23.2. General Scalar Transport Equation: Discretization and Solution

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.

Figure 23.3: Control Volume Used to Illustrate Discretization of a Scalar Transport Equation

Control Volume Used to Illustrate Discretization of a Scalar Transport Equation

For more information, see the following section: