Difference between revisions of "Domain decomposition"
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− | Domain decomposition is used for saving computer memory by spatially dividing large burnup calculation problems between multiple calculation nodes. Each node handles particle transport only within its own domain, and particles crossing the domain boundaries are sent to another node to complete the history. The implementation in Serpent relies on a collision-based approach, i.e. the transfer is invoked when the particle undergoes a collision in a material which belongs to another domain. The decomposition affects only burnable materials divided into depletion zones using the [[Input syntax manual#div (divisor definition)|div card]]. The most typical domain decomposition case is a full-core burnup calculation, in which the fuel is decomposed into separate domains to save memory. Interaction data for the other materials is shared by all parallel tasks. | + | Domain decomposition is used for saving computer memory by spatially dividing large burnup calculation problems between multiple calculation nodes. Each node handles particle transport only within its own domain, and particles crossing the domain boundaries are sent to another node to complete the history. The implementation in Serpent relies on a collision-based approach<ref>García, M., Leppänen, J. and Sánchez-Espinoza, V. ''"A Collision-based Domain Decomposition scheme for large-scale depletion with the Serpent 2 Monte Carlo code."'' Ann. Nucl. Energy [https://doi.org/10.1016/j.anucene.2020.108026 '''152''' (2021) 108026].</ref>, i.e. the transfer is invoked when the particle undergoes a collision in a material which belongs to another domain. The decomposition affects only burnable materials divided into depletion zones using the [[Input syntax manual#div (divisor definition)|div card]]. The most typical domain decomposition case is a full-core burnup calculation, in which the fuel is decomposed into separate domains to save memory. Interaction data for the other materials is shared by all parallel tasks. |
The current implementation in Serpent 2 is relatively simple, and mainly designed for reactor cores. The number of domains is determined by the number of MPI tasks, and the division using the [[Input syntax manual#set dd|set dd]] input option. There are three division types: | The current implementation in Serpent 2 is relatively simple, and mainly designed for reactor cores. The number of domains is determined by the number of MPI tasks, and the division using the [[Input syntax manual#set dd|set dd]] input option. There are three division types: | ||
Line 6: | Line 6: | ||
# geometry-based division into sectors and a central zone, <tt>''MODE''</tt> 3. | # geometry-based division into sectors and a central zone, <tt>''MODE''</tt> 3. | ||
− | The method is illustrated by a | + | <u>Notes:</u> |
+ | *The methodology was implemented in version 2.1.31. | ||
+ | *The domain decomposition methodology allows the use of the restart capability from Serpent 2.1.32 version. The multiple restart files generated within a domain decomposition simulation can be read either in a subsequent domain decomposition simulation or within an automated depletion sequence, e.g., group-constant generation (matching the number of MPI tasks). | ||
+ | *From Serpent 2.1.32 version and on, the associated depletion output file in a domain decomposition simulation is not limited to parent materials. | ||
+ | |||
+ | == Full-core example == | ||
+ | |||
+ | The method is illustrated by a full-core example, where the depletion zone division and domain decomposition is defined by input lines: | ||
<nowiki> | <nowiki> | ||
− | % --- Domain decomposition | + | % --- Domain decomposition ---------------------------------------------------- |
% --- Divide fuel into depletion zones: | % --- Divide fuel into depletion zones: | ||
Line 15: | Line 22: | ||
div fuel sep 1 | div fuel sep 1 | ||
− | % -- Domain decomposition (1 = simple, 2 = sector, 3 = sector + center) | + | % --- Domain decomposition (1 = simple, 2 = sector, 3 = sector + center) |
