Neutron flux for uniform parallelepiped ======================================= Neutron flux for a uniform rectangular parallelepiped reactor of side lengths :math:`a, b, c` depends on the cartesian coordinates :math:`x, y, z`. .. py:currentmodule:: symplyphysics.laws.nuclear.buckling.neutron_flux_for_uniform_parallelepiped .. py:data:: dimension_factor Dimension factor that appears as a coefficient in the solution to the :ref:`differential equation `. See :attr:`~symplyphysics.symbols.nuclear.neutron_flux`. Symbol: :code:`Phi_0` Latex: :math:`\Phi_{0}` Dimension: :code:`1/(area*time)` .. py:data:: x :attr:`~symplyphysics.symbols.classical_mechanics.position` along the :math:`x`-axis. Symbol: :code:`x_1` Latex: :math:`x_{1}` Dimension: :code:`length` .. py:data:: y :attr:`~symplyphysics.symbols.classical_mechanics.position` along the :math:`y`-axis. Symbol: :code:`x_2` Latex: :math:`x_{2}` Dimension: :code:`length` .. py:data:: z :attr:`~symplyphysics.symbols.classical_mechanics.position` along the :math:`z`-axis. Symbol: :code:`x_3` Latex: :math:`x_{3}` Dimension: :code:`length` .. py:data:: length :attr:`~symplyphysics.symbols.classical_mechanics.length` along the :math:`x`-axis. Symbol: :code:`l_1` Latex: :math:`l_{1}` Dimension: :code:`length` .. py:data:: width :attr:`~symplyphysics.symbols.classical_mechanics.length` along the :math:`y`-axis. Symbol: :code:`l_2` Latex: :math:`l_{2}` Dimension: :code:`length` .. py:data:: height :attr:`~symplyphysics.symbols.classical_mechanics.length` along the :math:`z`-axis. Symbol: :code:`l_3` Latex: :math:`l_{3}` Dimension: :code:`length` .. py:data:: neutron_flux :attr:`~symplyphysics.symbols.nuclear.neutron_flux` at a point with coordinates :attr:`~x`, :attr:`~y`, :attr:`~z`. Symbol: :code:`Phi` Latex: :math:`\Phi` Dimension: :code:`1/(area*time)` .. py:data:: law :code:`Phi = Phi_0 * cos(pi / l_2 * x_1) * cos(pi / l_1 * x_2) * cos(pi / l_3 * x_3)` Latex: .. math:: \Phi = \Phi_{0} \cos{\left(\frac{\pi}{l_{2}} x_{1} \right)} \cos{\left(\frac{\pi}{l_{1}} x_{2} \right)} \cos{\left(\frac{\pi}{l_{3}} x_{3} \right)}