Pitfalls and troubleshooting
Serpent produces two types of error messages:
- Input errors, identified by text "Input error", followed by the error message. If the error can be related to a specific input parameter, then also the name of the parameter and the line number in the input file are printed.
- Run-time errors, in which case the name of the associated subroutine is printed, along with some additional information.
Run-time errors should not occur, and they should always be reported to the developer team. This is also the case if the calculation crashes (segmentation fault or similar). In such case repeating the calculation in debug mode may reveal some additional information on what went wrong.
- 1 Things to check in case of suspicious results
- 2 Debugging the input model
Things to check in case of suspicious results
Material volumes are not necessarily needed for most transport simulations, but they do affect the results of burnup calculation. Serpent prints an error message if the volume of an irradiated material is not available. The most typical error related to volumes is that the code attempts to calculate the volumes of two-dimensional pin-structures automatically, but for some reason this calculation produces incorrect results. This happens, for example, when:
- The geometry has axial dimension (3D geometry is assumed to be 2D)
- Some parts of the fuel pins are located outside the geometry (pins are clipped by cell, universe or geometry boundary)
- When universe symmetries are used (unable to account for pins in symmetry positions)
Serpent cannot identify these problems, so no error message is printed.
Material volumes should always be checked using the Monte Carlo based volume checker routine before running the calculation. If the values are incorrect, or the calculation produces an error message on missing values, the volumes must be set manually.
Unresolved resonance probability table sampling
Unresolved resonance probability table sampling is not used by default. This method is needed to account for self-shielding effects in the unresolved resonance region. The effect is usually not significant in thermal systems, but can lead to noticeable discrepancies in fast-spectrum systems.
Probability table sampling is switched on using the set ures option.
Mass vs. atomic densities
The densities and compositions of materials can be entered in atomic or mass units (see the input syntax of the material card), and using incorrect units may lead to unexpected results. The difference may not be clearly noticeable if the material consists nuclides with similar atomic weight, but if there are both light and heavy nuclides the results can be off by tens of percent.
In particular, using incorrect units for isotopes in water causes a major distortion in the flux spectrum in LWR calculations. In burnup calculation this results in completely unexpected depletion rate of 235U and build-up rate of 239Pu.
The material and nuclide densities used in the calculation can be checked from the nuclide and material output file (<input>.out).
MPI parallelization without MPI mode
MPI scripts such as mpirun allow running Serpent even if the source code was not complied in MPI mode. Instead of starting a single parallel simulation, the result is multiple independent simulations that read and write the same input and output files. If two or more writing operations happen to overlap, identical sections are repeated in the output files. If the tasks are sufficiently off-sync, the writing operations do not overlap, and it may actually seem like everything is OK - the correct number of CPU's are working and the results look reasonable. The only thing that seems to be wrong is that the running time does not reflect the speed-up expected from the parallelization.
When MPI parallelization is executed correctly, the run-time output shows the number of mpi tasks, for example (MPI=10). The number of tasks is also printed in variable MPI_TASKS in the main output file. Whether the source code was compiled in MPI mode or not can be checked with sss2 -version.
Unable to start or maintain criticality source simulation
Criticality source simulation requires an initial guess for the fission source distribution. If no source definition is provided, Serpent samples source points uniformly throughout all fissile materials, i.e. materials with fissile isotopes. This creates two potential problems:
- If the fissile material covers only a small volume of the total geometry, the sampling of the initial source may fail completely.
- If the geometry contains both active and inactive fissile zones (e.g. seed and blanket), the calculation may fail after the first generation because the majority of source points are placed in the inactive zone.
The solution to both problems is to use explicit source definition that puts sufficient number of points in the active parts of the fuel. It should be noted that the use of an explicit source definition does not affect the results of the simulations, provided that the fission source is allowed to converge by skipping a sufficient number of inactive neutron generations.
Higher actinides not included in burnup calculation
Serpent forms the transmutation paths for burnup calculation automatically, starting from the initial composition defined in the material input. To avoid including everything available, the procedure applies a cut-off that after certain chain length discards all neutron reactions. The result is that some higher actinides, in particular berkelium and californium isotopes, are not produced through all possible chains, and some isotopes may not be included in the calculation at all.
Discarding these higher actinides should not affect the results of the calculation, but in some cases their concentrations are of particular interest. The transmutation chains can be extended further by adding nuclides at negligible concentrations (1E-15 or so). By adding isotopes like 240Cm 250Cm, 247Bk to 250Bk and 249Cf to 254Cf