:













            boundary_assignments = add_subexpressions_for_field_reads(boundary_assignments, data_type=default_data_type)



























        elements: list[Assignment] = []



























        index_arrs_node = indexing.create_code_node()













        elements += index_arrs_node.get_array_declarations()













        













        for node in boundary_functor.get_additional_code_nodes(lb_method)[::-1]:













            elements += node.get_array_declarations()













            













        elements += [Assignment(dir_symbol, index_field[0]('dir'))]













        elements += boundary_assignments.all_assignments



























        kernel = create_kernel(elements, config=config)













        return kernel













    else:













        config = CreateKernelConfig(index_fields=[index_field], target=target, default_number_int="int32",















                                    skip_independence_check=True, **kernel_creation_args)































        default_data_type = config.data_type.default_factory()

































src/lbmpy/boundaries/wall_function_models.py



+1
−1
















Original line number
Diff line number
Diff line








@@ -157,7 +157,7 @@ class MuskerLaw(ImplicitWallFunctionModel):













        def law(u_p, y_p):















            arctan = sp.Float(5.424) * sp.atan(sp.Float(0.119760479041916168) * y_p - sp.Float(0.488023952095808383))















            logarithm = (sp.Float(0.434) * sp.log((y_p + sp.Float(10.6)) ** sp.Float(9.6)













                                                  / (y_p ** 2 - sp.Float(8.15) * y_p + sp.Float(86)) ** 2, 10))













                                                  / (y_p ** 2 - sp.Float(8.15) * y_p + sp.Float(86)) ** 2))















            return (arctan + logarithm - sp.Float(3.50727901936264842)) - u_p































        u_plus = velocity_symbol / self.u_tau[0]

































src/lbmpy/creationfunctions.py



+65
−62
















Original line number
Diff line number
Diff line








@@ -58,16 +58,16 @@ from dataclasses import dataclass, field, replace













from typing import Union, List, Tuple, Any, Type, Iterable















from warnings import warn, filterwarnings





























import lbmpy.moment_transforms













import pystencils.astnodes













from ._compat import IS_PYSTENCILS_2





























import sympy as sp













import sympy.core.numbers































from lbmpy.enums import Stencil, Method, ForceModel, CollisionSpace, SubgridScaleModel















import lbmpy.forcemodels as forcemodels















from lbmpy.fieldaccess import CollideOnlyInplaceAccessor, PdfFieldAccessor, PeriodicTwoFieldsAccessor















from lbmpy.fluctuatinglb import add_fluctuations_to_collision_rule













from lbmpy.partially_saturated_cells import add_psm_to_collision_rule, PSMConfig













from lbmpy.partially_saturated_cells import (replace_by_psm_collision_rule, PSMConfig,













                                             add_psm_solid_collision_to_collision_rule)















from lbmpy.non_newtonian_models import add_cassons_model, CassonsParameters















from lbmpy.methods import (create_mrt_orthogonal, create_mrt_raw, create_central_moment,















                           create_srt, create_trt, create_trt_kbc)









@@ -81,17 +81,22 @@ from lbmpy.stencils import LBStencil













from lbmpy.turbulence_models import add_sgs_model















from lbmpy.updatekernels import create_lbm_kernel, create_stream_pull_with_output_kernel















from lbmpy.advanced_streaming.utility import Timestep, get_accessor













from .forcemodels import AbstractForceModel



























import pystencils















from pystencils import CreateKernelConfig, create_kernel













from pystencils.astnodes import Conditional, Block















from pystencils.cache import disk_cache_no_fallback













from pystencils.node_collection import NodeCollection













from pystencils.typing import collate_types















from pystencils.field import Field















from pystencils.simp import sympy_cse, SimplificationStrategy















# needed for the docstring















from lbmpy.methods.abstractlbmethod import LbmCollisionRule, AbstractLbMethod















from lbmpy.methods.cumulantbased import CumulantBasedLbMethod





























if IS_PYSTENCILS_2:













    from pystencils import Kernel as KernelFunction













else:













    from pystencils.astnodes import KernelFunction





























# Filter out JobLib warnings. They are not useful for use:















# https://github.com/joblib/joblib/issues/683















filterwarnings("ignore", message="Persisting input arguments took")









@@ -102,7 +107,7 @@ class LBMConfig:













    """















    **Below all parameters for the LBMConfig are explained**















    """













    stencil: lbmpy.stencils.LBStencil = LBStencil(Stencil.D2Q9)













    stencil: LBStencil = LBStencil(Stencil.D2Q9)















    """















    All stencils are defined in :class:`lbmpy.enums.Stencil`. From that :class:`lbmpy.stencils.LBStencil` 















    class will be created










@@ -161,7 +166,7 @@ class LBMConfig:













    truncated. Order 2 is sufficient to approximate Navier-Stokes. This parameter has no effect on cumulant-based















    methods, whose equilibrium terms have no contributions above order one.















    """













    c_s_sq: sympy.Rational = sp.Rational(1, 3)













    c_s_sq: sp.Expr = sp.Rational(1, 3)















    """















    The squared lattice speed of sound used to derive the LB method. It is very uncommon to use a value different 















    to 1 / 3.









@@ -178,7 +183,7 @@ class LBMConfig:













    If this argument is not provided, Gram-Schmidt orthogonalisation of the default modes is performed.















    """





























    force_model: Union[lbmpy.forcemodels.AbstractForceModel, ForceModel] = None













    force_model: Union[AbstractForceModel, ForceModel] = None















    """















    Force model to determine how forcing terms enter the collision rule.















    Possibilities are defined in :class: `lbmpy.enums.ForceModel`










@@ -338,9 +343,9 @@ class LBMConfig:













    Instance of :class:`lbmpy.methods.LbmCollisionRule`. If this parameter is `None`,















    the update rule is derived via *create_lb_update_rule*.















    """













    ast: pystencils.astnodes.KernelFunction = None













    ast: KernelFunction = None















    """













    Instance of *pystencils.astnodes.KernelFunction*. If this parameter is `None`,













    Instance of *pystencils.KernelFunction*. If this parameter is `None`,















    the ast is derived via `create_lb_ast`.















    """


























@@ -376,8 +381,8 @@ class LBMConfig:













        if not self.compressible and self.method in (Method.MONOMIAL_CUMULANT, Method.CUMULANT):















            raise ValueError("Incompressible cumulant-based methods are not supported (yet).")





























        if self.zero_centered and (self.entropic or self.fluctuating):













            raise ValueError("Entropic and fluctuating methods can only be created with `zero_centered=False`.")













        if self.zero_centered and self.entropic:













            raise ValueError("Entropic methods can only be created with `zero_centered=False`.")































