This page is under construction. I will update by adding a description of each solver and model.
| Conduction | 
- laplacianFoam (Transient)
| Convection | 
- buoyantBoussinesqSimpleFoam (Steady)
- buoyantBoussinesqPimpleFoam (Transient)
- buoyantSimpleFoam (Steady)
- buoyantPimpleFoam (Transient)
| Conduction + Convection (Conjugate Heat Transfer) | 
- chtMultiRegionSimpleFoam (Steady)
- chtMultiRegionFoam (Transient)
| + Radiation | 
All the above solvers but laplacianFoam are able to deal with the radiative heat transfer. There are the following five (virtually four) models available in OpenFOAM. Their source code is located in src/thermophysicalModels/radiation/radiationModels and we can see the brief descriptions in the header file of each radiation class.
- P1
| 24 25 26 27 28 29 30 31 32 33 34 | Class     Foam::radiation::P1 Description     Works well for combustion applications where optical thickness, tau is     large, i.e. tau = a*L > 3 (L = distance between objects)     Assumes      - all surfaces are diffuse      - tends to over predict radiative fluxes from sources/sinks        *** SOURCES NOT CURRENTLY INCLUDED *** | 
Keywords: optical thickness [2]
- fvDOM (Finite Volume Discrete Ordinates Method)
| 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 | Class     Foam::radiation::fvDOM Description     Finite Volume Discrete Ordinates Method. Solves the RTE equation for n     directions in a participating media, not including scatter.     Available absorption models:         constantAbsorptionEmission         greyMeanAbsoprtionEmission         wideBandAbsorptionEmission     i.e. dictionary     \verbatim         fvDOMCoeffs         {             nPhi        4;          // azimuthal angles in PI/2 on X-Y.                                     //(from Y to X)             nTheta      0;          // polar angles in PI (from Z to X-Y plane)             convergence 1e-3;       // convergence criteria for radiation                                     //iteration             maxIter     4;          // maximum number of iterations             cacheDiv    true;       // cache the div of the RTE equation.             //NOTE: Caching div is "only" accurate if the upwind scheme is used             //in div(Ji,Ii_h)         }         solverFreq   1; // Number of flow iterations per radiation iteration     \endverbatim     The total number of solid angles is  4*nPhi*nTheta.     In 1D the direction of the rays is X (nPhi and nTheta are ignored)     In 2D the direction of the rays is on X-Y plane (only nPhi is considered)     In 3D (nPhi and nTheta are considered) | 
- viewFactor
| 24 25 26 27 28 29 30 31 32 33 34 35 36 37 | Class     Foam::radiation::viewFactor Description     View factor radiation model. The system solved is: C q = b     where:             Cij  = deltaij/Ej - (1/Ej - 1)Fij             q    = heat flux             b    = A eb - Ho     and:             eb   = sigma*T^4             Ej   = emissivity             Aij  = deltaij - Fij             Fij  = view factor matrix | 
- opaqueSolid
| 24 25 26 27 28 29 30 | Class     Foam::radiation::opaqueSolid Description     Radiation for solid opaque solids - does nothing to energy equation source     terms (returns zeros) but creates absorptionEmissionModel and     scatterModel. | 
- none
| 24 25 26 27 28 29 | Class     Foam::radiation::noRadiation Description     No radiation - does nothing to energy equation source terms     (returns zeros) | 
The settings of the radiation models are described in constant/radiationProperties file.
| References | 

Thanks! This is very helpful.
It gave me a general idea of what I will be studying
many thanks