| 57 | |
| 58 | === Outflow boundary === |
| 59 | |
| 60 | At 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. |
| 61 | For the scalar quantities, Neumann boundary conditions are used at the outflow boundary which is the simplest way. |
| 62 | For 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. |
| 63 | Instead, 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]). |
| 64 | For 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 | }}} |
| 69 | which considers flow disturbances propagating with the mean flow and by waves. |
| 70 | Here ψ is the transported quantity and $\partial_n$ is the derivative normal to the outflow boundary. |
| 71 | In PALM, based on 5, the radiation boundary condition is realized in two ways as follows. |
| 72 | |