        #   Check or infer delta-equilibrium















        if self.delta_equilibrium is not None:










@@ -468,7 +473,7 @@ class LBMConfig:













        }































        if self.psm_config is not None and self.psm_config.fraction_field is not None:













            self.force = [(1.0 - self.psm_config.fraction_field.center) * f for f in self.force]













            self.force = [(1.0 - self.psm_config.fraction_field_symbol) * f for f in self.force]































        if isinstance(self.force_model, str):















            new_force_model = ForceModel[self.force_model.upper()]










@@ -555,7 +560,6 @@ def create_lb_function(ast=None, lbm_config=None, lbm_optimisation=None, config=





























    res.method = ast.method















    res.update_rule = ast.update_rule













    res.ast = ast















    return res









































@@ -571,9 +575,7 @@ def create_lb_ast(update_rule=None, lbm_config=None, lbm_optimisation=None, conf













        update_rule = create_lb_update_rule(lbm_config.collision_rule, lbm_config=lbm_config,















                                            lbm_optimisation=lbm_optimisation, config=config)





























    field_types = set(fa.field.dtype for fa in update_rule.defined_symbols if isinstance(fa, Field.Access))



























    config = replace(config, data_type=collate_types(field_types), ghost_layers=1)













    config = replace(config, ghost_layers=1)















    ast = create_kernel(update_rule, config=config)































    ast.method = update_rule.method









@@ -599,7 +601,11 @@ def create_lb_update_rule(collision_rule=None, lbm_config=None, lbm_optimisation





























    lb_method = collision_rule.method





























    field_data_type = config.data_type[lbm_config.field_name].numpy_dtype













    if IS_PYSTENCILS_2:













        fallback_field_data_type = config.get_option("default_dtype")













    else:













        fallback_field_data_type = config.data_type[lbm_config.field_name].numpy_dtype





























    q = collision_rule.method.stencil.Q































    if lbm_optimisation.symbolic_field is not None:









@@ -607,10 +613,11 @@ def create_lb_update_rule(collision_rule=None, lbm_config=None, lbm_optimisation













    elif lbm_optimisation.field_size:















        field_size = tuple([s + 2 for s in lbm_optimisation.field_size] + [q])















        src_field = Field.create_fixed_size(lbm_config.field_name, field_size, index_dimensions=1,













                                            layout=lbm_optimisation.field_layout, dtype=field_data_type)













                                            layout=lbm_optimisation.field_layout, dtype=fallback_field_data_type)















    else:















        src_field = Field.create_generic(lbm_config.field_name, spatial_dimensions=collision_rule.method.dim,













                                         index_shape=(q,), layout=lbm_optimisation.field_layout, dtype=field_data_type)













                                         index_shape=(q,), layout=lbm_optimisation.field_layout,













                                         dtype=fallback_field_data_type)































    if lbm_optimisation.symbolic_temporary_field is not None:















        dst_field = lbm_optimisation.symbolic_temporary_field










@@ -684,11 +691,6 @@ def create_lb_collision_rule(lb_method=None, lbm_config=None, lbm_optimisation=N













    else:















        collision_rule = lb_method.get_collision_rule(pre_simplification=pre_simplification)





























    if lbm_config.psm_config is not None:













        if lbm_config.psm_config.fraction_field is None or lbm_config.psm_config.object_velocity_field is None:













            raise ValueError("Specify a fraction and object velocity field in the PSM Config")













        collision_rule = add_psm_to_collision_rule(collision_rule, lbm_config.psm_config)





























    if lbm_config.galilean_correction:















        from lbmpy.methods.cumulantbased import add_galilean_correction















        collision_rule = add_galilean_correction(collision_rule)









@@ -706,6 +708,11 @@ def create_lb_collision_rule(lb_method=None, lbm_config=None, lbm_optimisation=N













                                                     bulk_relaxation_rate=lbm_config.relaxation_rates[1],















                                                     limiter=cumulant_limiter)





























    if lbm_config.psm_config is not None:













        if lbm_config.psm_config.fraction_field is None or lbm_config.psm_config.object_velocity_field is None:













            raise ValueError("Specify a fraction and object velocity field in the PSM Config")













        collision_rule = replace_by_psm_collision_rule(collision_rule, lbm_config.psm_config)





























    if lbm_config.entropic:















        if lbm_config.subgrid_scale_model or lbm_config.cassons:















            raise ValueError("Choose either entropic, subgrid-scale or cassons")










@@ -783,7 +790,7 @@ def create_lb_method(lbm_config=None, **params):













    if lbm_config.psm_config is None:















        fraction_field = None















    else:













        fraction_field = lbm_config.psm_config.fraction_field













        fraction_field = lbm_config.psm_config.fraction_field_symbol































    common_params = {















        'compressible': lbm_config.compressible,










@@ -869,46 +876,42 @@ def create_lb_method(lbm_config=None, **params):













































def create_psm_update_rule(lbm_config, lbm_optimisation):













    node_collection = []













    if IS_PYSTENCILS_2:













        raise NotImplementedError(













            "`create_psm_update_rule` is not yet available when using pystencils 2.0. "













            "To instead derive a (potentially less efficient) PSM kernel without branches, "













            "use `create_lb_update_rule` with a `PsmConfig` object instead."













        )













    













    from pystencils.astnodes import Conditional, Block













    from pystencils.node_collection import NodeCollection



























    if lbm_config.psm_config is None:













        raise ValueError("Specify a PSM Config in the LBM Config, when creating a psm update rule")



























    config_without_particles = copy.deepcopy(lbm_config)













    config_without_particles.psm_config.max_particles_per_cell = 0





























    # Use regular lb update rule for no overlapping particles













    config_without_psm = copy.deepcopy(lbm_config)













    config_without_psm.psm_config = None













    # TODO: the force is still multiplied by (1.0 - self.psm_config.fraction_field.center)













    #  (should not harm if memory bound since self.psm_config.fraction_field.center should always be 0.0)















    lb_update_rule = create_lb_update_rule(













        lbm_config=config_without_psm, lbm_optimisation=lbm_optimisation













    )













    node_collection.append(













        Conditional(













            lbm_config.psm_config.fraction_field.center(0) <= 0.0,













            Block(lb_update_rule.all_assignments),













        )













    )













        lbm_config=config_without_particles, lbm_optimisation=lbm_optimisation)



























    node_collection = lb_update_rule.all_assignments





























    # Only one particle, i.e., no individual_fraction_field is provided















    if lbm_config.psm_config.individual_fraction_field is None:













        assert lbm_config.psm_config.MaxParticlesPerCell == 1













        psm_update_rule = create_lb_update_rule(













            lbm_config=lbm_config, lbm_optimisation=lbm_optimisation













        )













        node_collection.append(













            Conditional(













                lbm_config.psm_config.fraction_field.center(0) > 0.0,













                Block(psm_update_rule.all_assignments),













            )













        )













        assert lbm_config.psm_config.max_particles_per_cell == 1













        fraction_field = lbm_config.psm_config.fraction_field















    else:













        for p in range(lbm_config.psm_config.MaxParticlesPerCell):













            # Add psm update rule for p overlapping particles













            config_with_p_particles = copy.deepcopy(lbm_config)













            config_with_p_particles.psm_config.MaxParticlesPerCell = p + 1













        fraction_field = lbm_config.psm_config.individual_fraction_field



























    for p in range(lbm_config.psm_config.max_particles_per_cell):



























        psm_solid_collision = add_psm_solid_collision_to_collision_rule(lb_update_rule, lbm_config, p)















        psm_update_rule = create_lb_update_rule(













                lbm_config=config_with_p_particles, lbm_optimisation=lbm_optimisation













            )













            collision_rule=psm_solid_collision, lbm_config=lbm_config, lbm_optimisation=lbm_optimisation)





























        node_collection.append(















            Conditional(













                    lbm_config.psm_config.individual_fraction_field.center(p) > 0.0,













                fraction_field.center(p) > 0.0,















                Block(psm_update_rule.all_assignments),















            )















