| 201 | | ||[=#PA0158 PA0158] ||no vertical boundary condition for variable "..." || Routine {{{advec_s_bc}}} was called for a variable, which does not have a specific boundary condition implemented. || |
| 202 | | ||[=#PA0159 PA0159] ||no term for component "..." || Routine {{{buoyancy}}} was called for the u/w-component while an inclined surface was used. In case of an inclined surface (see [../inipar#alpha_surface alpha_surface]) the buoyancy term appears in the equation of motion of the w-component and u-component. There is no buoyancy term implemented for the v-component as the surface can only be inclined in x-direction and no buoyancy term is required for the v-component. || |
| | 201 | ||[=#PA0158 PA0158] ||no vertical boundary condition for variable "..." || Routine {{{advec_s_bc}}} which calculates the advection term for scalar quantities using the Bott-Chlond scheme was called for a variable, which does not have a specific boundary condition implemented (Adding top and bottom boundaries according to the relevant boundary conditions is not possible). This should not happen. Please submit a [/newticket trouble ticket]. || |
| | 202 | ||[=#PA0159 PA0159] ||no term for component "..." || Routine {{{buoyancy}}} was called for a different wind component than the u/w-component while an inclined surface was used. In case of an inclined surface (see [../inipar#alpha_surface alpha_surface]) the buoyancy term appears in the equation of motion of the w-component and u-component. There is no buoyancy term implemented for the v-component as the surface can only be inclined in x-direction and no buoyancy term is required for the v-component. This should not happen. Please submit a [/newticket trouble ticket]. || |
| 203 | 203 | ||[=#PA0160 PA0160] ||non-cyclic lateral boundaries along x do not allow calculation of spectra along x || In case of non-cyclic conditions spectra would be largely affected by the non-cyclic lateral boundaries since this conflicts with the basic assumption used for the FFT that the spatial extention in the x and y-direction are infinitely large. See also [../sppar#data_output_sp data_output_sp]. || |
| 204 | 204 | ||[=#PA0161 PA0161] ||sorry, calculation of spectra in non parallel mode is still not realized || Calculation of spectra in non-parallel mode is not implemented. || |
| 205 | 205 | ||[=#PA0162 PA0162] ||non-cyclic lateral boundaries along y do not allow calculation of spectra along y || In case of non-cyclic conditions spectra would be largely affected by the non-cyclic lateral boundaries since this conflicts with the basic assumption used for the FFT that the spatial extention in the x and y-direction are infinitely large. See also [../sppar#data_output_sp data_output_sp]. || |
| 206 | 206 | ||[=#PA0163 PA0163] ||run will be terminated because it is running out of job cpu limit remaining time: ... s termination time needed: ... s ||In case that [../d3par#restart_time restart_time] has not been set manually, PALM determines internally when a new restart run has to be carried out depending on the setting of [../d3par#termination_time_needed termination_time_needed]. Within the remaining time PALM will, for example, copy binary files for restart runs, archive or transfer result data. Have a look at [../runs Initialization and restart runs] for further information. || |
