- Nov 13, 2015
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Henry Weller authored
Usage: createTurbulenceFields [OPTIONS] options: -case <dir> specify alternate case directory, default is the cwd -constant include the 'constant/' dir in the times list -fields <wordReList> specify which turbulence fields (k, epsilon, omega, R) to write - eg '(k omega)' or '(R)' or '(.*)'. -latestTime select the latest time -newTimes select the new times -noFunctionObjects do not execute functionObjects -noZero exclude the '0/' dir from the times list, has precedence over the -withZero option -parallel run in parallel -roots <(dir1 .. dirN)> slave root directories for distributed running -time <ranges> comma-separated time ranges - eg, ':10,20,40:70,1000:' -srcDoc display source code in browser -doc display application documentation in browser -help print the usage Resolves feature request http://www.openfoam.org/mantisbt/view.php?id=1912
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- Nov 11, 2015
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Henry Weller authored
Avoids the clutter and maintenance effort associated with providing the function signature string.
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- Nov 10, 2015
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Henry Weller authored
Avoids the clutter and maintenance effort associated with providing the function signature string.
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Henry Weller authored
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
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- Nov 07, 2015
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Henry Weller authored
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- Nov 06, 2015
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Henry Weller authored
to support phase volume fraction changes due to pressure
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- Nov 05, 2015
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Henry Weller authored
Resolves bug-report http://openfoam.org/mantisbt/view.php?id=1899
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Henry Weller authored
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- Nov 01, 2015
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Henry Weller authored
The new NotImplemented macro uses __PRETTY_FUNCTION__ for GNU compatible compilers otherwise __func__ to provide the function name string.
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- Oct 31, 2015
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Henry Weller authored
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1886
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- Oct 30, 2015
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Henry Weller authored
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Henry Weller authored
Patch provided by Daniel Jasinski Resolves feature request http://www.openfoam.org/mantisbt/view.php?id=1856
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Henry Weller authored
buoyantBoussinesqSimpleFoam: Add support for radiative heat-transfer consistent with buoyantBoussinesqPimpleFoam Patch provided by Daniel Jasinski: http://www.openfoam.org/mantisbt/view.php?id=1856
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- Oct 29, 2015
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Henry Weller authored
Provided by Juho Peltola
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Henry Weller authored
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- Oct 27, 2015
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Henry Weller authored
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1880
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Henry Weller authored
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- Oct 26, 2015
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Henry Weller authored
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- Oct 23, 2015
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Henry Weller authored
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1756
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- Oct 22, 2015
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Henry Weller authored
reactingEulerFoam: Updated handling of thermal diffusivity to support Prandtl number and thermal wall-functions
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- Oct 21, 2015
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Henry Weller authored
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1377
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- Oct 19, 2015
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Henry Weller authored
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...
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Henry Weller authored
Ur can be generated using a functionObject or in the post-processor
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- Oct 17, 2015
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Henry Weller authored
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1868
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Henry Weller authored
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1872
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- Oct 05, 2015
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Henry Weller authored
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Henry Weller authored
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Henry Weller authored
to use the transport matrix construction in MovingPhaseModel
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Henry Weller authored
Patches provided by Bruno Santos Resolves feature-request http://www.openfoam.org/mantisbt/view.php?id=1861
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- Oct 01, 2015
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Henry Weller authored
Now consistent with constructors.
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- Sep 28, 2015
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Henry Weller authored
Resolves bug-report http://www.openfoam.org/mantisbt/view.php?id=1227 Patch provided by Bruno Santos
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- Sep 25, 2015
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Henry Weller authored
between incompressible and compressible phases
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Henry Weller authored
Now combinations of incompressible, compressible phases with or without mass-transfer are supported efficiently.
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Henry Weller authored
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- Sep 18, 2015
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Henry Weller authored
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- Sep 17, 2015
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Henry Weller authored
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Henry Weller authored
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Henry Weller authored
This file contains definitions rather than declarations
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Henry Weller authored
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- Sep 16, 2015
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Henry Weller authored
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