        )

































src/lbmpy/custom_code_nodes.py



+8
−3
















Original line number
Diff line number
Diff line















import numpy as np















import sympy as sp





























from ._compat import IS_PYSTENCILS_2



























if IS_PYSTENCILS_2:













    raise ImportError("`lbmpy.custom_code_nodes` is only available when running with pystencils 1.x")





























from pystencils.typing import TypedSymbol, create_type















from pystencils.backends.cbackend import CustomCodeNode


























@@ -44,14 +49,14 @@ class MirroredStencilDirections(CustomCodeNode):













        return tuple(direction)































    @staticmethod













    def _mirrored_symbol(mirror_axis):













    def _mirrored_symbol(mirror_axis, _stencil):















        axis = ['x', 'y', 'z']















        return TypedSymbol(f"{axis[mirror_axis]}_axis_mirrored_stencil_dir", create_type('int32'))































    def __init__(self, stencil, mirror_axis, dtype=np.int32):















        offsets_dtype = create_type(dtype)





























        mirrored_stencil_symbol = MirroredStencilDirections._mirrored_symbol(mirror_axis)













        mirrored_stencil_symbol = MirroredStencilDirections._mirrored_symbol(mirror_axis, stencil)















        mirrored_directions = [stencil.index(MirroredStencilDirections.mirror_stencil(direction, mirror_axis))















                               for direction in stencil]















        code = "\n"

































src/lbmpy/fieldaccess.py



+3
−2
















Original line number
Diff line number
Diff line








@@ -4,11 +4,12 @@ import sympy as sp





























from pystencils import Field















# ------------------------------------------------ Interface -----------------------------------------------------------













from pystencils.astnodes import LoopOverCoordinate





























from pystencils.stencil import inverse_direction































from lbmpy.enums import Stencil















from lbmpy.stencils import LBStencil













from ._compat import get_loop_counter_symbol































__all__ = ['PdfFieldAccessor', 'CollideOnlyInplaceAccessor', 'StreamPullTwoFieldsAccessor',















           'AAEvenTimeStepAccessor', 'AAOddTimeStepAccessor',










@@ -114,7 +115,7 @@ class PeriodicTwoFieldsAccessor(PdfFieldAccessor):













                lower_limit = self._ghostLayers















                upper_limit = field.spatial_shape[coord_id] - 1 - self._ghostLayers















                limit_diff = upper_limit - lower_limit













                loop_counter = LoopOverCoordinate.get_loop_counter_symbol(coord_id)













                loop_counter = get_loop_counter_symbol(coord_id)















                if dir_element == 0:















                    periodic_pull_direction.append(0)















                elif dir_element == 1:

































src/lbmpy/fluctuatinglb.py



+60
−14
















Original line number
Diff line number
Diff line








@@ -3,36 +3,84 @@













to generate a fluctuating LBM the equilibrium moment values have to be scaled and an additive (random)















correction term is added to the collision rule















"""













from typing import overload



























from ._compat import IS_PYSTENCILS_2





























import numpy as np















import sympy as sp































from lbmpy.moments import MOMENT_SYMBOLS, is_shear_moment, get_order















from lbmpy.equilibrium import ContinuousHydrodynamicMaxwellian















from pystencils import Assignment, TypedSymbol













from pystencils.rng import PhiloxFourFloats, random_symbol















from pystencils.simp.assignment_collection import SymbolGen





























if IS_PYSTENCILS_2:













    from pystencils.sympyextensions.random import RngBase, Philox













    from pystencils.sympyextensions import tcast













else:













    from pystencils.rng import PhiloxFourFloats, random_symbol











































@overload















def add_fluctuations_to_collision_rule(collision_rule, temperature=None, amplitudes=(),













                                       block_offsets=(0, 0, 0), seed=TypedSymbol("seed", np.uint32),













                                       rng_node=PhiloxFourFloats, c_s_sq=sp.Rational(1, 3)):













    """"""













                                       *,













                                       block_offsets, seed, rng_node, c_s_sq):













    """Fluctuating LB implementation for pystencils 1.3"""









































@overload













def add_fluctuations_to_collision_rule(collision_rule, temperature=None, amplitudes=(),













                                       *,













                                       rng: 'RngBase | None' = None, c_s_sq):













    """Fluctuating LB implementation for pystencils 2.0













    













    Args:













        collision_rule: The base collision rule













        temperature: Expression representing the fluid temperature













        amplitudes: If ``temperature`` was not specified, expression representing the fluctuation amplitude













        rng: Random number generator instance used to compute the fluctuations.













            If `None`, the float32 Philox RNG will be used.













    """









































def add_fluctuations_to_collision_rule(collision_rule, temperature=None, amplitudes=(),













                                       c_s_sq=sp.Rational(1, 3), **kwargs):















    if not (temperature and not amplitudes) or (temperature and amplitudes):















        raise ValueError("Fluctuating LBM: Pass either 'temperature' or 'amplitudes'.")













    if collision_rule.method.conserved_quantity_computation.zero_centered_pdfs:













        raise ValueError("The fluctuating LBM is not implemented for zero-centered PDF storage.")















    















    method = collision_rule.method















    if not amplitudes:















        amplitudes = fluctuation_amplitude_from_temperature(method, temperature, c_s_sq)













    if block_offsets == 'walberla':













        block_offsets = tuple(TypedSymbol("block_offset_{}".format(i), np.uint32) for i in range(3))































    if not method.is_weighted_orthogonal:















        raise ValueError("Fluctuations can only be added to weighted-orthogonal methods")





























    rng_symbol_gen = random_symbol(collision_rule.subexpressions, seed=seed,













                                   rng_node=rng_node, dim=method.dim, offsets=block_offsets)













    if IS_PYSTENCILS_2:













        rng: RngBase = kwargs.get("rng", Philox("fluctuation_rng", np.float32, TypedSymbol("seed", np.uint32)))













        ts = TypedSymbol("time_step", np.uint32)



























        def _rng_symbol_gen():













            while True:













                rx, rasm = rng.get_random_vector(ts)













                collision_rule.subexpressions.insert(0, rasm)













                for i in range(rng.vector_size):













                    yield tcast.as_numeric(rx[i])



























        rng_symbol_gen = _rng_symbol_gen()













    else:













        block_offsets = kwargs.get("block_offsets", (0, 0, 0))













        rng_node = kwargs.get("rng_node", PhiloxFourFloats)













        seed = kwargs.get("seed", TypedSymbol("seed", np.uint32))



























        if block_offsets == 'walberla':













            block_offsets = tuple(TypedSymbol("block_offset_{}".format(i), np.uint32) for i in range(3))



























        rng_symbol_gen = random_symbol(













            collision_rule.subexpressions, seed=seed,













            rng_node=rng_node, dim=method.dim, offsets=block_offsets













        )





























    correction = fluctuation_correction(method, rng_symbol_gen, amplitudes)































    for i, corr in enumerate(correction):









