[cig-commits] [commit] master: remove accidentally added broken test (d14051b)
cig_noreply at geodynamics.org
cig_noreply at geodynamics.org
Sun Jun 8 07:15:13 PDT 2014
Repository : https://github.com/geodynamics/aspect
On branch : master
Link : https://github.com/geodynamics/aspect/compare/277ad233ad48d1c5db9e23cd1e74d6914cb94919...d14051bb8dc3b2a63654bfac6174f2c4371133f0
>---------------------------------------------------------------
commit d14051bb8dc3b2a63654bfac6174f2c4371133f0
Author: Timo Heister <timo.heister at gmail.com>
Date: Sun Jun 8 10:15:06 2014 -0400
remove accidentally added broken test
>---------------------------------------------------------------
d14051bb8dc3b2a63654bfac6174f2c4371133f0
tests/petsc_direct_solver.prm | 164 --------------------------------
tests/petsc_direct_solver/screen-output | 98 -------------------
tests/petsc_direct_solver/statistics | 18 ----
3 files changed, 280 deletions(-)
diff --git a/tests/petsc_direct_solver.prm b/tests/petsc_direct_solver.prm
deleted file mode 100644
index 9aab906..0000000
--- a/tests/petsc_direct_solver.prm
+++ /dev/null
@@ -1,164 +0,0 @@
-# test that the direct solver works in parallel with PETSc
-
-# LINEAR ALGEBRA: PETSC
-# MPI: 3
-
-set Dimension = 2
-
-set Use direct solver for Stokes system = true
-
-set Start time = 0
-set End time = 6e15
-set Use years in output instead of seconds = false
-
-set Output directory = output
-set Pressure normalization = surface
-
-
-subsection Geometry model
- set Model name = box
-
- subsection Box
- set X extent = 1000000
- set Y extent = 1000000
- end
-end
-
-
-subsection Gravity model
- set Model name = vertical
- subsection Vertical
- set Magnitude = 10.0
- end
-end
-
-
-subsection Model settings
-
- # As we only want to look at the effects of latent heating, we disable all
- # the other heating terms.
- set Include adiabatic heating = false
- set Include latent heat = true
- set Include shear heating = false
-
- # We only fix the temperature at the upper boundary, the other boundaries
- # are isolating. To guarantuee a steady downward flow, we fix the velocity
- # at the top and bottom, and set it to free slip on the sides.
- set Fixed temperature boundary indicators = 3
- set Prescribed velocity boundary indicators = 2:function, 3:function
- set Tangential velocity boundary indicators = 0, 1
-end
-
-
-############### Boundary conditions
-# We set the top temperature to T1=1000K.
-subsection Boundary temperature model
- set Model name = box
- subsection Box
- set Top temperature = 1000
- end
-end
-
-# We prescribe a constant downward flow.
-subsection Boundary velocity model
- subsection Function
- set Function expression = 0;-2.1422e-11
- set Variable names = x,y
- end
-end
-
-subsection Initial conditions
- set Model name = function
- subsection Function
- set Function expression = 1000.0
- set Variable names = x,y
- end
-end
-
-
-subsection Material model
- set Model name = latent heat
- subsection Latent heat
-
- # The change of density across the phase transition. Together with the
- # Clapeyron slope, this is what determines the entropy change.
- set Phase transition density jumps = 115.6
- set Corresponding phase for density jump = 0
-
- # If the temperature is equal to the phase transition temperature, the
- # phase transition will occur at the phase transition depth. However,
- # if the temperature deviates from this value, the Clapeyron slope
- # determines how much the pressure (and depth) of the phase boundary
- # changes. Here, the phase transition will be in the middle of the box
- # for T=T1.
- set Phase transition depths = 500000
- set Phase transition temperatures = 1000
- set Phase transition Clapeyron slopes = 1e7
-
- # We set the width of the phase transition to 5 km. You may want to
- # change this parameter to see how latent heating depends on the width
- # of the phase transition.
- set Phase transition widths = 5000
-
- set Reference density = 3400
- set Reference specific heat = 1000
- set Reference temperature = 1000
- set Thermal conductivity = 2.38
-
- # We set the thermal expansion amd the compressibility to zero, so that
- # all temperature (and density) changes are caused by advection, diffusion
- # and latent heating.
- set Thermal expansion coefficient = 0.0
- set Compressibility = 0.0
-
- # Viscosity is constant.
- set Thermal viscosity exponent = 0.0
- set Viscosity = 8.44e21
- set Viscosity prefactors = 1.0, 1.0
- set Composition viscosity prefactor = 1.0
- set Activation enthalpies = 3.9473e-3, 3.9473e-3
- end
-end
-
-
-subsection Mesh refinement
- set Initial adaptive refinement = 0
- set Initial global refinement = 5
- set Time steps between mesh refinement = 0
-
-end
-
-
-subsection Discretization
- subsection Stabilization parameters
- # The exponent $\alpha$ in the entropy viscosity stabilization. Units:
- # None.
- set alpha = 2
-
- # The $\beta$ factor in the artificial viscosity stabilization. An
- # appropriate value for 2d is 0.052 and 0.078 for 3d. Units: None.
- set beta = 0.078
-
- # The $c_R$ factor in the entropy viscosity stabilization. Units: None.
- set cR = 0.5 # default: 0.11
- end
-end
-
-
-subsection Postprocess
-
- set List of postprocessors = visualization
-
- subsection Visualization
-
- set Number of grouped files = 0
- set Output format = vtu
-
- # We are only interested in the last timestep (when the system hast reached
- # a steady state). For following the development of the system or checking
- # if the solution already reached steady state, this parameter can be set
- # to a smaller value.
