sergio authored 2 years ago and Kutalmış Berçin committed 2 years ago

Co-authored-by: Kutalmis Bercin <kutalmis.bercin@esi-group.com>

sergio authored 4 years ago and Andrew Heather committed 4 years ago

Member function dKcdTbyKc in thermo.H is calculated from S and G at Pstd.
Thus dGdT was removed from the thermos.

- Add optional hRef, eRef and Tref as optional.

- Use new thermo to multiphase solver icoReactingMuliPhaseFoam

- Remove hRefConst and eRefConst thermos.

TUT: Updated tutorials

- prelude to code refactoring

NOTE
    no source code change in this commit, only relocation,
    renaming and adjustment of Make/{files,options}

Renamed the original 'laminar' model to 'Stokes' to indicate it is a
linear stress model supporting both Newtonian and non-Newtonian
viscosity.

This general framework will support linear, non-linear, visco-elastic
etc. laminar transport models.

For backward compatibility the 'Stokes' laminar stress model can be
selected either the original 'laminar' 'simulationType'
specification in turbulenceProperties:

    simulationType laminar;

or using the new more general 'laminarModel' specification:

    simulationType laminar;

    laminar
    {
        laminarModel        Stokes;
    }

which allows other laminar stress models to be selected.

TurbulenceModels: Reorganized support macros to simplify the creation of additional turbulence model libraries

reactingEulerFoam: Updated handling of thermal diffusivity to support Prandtl number and thermal wall-functions

Supporting any number of phases with heat and mass transfer, phase-change and reactions

Supports separate turbulence models for each phase
Complete Lahey k-epsilon model provided
kineticTheory and particle-pressure models folded into same turbulence framework
by the addition of phase-pressure functions