@@ -44,9 +92,7 @@ def fluctuation_amplitude_from_temperature(method, temperature, c_s_sq=sp.Symbol













    """Produces amplitude equations according to (2.60) and (3.54) in Schiller08"""















    normalization_factors = sp.matrix_multiply_elementwise(method.moment_matrix, method.moment_matrix) * \















        sp.Matrix(method.weights)













    density = method.zeroth_order_equilibrium_moment_symbol













    if method.conserved_quantity_computation.zero_centered_pdfs:













        density += 1













    density = method._cqc.density_symbol















    mu = temperature * density / c_s_sq















    return [sp.sqrt(mu * norm * (1 - (1 - rr) ** 2))















            for norm, rr in zip(normalization_factors, method.relaxation_rates)]

































src/lbmpy/lbstep.py



+50
−14
















Original line number
Diff line number
Diff line








@@ -10,11 +10,18 @@ from lbmpy.macroscopic_value_kernels import (













    create_advanced_velocity_setter_collision_rule, pdf_initialization_assignments)















from lbmpy.simplificationfactory import create_simplification_strategy















from lbmpy.stencils import LBStencil













from pystencils import create_data_handling, create_kernel, make_slice, Target, Backend



























from pystencils import CreateKernelConfig













from pystencils import create_data_handling, create_kernel, make_slice, Target















from pystencils.slicing import SlicedGetter















from pystencils.timeloop import TimeLoop













































from ._compat import IS_PYSTENCILS_2













if not IS_PYSTENCILS_2:













    from pystencils import Backend











































class LatticeBoltzmannStep:































    def __init__(self, domain_size=None, lbm_kernel=None, periodicity=False,









@@ -24,7 +31,9 @@ class LatticeBoltzmannStep:













                 velocity_input_array_name=None, time_step_order='stream_collide', flag_interface=None,















                 alignment_if_vectorized=64, fixed_loop_sizes=True,















                 timeloop_creation_function=TimeLoop,













                 lbm_config=None, lbm_optimisation=None, config=None, **method_parameters):













                 lbm_config=None, lbm_optimisation=None,













                 config: CreateKernelConfig | None = None,













                 **method_parameters):































        if optimization is None:















            optimization = {}









@@ -36,6 +45,9 @@ class LatticeBoltzmannStep:













                raise ValueError("When passing a data_handling, the domain_size parameter can not be specified")































        if config is not None:













            if IS_PYSTENCILS_2:













                target = config.get_target()













            else:















                target = config.target















        else:















            target = optimization.get('target', Target.CPU)









@@ -60,6 +72,10 @@ class LatticeBoltzmannStep:













                                                                              lbm_config, lbm_optimisation, config)































        # the parallel datahandling understands only numpy datatypes. Strings lead to an errors













        if IS_PYSTENCILS_2:













            from pystencils import create_type













            field_dtype = create_type(config.get_option("default_dtype")).numpy_dtype













        else:















            field_dtype = config.data_type.default_factory().numpy_dtype































        if lbm_kernel:









@@ -75,10 +91,19 @@ class LatticeBoltzmannStep:













        self.density_data_name = name + "_density" if density_data_name is None else density_data_name















        self.density_data_index = density_data_index





























        if IS_PYSTENCILS_2:













            self._gpu = target.is_gpu()













        else:















            self._gpu = target == Target.GPU





























        layout = lbm_optimisation.field_layout































        alignment = False



























        if IS_PYSTENCILS_2:













            if config.get_target().is_vector_cpu() and config.cpu.vectorize.enable:













                alignment = alignment_if_vectorized













        else:















            if config.backend == Backend.C and config.cpu_vectorize_info:















                alignment = alignment_if_vectorized


























@@ -150,10 +175,14 @@ class LatticeBoltzmannStep:













        self._sync_tmp = data_handling.synchronization_function([self._tmp_arr_name], stencil_name, target,















                                                                stencil_restricted=True)





























        self._boundary_handling = LatticeBoltzmannBoundaryHandling(self.method, self._data_handling, self._pdf_arr_name,













        self._boundary_handling = LatticeBoltzmannBoundaryHandling(













            self.method, self._data_handling, self._pdf_arr_name,















            name=name + "_boundary_handling",















            flag_interface=flag_interface,













                                                                   target=target, openmp=config.cpu_openmp)













            target=target,













            openmp=config.cpu_openmp,













            **({"default_dtype": field_dtype} if IS_PYSTENCILS_2 else dict())













        )































        self._lbm_config = lbm_config















        self._lbm_optimisation = lbm_optimisation










@@ -223,7 +252,7 @@ class LatticeBoltzmannStep:













    @property















    def config(self):















        """Configutation of pystencils parameters"""













        return self.config













        return self._config































    def _get_slice(self, data_name, slice_obj, masked):















        if slice_obj is None:










@@ -439,12 +468,19 @@ class LatticeBoltzmannStep:













        rho_field = rho_field.center if self.density_data_index is None else rho_field(self.density_data_index)















        vel_field = self._data_handling.fields[self.velocity_data_name]





























        if IS_PYSTENCILS_2:













            gen_config = CreateKernelConfig(target=Target.CPU)













            gen_config.cpu.openmp.enable = self._config.cpu.openmp.get_option("enable")













            gen_config.default_dtype = self._config.get_option("default_dtype")













        else:













            gen_config = CreateKernelConfig(target=Target.CPU, cpu_openmp=self._config.cpu_openmp)





























        getter_eqs = cqc.output_equations_from_pdfs(pdf_field.center_vector,















                                                    {'density': rho_field, 'velocity': vel_field})













        getter_kernel = create_kernel(getter_eqs, target=Target.CPU, cpu_openmp=self._config.cpu_openmp).compile()













        getter_kernel = create_kernel(getter_eqs, config=gen_config).compile()































        setter_eqs = pdf_initialization_assignments(lb_method, rho_field,















                                                    vel_field.center_vector, pdf_field.center_vector)















        setter_eqs = create_simplification_strategy(lb_method)(setter_eqs)













        setter_kernel = create_kernel(setter_eqs, target=Target.CPU, cpu_openmp=self._config.cpu_openmp).compile()













        setter_kernel = create_kernel(setter_eqs, config=gen_config).compile()















        return getter_kernel, setter_kernel
























src/lbmpy/lookup_tables.py
0 → 100644



+128
−0
















Original line number
Diff line number
Diff line













from typing import Sequence, Any













from abc import ABC, abstractmethod













import numpy as np













import sympy as sp



























from ._compat import IS_PYSTENCILS_2



























if not IS_PYSTENCILS_2:













    raise ImportError("`lbmpy.lookup_tables` is only available when running with pystencils 2.x")



























from pystencils import Assignment













from pystencils.sympyextensions import TypedSymbol













from pystencils.types.quick import Arr













from pystencils.types import UserTypeSpec, create_type









































class LookupTables(ABC):













    @abstractmethod













    def get_array_declarations(self) -> list[Assignment]:













        pass









































class NeighbourOffsetArrays(LookupTables):



