set dd 3 | set dd 3 | ||
− | % | + | % -----------------------------------------------------------------------------</nowiki> |
When the calculation is run with 5 MPI tasks, it produces the following output: | When the calculation is run with 5 MPI tasks, it produces the following output: | ||
Line 57: | Line 64: | ||
[[File:Dd_mode3.png|358px]] [[File:Dd_mode2.png|358px]] [[File:Dd_mode1.png|358px]] | [[File:Dd_mode3.png|358px]] [[File:Dd_mode2.png|358px]] [[File:Dd_mode1.png|358px]] | ||
− | < | + | <div class="toccolours mw-collapsible mw-collapsed" style="width:85em;"> |
− | + | '''complete full-core input''' | |
− | + | <div class="mw-collapsible-content"> | |
− | + | <nowiki> | |
+ | % ----------------------------------------------------------------------------- | ||
+ | |||
+ | set title "Monte Carlo performance benchmark" | ||
+ | |||
+ | % Based on revision 1.2 (July 2011) of Monte Carlo performance benchmark: | ||
+ | % | ||
+ | % http://www.oecd-nea.org/dbprog/MonteCarloPerformanceBenchmark.htm | ||
+ | |||
+ | % ----------------------------------------------------------------------------- | ||
+ | |||
+ | % --- Neutron population and criticality cycles: | ||
+ | |||
+ | set pop 500000 1000 200 | ||
+ | set opti 1 | ||
+ | |||
+ | % --- Plot: | ||
+ | |||
+ | plot 3 1000 1000 0 -187.6 187.6 -187.6 187.6 | ||
+ | |||
+ | % --- Thermal flux / fission rate mesh: | ||
+ | |||
+ | mesh 2 996 904 | ||
+ | mesh 3 996 996 | ||
+ | |||
+ | % ----------------------------------------------------------------------------- | ||
+ | % ----- Geometry -------------------------------------------------------------- | ||
+ | |||
+ | % --- Cross section library file path: | ||
+ | |||
+ | set acelib "sss_jeff31u.xsdata" | ||
+ | |||
+ | % --- Boundary between hot and cold: | ||
+ | |||
+ | surf 1 pz 0.0 | ||
+ | |||
+ | % -- Water layers: | ||
+ | |||
+ | cell 31 3 cold_water -1 | ||
+ | cell 32 3 hot_water 1 | ||
+ | |||
+ | % --- Fuel pin: | ||
+ | |||
+ | pin 1 | ||
+ | fuel 0.41 | ||
+ | clad 0.475 | ||
+ | fill 3 | ||
+ | |||
+ | % --- Guide tube: | ||
+ | |||
+ | pin 2 | ||
+ | fill 3 0.56 | ||
+ | clad 0.62 | ||
+ | fill 3 | ||
+ | |||
+ | % --- Pin lattice: | ||
+ | |||
+ | lat 110 1 0.0 0.0 17 17 1.26 | ||
+ | |||
+ | 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 | ||
+ | 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 | ||
+ | 1 1 1 1 1 2 1 1 2 1 1 2 1 1 1 1 1 | ||
+ | 1 1 1 2 1 1 1 1 1 1 1 1 1 2 1 1 1 | ||
+ | 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 | ||
+ | 1 1 2 1 1 2 1 1 2 1 1 2 1 1 2 1 1 | ||
+ | 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 | ||
+ | 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 | ||
+ | 1 1 2 1 1 2 1 1 2 1 1 2 1 1 2 1 1 | ||
+ | 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 | ||
+ | 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 | ||
+ | 1 1 2 1 1 2 1 1 2 1 1 2 1 1 2 1 1 | ||
+ | 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 | ||
+ | 1 1 1 2 1 1 1 1 1 1 1 1 1 2 1 1 1 | ||
+ | 1 1 1 1 1 2 1 1 2 1 1 2 1 1 1 1 1 | ||
+ | 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 | ||
+ | 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 | ||
+ | |||
+ | % --- assembly data: | ||
+ | |||
+ | surf 1000 inf | ||
+ | |||
+ | cell 110 4 fill 110 -1000 | ||
+ | |||
+ | % --- Radial reflector: | ||
+ | |||
+ | cell 51 5 lower_radial_refl -1 | ||
+ | cell 52 5 upper_radial_refl 1 | ||
+ | |||
+ | % --- Core lattice: | ||
+ | |||
+ | lat 211 1 0.0 0.0 17 17 21.42 | ||
+ | |||
+ | 5 5 5 5 5 4 4 4 4 4 4 4 5 5 5 5 5 | ||
+ | 5 5 5 4 4 4 4 4 4 4 4 4 4 4 5 5 5 | ||
+ | 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 | ||
+ | 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 | ||
+ | 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 | ||
+ | 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 | ||
+ | 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 | ||
+ | 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 | ||
+ | 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 | ||
+ | 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 | ||