- set Time between graphical output = 0
- set List of output variables = density
- end
-end
diff --git a/tests/petsc_direct_solver/screen-output b/tests/petsc_direct_solver/screen-output
deleted file mode 100644
index 0ca5c9b..0000000
--- a/tests/petsc_direct_solver/screen-output
+++ /dev/null
@@ -1,98 +0,0 @@
------------------------------------------------------------------------------
--- This is ASPECT, the Advanced Solver for Problems in Earth's ConvecTion.
--- . running in DEBUG mode
--- . running with 3 MPI processes
--- . using Trilinos
------------------------------------------------------------------------------
-
-Number of active cells: 1,024 (on 6 levels)
-Number of degrees of freedom: 13,764 (9,539+4,225)
-
-*** Timestep 0: t=0 seconds
- Solving temperature system... 0 iterations.
- Solving Stokes system... done.
-
- Postprocessing:
- Writing graphical output: output-direct_solver_2/solution-00000
-
-*** Timestep 1: t=7.26222e+14 seconds
- Solving temperature system... 189 iterations.
- Solving Stokes system... done.
-
- Postprocessing:
- Writing graphical output: output-direct_solver_2/solution-00001
-
-*** Timestep 2: t=1.4246e+15 seconds
- Solving temperature system... 22 iterations.
- Solving Stokes system... done.
-
- Postprocessing:
- Writing graphical output: output-direct_solver_2/solution-00002
-
-*** Timestep 3: t=2.11579e+15 seconds
- Solving temperature system... 20 iterations.
- Solving Stokes system... done.
-
- Postprocessing:
- Writing graphical output: output-direct_solver_2/solution-00003
-
-*** Timestep 4: t=2.79859e+15 seconds
- Solving temperature system... 21 iterations.
- Solving Stokes system... done.
-
- Postprocessing:
- Writing graphical output: output-direct_solver_2/solution-00004
-
-*** Timestep 5: t=3.48103e+15 seconds
- Solving temperature system... 20 iterations.
- Solving Stokes system... done.
-
- Postprocessing:
- Writing graphical output: output-direct_solver_2/solution-00005
-
-*** Timestep 6: t=4.16434e+15 seconds
- Solving temperature system... 20 iterations.
- Solving Stokes system... done.
-
- Postprocessing:
- Writing graphical output: output-direct_solver_2/solution-00006
-
-*** Timestep 7: t=4.85169e+15 seconds
- Solving temperature system... 19 iterations.
- Solving Stokes system... done.
-
- Postprocessing:
- Writing graphical output: output-direct_solver_2/solution-00007
-
-*** Timestep 8: t=5.54591e+15 seconds
- Solving temperature system... 19 iterations.
- Solving Stokes system... done.
-
- Postprocessing:
- Writing graphical output: output-direct_solver_2/solution-00008
-
-*** Timestep 9: t=6e+15 seconds
- Solving temperature system... 16 iterations.
- Solving Stokes system... done.
-
- Postprocessing:
- Writing graphical output: output-direct_solver_2/solution-00009
-
-Termination requested by criterion: end time
-
-
-+---------------------------------------------+------------+------------+
-| Total wallclock time elapsed since start | 3.75s | |
-| | | |
-| Section | no. calls | wall time | % of total |
-+---------------------------------+-----------+------------+------------+
-| Assemble Stokes system | 10 | 0.65s | 17% |
-| Assemble temperature system | 10 | 0.497s | 13% |
-| Build temperature preconditioner| 10 | 0.0327s | 0.87% |
-| Solve Stokes system | 10 | 1.88s | 50% |
-| Solve temperature system | 10 | 0.0984s | 2.6% |
-| Initialization | 2 | 0.0393s | 1% |
-| Postprocessing | 10 | 0.24s | 6.4% |
-| Setup dof systems | 1 | 0.0692s | 1.8% |
-+---------------------------------+-----------+------------+------------+
-
diff --git a/tests/petsc_direct_solver/statistics b/tests/petsc_direct_solver/statistics
deleted file mode 100644
index 3735ebc..0000000
--- a/tests/petsc_direct_solver/statistics
+++ /dev/null
@@ -1,18 +0,0 @@
-# 1: Time step number
-# 2: Time (seconds)
-# 3: Number of mesh cells
-# 4: Number of Stokes degrees of freedom
-# 5: Number of temperature degrees of freedom
-# 6: Iterations for temperature solver
-# 7: Time step size (seconds)
-# 8: Visualization file name
-0 0.0000e+00 1024 9539 4225 0 7.2622e+14 output-direct_solver_2/solution-00000
-1 7.2622e+14 1024 9539 4225 189 6.9838e+14 output-direct_solver_2/solution-00001
-2 1.4246e+15 1024 9539 4225 22 6.9119e+14 output-direct_solver_2/solution-00002
-3 2.1158e+15 1024 9539 4225 20 6.8280e+14 output-direct_solver_2/solution-00003
-4 2.7986e+15 1024 9539 4225 21 6.8244e+14 output-direct_solver_2/solution-00004
-5 3.4810e+15 1024 9539 4225 20 6.8331e+14 output-direct_solver_2/solution-00005
-6 4.1643e+15 1024 9539 4225 20 6.8734e+14 output-direct_solver_2/solution-00006
-7 4.8517e+15 1024 9539 4225 19 6.9422e+14 output-direct_solver_2/solution-00007
-8 5.5459e+15 1024 9539 4225 19 4.5409e+14 output-direct_solver_2/solution-00008
-9 6.0000e+15 1024 9539 4225 16 7.1111e+14 output-direct_solver_2/solution-00009
More information about the CIG-COMMITS
mailing list