    @staticmethod













    def neighbour_offset(dir_idx, stencil):













        if isinstance(sp.sympify(dir_idx), sp.Integer):













            return stencil[dir_idx]













        else:













            return tuple(













                [













                    sp.IndexedBase(symbol, shape=(1,))[dir_idx]













                    for symbol in NeighbourOffsetArrays._offset_symbols(stencil)













                ]













            )



























    @staticmethod













    def _offset_symbols(stencil):













        q = len(stencil)













        dim = len(stencil[0])













        return [













            TypedSymbol(f"neighbour_offset_{d}", Arr(create_type("int32"), q))













            for d in ["x", "y", "z"][:dim]













        ]



























    def __init__(self, stencil, offsets_dtype: UserTypeSpec = np.int32):













        self._offsets_dtype = create_type(













            offsets_dtype













        )  # TODO: Currently, this has no effect













        self._stencil = stencil













        self._dim = len(stencil[0])



























    def get_array_declarations(self) -> list[Assignment]:













        array_symbols = NeighbourOffsetArrays._offset_symbols(self._stencil)













        return [













            Assignment(arrsymb, tuple((d[i] for d in self._stencil)))













            for i, arrsymb in enumerate(array_symbols)













        ]









































class MirroredStencilDirections(LookupTables):



























    @staticmethod













    def mirror_stencil(direction, mirror_axis):













        assert mirror_axis <= len(













            direction













        ), f"only {len(direction)} axis available for mirage"













        direction = list(direction)













        direction[mirror_axis] = -direction[mirror_axis]



























        return tuple(direction)



























    @staticmethod













    def _mirrored_symbol(mirror_axis, stencil):













        axis = ["x", "y", "z"]













        q = len(stencil)













        return TypedSymbol(













            f"{axis[mirror_axis]}_axis_mirrored_stencil_dir", Arr(create_type("int32"), q)













        )



























    def __init__(self, stencil, mirror_axis, dtype=np.int32):













        self._offsets_dtype = create_type(dtype)  # TODO: Currently, this has no effect



























        self._mirrored_stencil_symbol = MirroredStencilDirections._mirrored_symbol(













            mirror_axis, stencil













        )













        self._mirrored_directions = tuple(













            stencil.index(













                MirroredStencilDirections.mirror_stencil(direction, mirror_axis)













            )













            for direction in stencil













        )



























    def get_array_declarations(self) -> list[Assignment]:













        return [Assignment(self._mirrored_stencil_symbol, self._mirrored_directions)]









































class LbmWeightInfo(LookupTables):













    def __init__(self, lb_method, data_type="double"):













        self._weights = lb_method.weights













        self._weights_array = TypedSymbol("weights", Arr(create_type(data_type), len(self._weights)))



























    def weight_of_direction(self, dir_idx, lb_method=None):













        if isinstance(sp.sympify(dir_idx), sp.Integer):













            assert lb_method is not None













            return lb_method.weights[dir_idx].evalf(17)













        else:













            return sp.IndexedBase(self._weights_array, shape=(1,))[dir_idx]



























    def get_array_declarations(self) -> list[Assignment]:













        return [Assignment(self._weights_array, tuple(self._weights))]









































class TranslationArraysNode(LookupTables):



























    def __init__(self, array_content: Sequence[tuple[TypedSymbol, Sequence[Any]]]):













        self._decls = [













            Assignment(symb, tuple(content)) for symb, content in array_content













        ]



























    def __str__(self):













        return "Variable PDF Access Translation Arrays"



























    def __repr__(self):













        return "Variable PDF Access Translation Arrays"



























    def get_array_declarations(self) -> list[Assignment]:













        return self._decls
























src/lbmpy/macroscopic_value_kernels.py



+57
−4
















Original line number
Diff line number
Diff line








@@ -4,7 +4,7 @@ from copy import deepcopy













from lbmpy.simplificationfactory import create_simplification_strategy















from pystencils import create_kernel, CreateKernelConfig, Assignment















from pystencils.field import Field, get_layout_of_array













from pystencils.enums import Target













from pystencils import Target































from lbmpy.advanced_streaming.utility import get_accessor, Timestep















from lbmpy.relaxationrates import get_shear_relaxation_rate









@@ -26,7 +26,14 @@ def get_field_accesses(lb_method, pdfs, streaming_pattern, previous_timestep, pr













    return field_accesses













































def pdf_initialization_assignments(lb_method, density, velocity, pdfs,













def get_individual_or_common_fraction_field(psm_config):













    if psm_config.individual_fraction_field is not None:













        return psm_config.individual_fraction_field













    else:













        return psm_config.fraction_field









































def pdf_initialization_assignments(lb_method, density, velocity, pdfs, psm_config=None,















                                   streaming_pattern='pull', previous_timestep=Timestep.BOTH,















                                   set_pre_collision_pdfs=False):















    """Assignments to initialize the pdf field with equilibrium"""









@@ -42,10 +49,35 @@ def pdf_initialization_assignments(lb_method, density, velocity, pdfs,













    setter_eqs = lb_method.get_equilibrium(conserved_quantity_equations=inp_eqs)















    setter_eqs = setter_eqs.new_with_substitutions({sym: field_accesses[i]















                                                    for i, sym in enumerate(lb_method.post_collision_pdf_symbols)})



























    if lb_method.fraction_field is not None:













        if psm_config is None:













            raise ValueError("If setting up LBM with PSM, please specify a PSM config in the macroscopic setter")













        else:













            for equ in setter_eqs:













                if equ.lhs in lb_method.first_order_equilibrium_moment_symbols:













                    pos = lb_method.first_order_equilibrium_moment_symbols.index(equ.lhs)













                    new_rhs = 0













                    if isinstance(equ.rhs, sp.core.Add):













                        for summand in equ.rhs.args:













                            if summand in velocity:













                                new_rhs += (1.0 - psm_config.fraction_field.center) * summand













                            else:













                                new_rhs += summand.subs(lb_method.fraction_field, psm_config.fraction_field.center)













                    else:













                        new_rhs += (1.0 - psm_config.fraction_field.center) * equ.rhs



























                    fraction_field = get_individual_or_common_fraction_field(psm_config)













                    for p in range(psm_config.max_particles_per_cell):













                        new_rhs += psm_config.object_velocity_field(p * lb_method.dim + pos) * fraction_field.center(p)



























                    setter_eqs.subexpressions.remove(equ)













                    setter_eqs.subexpressions.append(Assignment(equ.lhs, new_rhs))





























    return setter_eqs













































def macroscopic_values_getter(lb_method, density, velocity, pdfs,













def macroscopic_values_getter(lb_method, density, velocity, pdfs, psm_config=None,















                              streaming_pattern='pull', previous_timestep=Timestep.BOTH,















                              use_pre_collision_pdfs=False):

























@@ -58,7 +90,28 @@ def macroscopic_values_getter(lb_method, density, velocity, pdfs,













        output_spec['velocity'] = velocity















    if density is not None:















        output_spec['density'] = density













    return cqc.output_equations_from_pdfs(field_accesses, output_spec)













    getter_equ = cqc.output_equations_from_pdfs(field_accesses, output_spec)



























    if lb_method.fraction_field is not None:













        if psm_config.fraction_field is None:













            raise ValueError("If setting up LBM with PSM, please specify a PSM config in the macroscopic getter")













        else:













            if lb_method.force_model is not None:













                for equ in getter_equ:













                    if equ.lhs in lb_method.force_model.symbolic_force_vector:













