[aspect-devel] AGU meeting feedback
Juliane Dannberg
dannberg at gfz-potsdam.de
Fri Jan 10 09:43:35 PST 2014
Hi all,
On 01/09/2014 05:53 PM, Timo Heister wrote:
>> - Second, what happens if we use a smooth field, say using an arctangent
>> with a width of 2-3 cells. I bet that the first peak is exactly where
>> it was before, whereas the second one suddenly becomes grid
>> independent.
> Yes, I think so too. I am somewhat swamped right now, so I anybody
> wants to try this out...
>
> In the long run we should find a way to get this smoothing behavior
> automatically (this is basically what a levelset reinitialization
> would do). This assumes that this fixes the problem we are seeing.
>
okay, so I just tried this and it looks quite well
I have attached a plot of root mean square velocity in dependence of
time for different meshes, and now the solution seems not longer to be
mesh-dependent and the second peak seems to converge to a value similar
to the one in the van Keken Benchmark, too. I also attached my input
file, in case anybody wants to do some more testing. In principle I just
used a hyperbolic tangent function to smooth the boundary between the
compositional fields.
Cheers,
Juliane
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############### Global parameters
# We use a 3d setup. Since we are only interested
# in a steady state solution, we set the end time
# equal to the start time to force a single time
# step before the program terminates.
set Dimension = 2
set Start time = 0
set End time = 2000
set Use years in output instead of seconds = false
set CFL number = 1.0
set Output directory = van_Keken_8_smooth
subsection Geometry model
set Model name = box
subsection Box
set X extent = 0.9142
set Y extent = 1.0000
end
end
subsection Model settings
set Include adiabatic heating = false
set Include shear heating = false # default: true
set Tangential velocity boundary indicators = 0,1
set Zero velocity boundary indicators = 2,3
end
subsection Material model
set Model name = simple
subsection Simple model
set Reference density = 1010
set Viscosity = 1e2
set Thermal expansion coefficient = 0
end
end
subsection Gravity model
set Model name = vertical
subsection Vertical
set Magnitude = 10
end
end
############### Parameters describing the temperature field
# As above, there is no need to set anything for the
# temperature boundary conditions.
subsection Boundary temperature model
set Model name = box
end
subsection Initial conditions
set Model name = function
subsection Function
set Variable names = x,z
set Function constants = pi=3.14159
set Function expression = if((z>0.2+0.02*cos(pi*x/0.9142)),0,1)
end
end
############### Parameters describing the compositional field
subsection Compositional fields
set Number of fields = 1
end
subsection Compositional initial conditions
set Model name = function
subsection Function
set Variable names = x,z
set Function constants = pi=3.14159
set Function expression = 0.5*(1+tanh((0.2+0.02*cos(pi*x/0.9142)-z)*10/0.2))
end
end
subsection Material model
subsection Simple model
set Density differential for compositional field 1 = -10
end
end
############### Parameters describing the discretization
subsection Mesh refinement
set Initial adaptive refinement = 0
set Strategy = composition
set Initial global refinement = 8
set Time steps between mesh refinement = 1000000
set Coarsening fraction = 0.05
set Refinement fraction = 0.3
end
##subsection Discretization
## set Composition polynomial degree = 2
## subsection Stabilization parameters
## set beta = 0.5
## set cR = 1e15
## end
#3end
############### Parameters describing the what to do with the solution
subsection Postprocess
set List of postprocessors = visualization, velocity statistics, composition statistics
subsection Visualization
set List of output variables = all
set Output format = vtu
set Time between graphical output = 100
end
end
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