Changes between Version 3 and Version 4 of doc/tec/noncyclic


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Timestamp:
Mar 12, 2013 5:32:55 PM (12 years ago)
Author:
fricke
Comment:

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  • doc/tec/noncyclic

    v3 v4  
    5555So far, we have experience with gravity waves in case of cold air outbreaks, which grow in amplitude up to quite extreme values, if no damping is applied.
    5656In the respective simulations, we used typical values for [../../app/inipar/#pt_damping_factor pt_damping_factor] of 0.05 and for [../../app/inipar/#pt_damping_width pt_damping_width] of 25 km in order to prevent the gravity waves from growing.
     57
     58=== Outflow boundary ===
     59
     60At the outflow, an open boundary condition is needed to ensure that disturbances of the mean flow can exit the model domain without effecting the flow upstream.
     61For the scalar quantities, Neumann boundary conditions are used at the outflow boundary which is the simplest way.
     62For the velocity components, a Neumann condition would require to be considered in the solution of the Poisson equation for perturbation pressure, which has not been realized so far, because it requires some technical effort.
     63Instead, PALM offers two types of radiation boundary conditions for the velocity components, which are not in conflict with the pressure solver (see [../../app/inipar/#bc_lr bc_lr] and [../../app/inipar/#bc_ns bc_ns]).
     64For the radiation condition, the Sommerfeld radiation equation is solved at the outflow
     65{{{
     66#!Latex
     67 \partial_t \psi  + c_{\psi} \partial_n \psi  = 0 \; , \quad (5)
     68}}}
     69which considers flow disturbances propagating with the mean flow and by waves.
     70Here ψ is the transported quantity and  $\partial_n$ is the derivative normal to the outflow boundary.
     71In PALM, based on 5, the radiation boundary condition is realized in two ways as follows.
     72