                        new_rhs = equ.rhs.subs(lb_method.fraction_field, psm_config.fraction_field.center)













                        getter_equ.subexpressions.remove(equ)













                        getter_equ.subexpressions.append(Assignment(equ.lhs, new_rhs))



























            for i, equ in enumerate(getter_equ.main_assignments[-lb_method.dim:]):













                new_rhs = (1.0 - psm_config.fraction_field.center) * equ.rhs













                fraction_field = get_individual_or_common_fraction_field(psm_config)













                for p in range(psm_config.max_particles_per_cell):













                    new_rhs += psm_config.object_velocity_field(p * lb_method.dim + i) * fraction_field.center(p)













                getter_equ.main_assignments.remove(equ)













                getter_equ.main_assignments.append(Assignment(equ.lhs, new_rhs))













        getter_equ.topological_sort()













    return getter_equ















































macroscopic_values_setter = pdf_initialization_assignments

































src/lbmpy/maxwellian_equilibrium.py



+206
−76
















Original line number
Diff line number
Diff line








@@ -18,51 +18,106 @@ from pystencils.cache import disk_cache













from pystencils.sympyextensions import remove_higher_order_terms































from lbmpy.moments import MOMENT_SYMBOLS













from lbmpy.continuous_distribution_measures import continuous_moment, continuous_central_moment, continuous_cumulant













from lbmpy.continuous_distribution_measures import (













    continuous_moment,













    continuous_central_moment,













    continuous_cumulant,













)













































def get_weights(stencil, c_s_sq=sp.Rational(1, 3)):













    if c_s_sq != sp.Rational(1, 3) and c_s_sq != sp.Symbol("c_s") ** 2:













        warnings.warn("Weights of discrete equilibrium are only valid if c_s^2 = 1/3")



























def get_weights(stencil):















    def weight_for_direction(direction):













        abs_sum = sum([abs(d) for d in direction])













        return get_weights.weights[stencil.Q][abs_sum]













        squared_length = sum([d**2 for d in direction])













        return get_weights.weights[stencil.D][stencil.Q][squared_length]





























    return [weight_for_direction(d) for d in stencil]













































get_weights.weights = {













    9: {













get_weights.weights = dict(













    {













        2: dict(













            {













                9: dict(













                    {















                        0: sp.Rational(4, 9),















                        1: sp.Rational(1, 9),















                        2: sp.Rational(1, 36),













    },













    7: {













                    }













                ),













                # weights taken from Coreixas et al. (2017), PRE.













                # https://doi.org/10.1103/PhysRevE.96.033306













                # (Appendix D Table 1)













                17: dict(













                    {













                        0: sp.S((575 + 193 * sp.sqrt(193)) / 8100),













                        1: sp.S((3355 - 91 * sp.sqrt(193)) / 18000),













                        2: sp.S((655 + 17 * sp.sqrt(193)) / 27000),













                        8: sp.S((685 - 49 * sp.sqrt(193)) / 54000),













                        9: sp.S((1445 - 101 * sp.sqrt(193)) / 162000),













                    }













                ),













                # weights taken from Coreixas et al. (2017), PRE.













                # https://doi.org/10.1103/PhysRevE.96.033306













                # (Appendix D Table 1)













                37: dict(













                    {













                        0: sp.S(0.23315066913235250228650),













                        1: sp.S(0.10730609154221900241246),













                        2: sp.S(0.05766785988879488203006),













                        4: sp.S(0.01420821615845075026469),













                        5: sp.S(0.00535304900051377523273),













                        8: sp.S(0.00101193759267357547541),













                        9: sp.S(0.00024530102775771734547),













                        10: sp.S(0.00028341425299419821740),













                    }













                ),













            }













        ),













        3: dict(













            {













                7: dict(













                    {















                        0: Zero(),















                        1: sp.Rational(1, 6),













    },













    15: {













                    }













                ),













                15: dict(













                    {















                        0: sp.Rational(2, 9),















                        1: sp.Rational(1, 9),















                        3: sp.Rational(1, 72),













    },













    19: {













                    }













                ),













                19: dict(













                    {















                        0: sp.Rational(1, 3),















                        1: sp.Rational(1, 18),















                        2: sp.Rational(1, 36),













    },













    27: {













                    }













                ),













                27: dict(













                    {















                        0: sp.Rational(8, 27),















                        1: sp.Rational(2, 27),















                        2: sp.Rational(1, 54),















                        3: sp.Rational(1, 216),















                    }













                ),













            }













        ),















    }













)















































@disk_cache













def discrete_maxwellian_equilibrium(stencil, rho=sp.Symbol("rho"), u=sp.symbols("u_:3"), order=2,













                                    c_s_sq=sp.Symbol("c_s") ** 2, compressible=True):













def discrete_maxwellian_equilibrium(













    stencil,













    rho=sp.Symbol("rho"),













    u=sp.symbols("u_:3"),













    order=2,













    c_s_sq=sp.Symbol("c_s") ** 2,













    compressible=True,













):















    """















    Returns the common discrete LBM equilibrium as a list of sympy expressions

























@@ -74,16 +129,26 @@ def discrete_maxwellian_equilibrium(stencil, rho=sp.Symbol("rho"), u=sp.symbols(













        c_s_sq: square of speed of sound















        compressible: compressibility















    """













    weights = get_weights(stencil, c_s_sq)













    weights = get_weights(stencil)















    assert stencil.Q == len(weights)















    u = u[: stencil.D]





























    res = [discrete_equilibrium(e_q, u, rho, w_q, order, c_s_sq, compressible) for w_q, e_q in zip(weights, stencil)]













    res = [













        discrete_equilibrium(e_q, u, rho, w_q, order, c_s_sq, compressible)













        for w_q, e_q in zip(weights, stencil)













    ]















    return tuple(res)













































def discrete_equilibrium(v=sp.symbols("v_:3"), u=sp.symbols("u_:3"), rho=sp.Symbol("rho"), weight=sp.Symbol("w"),













                         order=2, c_s_sq=sp.Symbol("c_s") ** 2, compressible=True):













def discrete_equilibrium(













    v=sp.symbols("v_:3"),













    u=sp.symbols("u_:3"),













    rho=sp.Symbol("rho"),













    weight=sp.Symbol("w"),













    order=2,













    c_s_sq=sp.Symbol("c_s") ** 2,













    compressible=True,













):















    """















    Returns the common discrete LBM equilibrium depending on the mesoscopic velocity and the directional lattice weight


























