Ansys Fluent uses a control-volume-based technique to convert a general scalar transport equation to an algebraic equation that can be solved numerically. This control volume technique consists of integrating the transport equation about each control volume, yielding a discrete equation that expresses the conservation law on a control-volume basis.
Discretization of the governing equations can be illustrated most easily by considering the unsteady conservation equation for transport of a scalar quantity . This is demonstrated by the following equation written in integral form for an arbitrary control volume as follows:
(23–1) |
where | |
= density | |
= velocity vector (= in 2D) | |
= surface area vector | |
= diffusion coefficient for | |
= gradient of (= in 2D) | |
= source of per unit volume |
Equation 23–1 is applied to each control volume, or cell, in the computational domain. The two-dimensional, triangular cell shown in Figure 23.3: Control Volume Used to Illustrate Discretization of a Scalar Transport Equation is an example of such a control volume. Discretization of Equation 23–1 on a given cell yields
(23–2) |
where | |
= number of faces enclosing cell | |
= value of convected through face | |
= mass flux through the face | |
= area vector of face , (= in 2D) | |
= gradient of at face | |
= cell volume |
Where is defined in Temporal Discretization. The equations solved by Ansys Fluent take the same general form as the one given above and apply readily to multi-dimensional, unstructured meshes composed of arbitrary polyhedra.
For more information, see the following section: