The heat flux vector is given by:
|
| (105) |
where
is the effective thermal conductivity given by:
|
| (106) |
with
being the turbulent Prandtl number. The diffusive flux at an interior face is then discretized as described in Finite Volume Discretization as follows:
|
| (107) |
For inviscid flows, the heat flux is zero.
For viscous flows, the heat flux is required. This is specified directly in the case of adiabatic or specified heat flux walls. It can also inferred as a convective heat transfer condition, such that
|
| (108) |
where
is a convective heat transfer coefficient and
is a reference temperature.
For laminar flow in which the wall temperature is specified, the heat flux is obtained as follows:
|
| (109) |
For turbulent flow in which the wall temperature is specified, thermal wall laws are employed as follows:
| (110) |
where
is defined in terms of the appropriate thermal wall law.