Homec4science
Diffusion akantu (features/50-using-gitpod-in-gitlab) Browse

rAKA/examples/c++/diffusion_model/README.rst
571699bcd9affeatures/50-using…

Last Change
Raw File

README.rst
View Options

Diffusion Model (2D and 3D)
```````````````````````````
:Sources:
.. collapse:: heat_diffusion_static_2d.cc (click to expand)
.. literalinclude:: examples/c++/diffusion_model/heat_diffusion_static_2d.cc
:language: c++
:lines: 20-
.. collapse:: material.dat (click to expand)
.. literalinclude:: examples/c++/diffusion_model/material.dat
:language: text
:Location:
``examples/c++/`` `diffusion_model <https://gitlab.com/akantu/akantu/-/blob/master/examples/c++/diffusion_model>`_
In ``diffusion_model``, examples of the ``HeatTransferModel`` are presented.
An example of a static heat propagation is presented in
``heat_diffusion_static_2d.cc``. This example consists of a square 2D plate of
:math:`1 \text{m}^2` having an initial temperature of :math:`100 \text{K}`
everywhere but a non centered hot point maintained at
:math:`300 \text{K}`. :numref:`fig-ex-diffusion_static` presents the geometry
of this case (left) and the results (right). The material used is a linear
fictitious elastic material with a density of :math:`8940 \text{kg}/\text{m}^3`,
a conductivity of :math:`401 \text{W}/\text{m}/\text{K}` and a specific heat
capacity of :math:`385 \text{J}/\text{K}/\text{kg}`.
The simulation is set following the procedure described in :ref:`sect-dm-using`
.. _fig-ex-diffusion_static:
.. figure:: examples/c++/diffusion_model/images/diffusion_static.png
:align: center
:width: 70%
Initial (left) and final (right) temperature field
:Sources:
.. collapse:: heat_diffusion_dynamic_2d.cc (click to expand)
.. literalinclude:: examples/c++/diffusion_model/heat_diffusion_static_2d.cc
:language: c++
:lines: 20-
.. collapse:: material.dat (click to expand)
.. literalinclude:: examples/c++/diffusion_model/material.dat
:language: text
In ``heat_diffusion_dynamics_2d.cc``, the same example is solved dynamically
using an explicit time scheme. The time step used is :math:`0.12 \text{s}`. The only main difference with the previous example lies in the model initiation::
model.initFull(_analysis_method = _explicit_lumped_mass);
.. _fig-ex-diffusion_explicit:
.. figure:: examples/c++/diffusion_model/images/hot-point-2.png
:align: center
:width: 60%
Temperature field after 15000 time steps = 30 minutes. The lines represent
iso-surfaces.
:Sources:
.. collapse:: heat_diffusion_dynamic_2d.cc (click to expand)
.. literalinclude:: examples/c++/diffusion_model/heat_diffusion_static_2d.cc
:language: c++
:lines: 20-
.. collapse:: material.dat (click to expand)
.. literalinclude:: examples/c++/diffusion_model/material.dat
:language: text
In ``heat_diffusion_dynamics_3d.cc``, a 3D explicit dynamic heat propagation
problem is solved. It consists of a cube having an initial temperature of
:math:`100 \text{K}` everywhere but a centered sphere maintained at
:math:`300 \text{K}`.
The simulation is set exactly as ``heat_diffusion_dynamics_2d.cc`` except that the mesh is now a 3D mesh and that the heat source has a third coordinate and is placed at the cube center.
The mesh is initialized with::
Int spatial_dimension = 3;
Mesh mesh(spatial_dimension);
mesh.read("cube.msh");
:numref:`fig-ex-diffusion_3d` presents the resulting temperature field evolution.
.. _fig-ex-diffusion_3d:
.. figure:: examples/c++/diffusion_model/images/diffusion_3d.gif
:align: center
:width: 70%
Temperature field evolution.
c4science · Help