Maybe resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1335
awaiting feedback from reporter.

Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1726

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

Resolves bug-report: http://www.openfoam.org/mantisbt/view.php?id=1664

by ensuring tetBasePtIs is called on all processors, even for those with
0 cells.  Also use unique communicator for globalMeshData to avoid data
transfer interference.

Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1792

Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1792

The built-in explicit symplectic integrator has been replaced by a
general framework supporting run-time selectable integrators.  Currently
the explicit symplectic, implicit Crank-Nicolson and implicit Newmark
methods are provided, all of which are 2nd-order in time:

Symplectic 2nd-order explicit time-integrator for 6DoF solid-body motion:

    Reference:
        Dullweber, A., Leimkuhler, B., & McLachlan, R. (1997).
        Symplectic splitting methods for rigid body molecular dynamics.
        The Journal of chemical physics, 107(15), 5840-5851.

    Can only be used for explicit integration of the motion of the body,
    i.e. may only be called once per time-step, no outer-correctors may be
    applied.  For implicit integration with outer-correctors choose either
    CrankNicolson or Newmark schemes.

    Example specification in dynamicMeshDict:
    solver
    {
        type    symplectic;
    }

Newmark 2nd-order time-i...

Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1870

Resolves some stability issues with the outlet of multiphase problems.

read in the construction from dictionary.

It is important that the initial value is obtained from the table
provided to avoid the user having to evaluate a consistent one or risk
the code crashing from a very sudden change in the value.

For explicit motion (and the first iteration of iterative motion
correction) the 2nd-order symplectic motion integrator is used.

For iterative correction a form of lagged Crank-Nicolson is used in
which the current time-step values correspond to the current iteration.
This converges to a 2nd-order implicit solution.

Now consistent with constructors.

surfaceFilmModels/submodels/thermo/phaseChangeModel/solidification: Corrected and improved solidification rate controls

    Solidification phase change model where all film mass is converted when the
    local temperature > activation temperature.  The latent heat is
    assumed to be removed by heat-transfer to the wall.

Deprecated old versions.

Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1858

Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1854

Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1853

PtrListDictionary: New form of Dictionary in which the list type is PtrList rather than a linked-list

Avoids problems with overlapping communicationbetween these reductions
and the calculation of deltaCoeffs.  This is a temporary fix while code
reorganizations are undertaken to ensure the globalMeshData is updated
before deltaCoeffs are requested.

Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1780

Patch provided by Daniel Jasinski
Resolved bug-report http://www.openfoam.org/mantisbt/view.php?id=1843

The previous method using a HashTable required a separate ordered list
of names which is hard to work with and maintain.

to allow the turbulent energy transport properties to be updated for
every energy solution if required.

Added correctEnergyTransport() call to reactingTwoPhaseEulerFoam

Updated files provided by Bruno Santos
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1793

Patch provided by Juho Peltola