@@ -111,39 +176,60 @@ def discrete_equilibrium(v=sp.symbols("v_:3"), u=sp.symbols("u_:3"), rho=sp.Symb













    u_times_u = 0















    for u_alpha in u:















        u_times_u += u_alpha * u_alpha













    fq += sp.Rational(1, 2) / c_s_sq**2 * e_times_u ** 2 - sp.Rational(1, 2) / c_s_sq * u_times_u













    fq += (













        sp.Rational(1, 2) / c_s_sq**2 * e_times_u**2













        - sp.Rational(1, 2) / c_s_sq * u_times_u













    )































    if order <= 2:















        return fq * rho_outside * weight





























    fq += sp.Rational(1, 6) / c_s_sq**3 * e_times_u**3 - sp.Rational(1, 2) / c_s_sq**2 * u_times_u * e_times_u













    fq += (













        sp.Rational(1, 6) / c_s_sq**3 * e_times_u**3













        - sp.Rational(1, 2) / c_s_sq**2 * u_times_u * e_times_u













    )































    return sp.expand(fq * rho_outside * weight)















































@disk_cache













def generate_equilibrium_by_matching_moments(stencil, moments, rho=sp.Symbol("rho"), u=sp.symbols("u_:3"),













                                             c_s_sq=sp.Symbol("c_s") ** 2, order=None):













def generate_equilibrium_by_matching_moments(













    stencil,













    moments,













    rho=sp.Symbol("rho"),













    u=sp.symbols("u_:3"),













    c_s_sq=sp.Symbol("c_s") ** 2,













    order=None,













):















    """















    Computes discrete equilibrium, by setting the discrete moments to values taken from the continuous Maxwellian.















    The number of moments has to match the number of directions in the stencil. For documentation of other parameters















    see :func:`get_equilibrium_values_of_maxwell_boltzmann_function`















    """















    from lbmpy.moments import moment_matrix













    assert len(moments) == stencil.Q, f"Moment count({len(moments)}) does not match stencil size({stencil.Q})"













    continuous_moments_vector = get_equilibrium_values_of_maxwell_boltzmann_function(moments, stencil.D, rho, u, c_s_sq,













                                                                                     order, space="moment")



























    assert (













        len(moments) == stencil.Q













    ), f"Moment count({len(moments)}) does not match stencil size({stencil.Q})"













    continuous_moments_vector = get_equilibrium_values_of_maxwell_boltzmann_function(













        moments, stencil.D, rho, u, c_s_sq, order, space="moment"













    )















    continuous_moments_vector = sp.Matrix(continuous_moments_vector)















    M = moment_matrix(moments, stencil)













    assert M.rank() == stencil.Q, f"Rank of moment matrix ({M.rank()}) does not match stencil size ({stencil.Q})"













    assert (













        M.rank() == stencil.Q













    ), f"Rank of moment matrix ({M.rank()}) does not match stencil size ({stencil.Q})"















    return M.inv() * continuous_moments_vector















































@disk_cache













def continuous_maxwellian_equilibrium(dim=3, rho=sp.Symbol("rho"),













def continuous_maxwellian_equilibrium(













    dim=3,













    rho=sp.Symbol("rho"),















    u=sp.symbols("u_:3"),















    v=sp.symbols("v_:3"),













                                      c_s_sq=sp.Symbol("c_s") ** 2):













    c_s_sq=sp.Symbol("c_s") ** 2,













):















    """















    Returns sympy expression of Maxwell Boltzmann distribution

























@@ -158,15 +244,24 @@ def continuous_maxwellian_equilibrium(dim=3, rho=sp.Symbol("rho"),













    v = v[:dim]































    vel_term = sum([(v_i - u_i) ** 2 for v_i, u_i in zip(v, u)])













    return rho / (2 * sp.pi * c_s_sq) ** (sp.Rational(dim, 2)) * sp.exp(- vel_term / (2 * c_s_sq))













    return (













        rho













        / (2 * sp.pi * c_s_sq) ** (sp.Rational(dim, 2))













        * sp.exp(-vel_term / (2 * c_s_sq))













    )















































# -------------------------------- Equilibrium moments  ----------------------------------------------------------------















@disk_cache













def get_equilibrium_values_of_maxwell_boltzmann_function(moments, dim, rho=sp.Symbol("rho"),













def get_equilibrium_values_of_maxwell_boltzmann_function(













    moments,













    dim,













    rho=sp.Symbol("rho"),















    u=sp.symbols("u_:3"),













                                                         c_s_sq=sp.Symbol("c_s") ** 2, order=None,













                                                         space="moment"):













    c_s_sq=sp.Symbol("c_s") ** 2,













    order=None,













    space="moment",













):















    """















    Computes equilibrium values from the continuous Maxwell Boltzmann equilibrium.

























@@ -186,16 +281,30 @@ def get_equilibrium_values_of_maxwell_boltzmann_function(moments, dim, rho=sp.Sy













    # trick to speed up sympy integration (otherwise it takes multiple minutes, or aborts):















    # use a positive, real symbol to represent c_s_sq -> then replace this symbol afterwards with the real c_s_sq















    c_s_sq_helper = sp.Symbol("csq_helper", positive=True, real=True)













    mb = continuous_maxwellian_equilibrium(dim, rho, u, MOMENT_SYMBOLS[:dim], c_s_sq_helper)













    mb = continuous_maxwellian_equilibrium(













        dim, rho, u, MOMENT_SYMBOLS[:dim], c_s_sq_helper













    )















    if space == "moment":













        result = [continuous_moment(mb, moment, MOMENT_SYMBOLS[:dim]).subs(c_s_sq_helper, c_s_sq)













                  for moment in moments]













        result = [













            continuous_moment(mb, moment, MOMENT_SYMBOLS[:dim]).subs(













                c_s_sq_helper, c_s_sq













            )













            for moment in moments













        ]















    elif space == "central moment":













        result = [continuous_central_moment(mb, moment, MOMENT_SYMBOLS[:dim], velocity=u).subs(c_s_sq_helper, c_s_sq)













                  for moment in moments]













        result = [













            continuous_central_moment(













                mb, moment, MOMENT_SYMBOLS[:dim], velocity=u













            ).subs(c_s_sq_helper, c_s_sq)













            for moment in moments













        ]















    elif space == "cumulant":













        result = [continuous_cumulant(mb, moment, MOMENT_SYMBOLS[:dim]).subs(c_s_sq_helper, c_s_sq)













                  for moment in moments]













        result = [













            continuous_cumulant(mb, moment, MOMENT_SYMBOLS[:dim]).subs(













                c_s_sq_helper, c_s_sq













            )













            for moment in moments













        ]















    else:















        raise ValueError("Only moment, central moment or cumulant space are supported")

























@@ -206,9 +315,15 @@ def get_equilibrium_values_of_maxwell_boltzmann_function(moments, dim, rho=sp.Sy













































@disk_cache













def get_moments_of_discrete_maxwellian_equilibrium(stencil, moments,













                                                   rho=sp.Symbol("rho"), u=sp.symbols("u_:3"),













                                                   c_s_sq=sp.Symbol("c_s") ** 2, order=None, compressible=True):













def get_moments_of_discrete_maxwellian_equilibrium(













    stencil,













    moments,













    rho=sp.Symbol("rho"),













    u=sp.symbols("u_:3"),













    c_s_sq=sp.Symbol("c_s") ** 2,













    order=None,













    compressible=True,













):















    """Compute moments of discrete maxwellian equilibrium.































