Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1913

Avoids the clutter and maintenance effort associated with providing the
function signature string.

Avoids the clutter and maintenance effort associated with providing the
function signature string.

Avoids the clutter and maintenance effort associated with providing the
function signature string.

Avoids the clutter and maintenance effort associated with providing the
function signature string.

Now solvers return solver performance information for all components
with backward compatibility provided by the "max" function which created
the scalar solverPerformance from the maximum component residuals from
the SolverPerformance<Type>.

The residuals functionObject has been upgraded to support
SolverPerformance<Type> so that now the initial residuals for all
(valid) components are tabulated, e.g. for the cavity tutorial case the
residuals for p, Ux and Uy are listed vs time.

Currently the residualControl option of pimpleControl and simpleControl
is supported in backward compatibility mode (only the maximum component
residual is considered) but in the future this will be upgraded to
support convergence control for the components individually.

This development started from patches provided by Bruno Santos, See
http://www.openfoam.org/mantisbt/view.php?id=1824

This reverts commit 62062804.

Avoids the clutter and maintenance effort associated with providing the
function signature string.

Based on patch provided by Daniel Jasinski
See http://www.openfoam.org/mantisbt/view.php?id=1888

Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1479
Patches provided by Bruno Santos based on the work of Mattijs Janssens

The new NotImplemented macro uses __PRETTY_FUNCTION__ for GNU compatible
compilers otherwise __func__ to provide the function name string.

equationOfState/Boussinesq: New equation of state for the Boussinesq approximation for buoyant flows

Description
    Incompressible gas equation of state using the Boussinesq approximation for
    the density as a function of temperature only:

    \verbatim
        rho = rho0*(1 - beta*(T - T0))
    \endverbatim

To be used with the buoyantPimpleFoam and buoyantSimpleFoam solvers as
an alternative to using buoyantBoussinesqPimpleFoam or
buoyantBoussinesqSimpleFoam, providing consistency with all other
solvers and utilities using the thermodynamics package in OpenFOAM.

which use the __PRETTY_FUNCTION__ constant string to provide the function name

Patch provided by Daniel Jasinski: http://www.openfoam.org/mantisbt/view.php?id=1856

Reported in http://www.openfoam.org/mantisbt/view.php?id=1856

Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1884

Patch provided by Aron Jóhannesson
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1877

Provided by Bruno Santos
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1875

Resolves report http://www.openfoam.org/mantisbt/view.php?id=1875
Patch provided by Bruno Santos

Resolves report http://www.openfoam.org/mantisbt/view.php?id=1875

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.