    Args:









@@ -221,6 +336,7 @@ def get_moments_of_discrete_maxwellian_equilibrium(stencil, moments,













        compressible: compressible or incompressible form















    """















    from lbmpy.moments import discrete_moment





























    if order is None:















        order = 4















    mb = discrete_maxwellian_equilibrium(stencil, rho, u, order, c_s_sq, compressible)









@@ -246,12 +362,16 @@ def compressible_to_incompressible_moment_value(term, rho, u):













    Returns:















        incompressible equilibrium value















    """













    warnings.warn("Usage of `compressible_to_incompressible_moment_value` is deprecated,"













                  " and the method will be removed soon.")













    warnings.warn(













        "Usage of `compressible_to_incompressible_moment_value` is deprecated,"













        " and the method will be removed soon."













    )















    term = sp.sympify(term)















    term = term.expand()















    if term.func != sp.Add:













        args = [term, ]













        args = [













            term,













        ]















    else:















        args = term.args

























@@ -264,15 +384,25 @@ def compressible_to_incompressible_moment_value(term, rho, u):













            res += t















    return res













































# -------------------------------- Equilibrium cumulants ---------------------------------------------------------------















































@disk_cache













def get_cumulants_of_discrete_maxwellian_equilibrium(stencil, cumulants,













                                                     rho=sp.Symbol("rho"), u=sp.symbols("u_:3"),













                                                     c_s_sq=sp.Symbol("c_s") ** 2, order=None, compressible=True):













def get_cumulants_of_discrete_maxwellian_equilibrium(













    stencil,













    cumulants,













    rho=sp.Symbol("rho"),













    u=sp.symbols("u_:3"),













    c_s_sq=sp.Symbol("c_s") ** 2,













    order=None,













    compressible=True,













):















    from lbmpy.cumulants import discrete_cumulant





























    if order is None:















        order = 4















    mb = discrete_maxwellian_equilibrium(stencil, rho, u, order, c_s_sq, compressible)













    return tuple([discrete_cumulant(mb, cumulant, stencil).expand() for cumulant in cumulants])












    return tuple(













        [discrete_cumulant(mb, cumulant, stencil).expand() for cumulant in cumulants]













    )
























src/lbmpy/methods/creationfunctions.py



+13
−10
















Original line number
Diff line number
Diff line








@@ -201,19 +201,23 @@ def create_from_equilibrium(stencil, equilibrium, conserved_quantity_computation





























    if cspace.collision_space == CollisionSpace.POPULATIONS:















        return MomentBasedLbMethod(stencil, equilibrium, mom_to_rr_dict, conserved_quantity_computation=cqc,













                                   force_model=force_model, zero_centered=zero_centered, fraction_field=fraction_field,













                                   force_model=force_model, zero_centered=zero_centered,













                                   fraction_field=fraction_field,















                                   moment_transform_class=None)















    elif cspace.collision_space == CollisionSpace.RAW_MOMENTS:















        return MomentBasedLbMethod(stencil, equilibrium, mom_to_rr_dict, conserved_quantity_computation=cqc,













                                   force_model=force_model, zero_centered=zero_centered, fraction_field=fraction_field,













                                   force_model=force_model, zero_centered=zero_centered,













                                   fraction_field=fraction_field,















                                   moment_transform_class=cspace.raw_moment_transform_class)















    elif cspace.collision_space == CollisionSpace.CENTRAL_MOMENTS:















        return CentralMomentBasedLbMethod(stencil, equilibrium, mom_to_rr_dict, conserved_quantity_computation=cqc,















                                          force_model=force_model, zero_centered=zero_centered,













                                          fraction_field=fraction_field,















                                          central_moment_transform_class=cspace.central_moment_transform_class)















    elif cspace.collision_space == CollisionSpace.CUMULANTS:















        return CumulantBasedLbMethod(stencil, equilibrium, mom_to_rr_dict, conserved_quantity_computation=cqc,















                                     force_model=force_model, zero_centered=zero_centered,













                                     fraction_field=fraction_field,















                                     central_moment_transform_class=cspace.central_moment_transform_class,















                                     cumulant_transform_class=cspace.cumulant_transform_class)


























@@ -334,7 +338,7 @@ def create_mrt_raw(stencil, relaxation_rates, continuous_equilibrium=True, conse













































def create_central_moment(stencil, relaxation_rates, nested_moments=None,













                          continuous_equilibrium=True, conserved_moments=True, fraction_field=None, **kwargs):













                          continuous_equilibrium=True, conserved_moments=True, **kwargs):















    r"""















    Creates moment based LB method where the collision takes place in the central moment space.

























@@ -348,7 +352,6 @@ def create_central_moment(stencil, relaxation_rates, nested_moments=None,













        continuous_equilibrium: determines if the discrete or continuous maxwellian equilibrium is















                        used to compute the equilibrium moments.















        conserved_moments: If lower order moments are conserved or not.













        fraction_field: fraction field for the PSM method















    Returns:















        :class:`lbmpy.methods.momentbased.CentralMomentBasedLbMethod` instance















    """









@@ -371,8 +374,8 @@ def create_central_moment(stencil, relaxation_rates, nested_moments=None,













        nested_moments = cascaded_moment_sets_literature(stencil)































    rr_dict = _get_relaxation_info_dict(relaxation_rates, nested_moments, stencil.D, conserved_moments)













    if fraction_field is not None:













        relaxation_rates_modifier = (1.0 - fraction_field.center)













    if 'fraction_field' in kwargs and kwargs['fraction_field'] is not None:













        relaxation_rates_modifier = (1.0 - kwargs['fraction_field'])















        rr_dict = _get_relaxation_info_dict(relaxation_rates, nested_moments, stencil.D,















                                            relaxation_rates_modifier=relaxation_rates_modifier)


























@@ -489,7 +492,7 @@ def create_mrt_orthogonal(stencil, relaxation_rates, continuous_equilibrium=True













    check_and_set_mrt_space(CollisionSpace.RAW_MOMENTS)































    if weighted:













        weights = get_weights(stencil, sp.Rational(1, 3))













        weights = get_weights(stencil)















    else:















        weights = None


























@@ -527,7 +530,7 @@ def create_mrt_orthogonal(stencil, relaxation_rates, continuous_equilibrium=True













































# ----------------------------------------- Cumulant method creators ---------------------------------------------------













def create_cumulant(stencil, relaxation_rates, cumulant_groups, conserved_moments=True, fraction_field=None, **kwargs):













def create_cumulant(stencil, relaxation_rates, cumulant_groups, conserved_moments=True, **kwargs):















    r"""Creates a cumulant-based lattice Boltzmann method.































    Args:









@@ -547,8 +550,8 @@ def create_cumulant(stencil, relaxation_rates, cumulant_groups, conserved_moment













    """















    cumulant_to_rr_dict = _get_relaxation_info_dict(relaxation_rates, cumulant_groups, stencil.D, conserved_moments)





























    if fraction_field is not None:













        relaxation_rates_modifier = (1.0 - fraction_field.center)













    if 'fraction_field' in kwargs and kwargs['fraction_field'] is not None:













        relaxation_rates_modifier = (1.0 - kwargs['fraction_field'])















        cumulant_to_rr_dict = _get_relaxation_info_dict(relaxation_rates, cumulant_groups, stencil.D,















                                                        relaxation_rates_modifier=relaxation_rates_modifier)