+ | 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 | ||
+ | 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 | ||
+ | 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 | ||
+ | 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 | ||
+ | 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 | ||
+ | 5 5 5 4 4 4 4 4 4 4 4 4 4 4 5 5 5 | ||
+ | 5 5 5 5 5 4 4 4 4 4 4 4 5 5 5 5 5 | ||
+ | |||
+ | surf 211 sqc 0.0 0.0 182.07 | ||
+ | |||
+ | cell 211 210 fill 211 -211 | ||
+ | cell 212 210 lower_radial_refl 211 -1 | ||
+ | cell 213 210 upper_radial_refl 211 1 | ||
+ | |||
+ | % --- Core geometry: | ||
+ | |||
+ | surf 11 pz -229.0 | ||
+ | surf 12 pz -199.0 | ||
+ | surf 13 pz -193.0 | ||
+ | surf 14 pz -183.0 | ||
+ | surf 15 pz 183.0 | ||
+ | surf 16 pz 203.0 | ||
+ | surf 17 pz 215.0 | ||
+ | surf 18 pz 223.0 | ||
+ | |||
+ | surf 20 cyl 0.0 0.0 187.6 | ||
+ | surf 21 cyl 0.0 0.0 209.0 | ||
+ | surf 22 cyl 0.0 0.0 229.0 | ||
+ | surf 23 cyl 0.0 0.0 249.0 | ||
+ | |||
+ | cell 1 0 bottom_plate -22 11 -12 | ||
+ | cell 2 0 bottom_nozzle -20 12 -13 | ||
+ | cell 3 0 bottom_fa -20 13 -14 | ||
+ | cell 4 0 lower_radial_refl 20 -21 12 -14 | ||
+ | cell 5 0 fill 210 -21 14 -15 | ||
+ | cell 6 0 upper_radial_refl 20 -21 15 -17 | ||
+ | cell 7 0 top_fa -20 15 -16 | ||
+ | cell 8 0 top_nozzle -20 16 -17 | ||
+ | cell 9 0 cold_water 21 -22 12 -17 | ||
+ | cell 10 0 top_plate -22 17 -18 | ||
+ | cell 11 0 vessel 22 -23 11 -18 | ||
+ | |||
+ | cell 666 0 outside 23 11 -18 | ||
+ | cell 667 0 outside -11 | ||
+ | cell 668 0 outside 18 | ||
+ | |||
+ | % ----------------------------------------------------------------------------- | ||
+ | % --- Materials --------------------------------------------------------------- | ||
+ | |||
+ | mat fuel -10.062 burn 1 | ||
+ | |||
+ | 92234.03c 4.9476E-6 | ||
+ | 92235.03c 4.8218E-4 | ||
+ | 92236.03c 9.0402E-5 | ||
+ | 92238.03c 2.1504E-2 | ||
+ | 93237.03c 7.3733E-6 | ||
+ | 94238.03c 1.5148E-6 | ||
+ | 94239.03c 1.3955E-4 | ||
+ | 94240.03c 3.4405E-5 | ||
+ | 94241.03c 2.1439E-5 | ||
+ | 94242.03c 3.7422E-6 | ||
+ | 95241.03c 4.5041E-7 | ||
+ | 95242.03c 9.2301E-9 | ||
+ | 95243.03c 4.7878E-7 | ||
+ | 96242.03c 1.0485E-7 | ||
+ | 96243.03c 1.4268E-9 | ||
+ | 96244.03c 8.8756E-8 | ||
+ | 96245.03c 3.5285E-9 | ||
+ | 42095.03c 2.6497E-5 | ||
+ | 43099.03c 3.2772E-5 | ||
+ | 44101.03c 3.0742E-5 | ||
+ | 44103.03c 2.3505E-6 | ||
+ | 47109.03c 2.0009E-6 | ||
+ | 54135.03c 1.0801E-8 | ||
+ | 55133.03c 3.4612E-5 | ||
+ | 60143.03c 2.6078E-5 | ||
+ | 60145.03c 1.9898E-5 | ||
+ | 62147.03c 1.6128E-6 | ||
+ | 62149.03c 1.1627E-7 | ||
+ | 62150.03c 7.1727E-6 | ||
+ | 62151.03c 5.4947E-7 | ||
+ | 62152.03c 3.0221E-6 | ||
+ | 63153.03c 2.6209E-6 | ||
+ | 64155.03c 1.5369E-9 | ||
+ | 8016.03c 4.5737E-2 | ||
+ | |||
+ | mat clad -5.77 rgb 100 100 100 | ||
+ | |||
+ | 40000.03c 1.0 | ||
+ | |||
+ | mat cold_water -0.74 moder lwtr 1001 rgb 100 150 200 | ||
+ | |||
+ | 1001.03c 2.000 | ||
+ | 8016.03c 1.000 | ||
+ | 5010.03c 6.490E-4 | ||
+ | 5011.03c 2.689E-3 | ||
+ | |||
+ | mat hot_water -0.66 moder lwtr 1001 rgb 100 150 200 | ||
+ | |||
+ | 1001.03c 2.000 | ||
+ | 8016.03c 1.000 | ||
+ | 5010.03c 6.490E-4 | ||
+ | 5011.03c 2.689E-3 | ||
+ | |||
+ | mat vessel -7.9 rgb 50 50 50 | ||
+ | |||
+ | 26000.03c -96.3 | ||
+ | 28000.03c -1.0 | ||
+ | 25055.03c -1.0 | ||
+ | 42000.03c -0.6 | ||
+ | 14000.03c -0.4 | ||
+ | 24000.03c -0.25 | ||
+ | 6000.03c -0.25 | ||
+ | 29000.03c -0.2 | ||
+ | |||
+ | mat lower_radial_refl -4.32 moder lwtr 1001 rgb 100 100 100 | ||
+ | |||
+ | 1001.03c -0.0095661 | ||
+ | 8016.03c -0.0759107 | ||
+ | 5010.03c -3.08409E-4 | ||
+ | 5011.03c -1.40499E-5 | ||
+ | 26000.03c -0.6309028 | ||
+ | 28000.03c -0.0822917 | ||
+ | 25055.03c -0.0182870 | ||
+ | 14000.03c -0.0091435 | ||
+ | 24000.03c -0.1737269 | ||
+ | |||
+ | mat upper_radial_refl -4.28 moder lwtr 1001 rgb 100 100 100 | ||
+ | |||
+ | 1001.03c -0.0086117 | ||
+ | 8016.03c -0.0683369 | ||
+ | 5010.03c -2.77638E-5 | ||
+ | 5011.03c -1.26481E-4 | ||
+ | 26000.03c -0.6367991 | ||
+ | 28000.03c -0.0830607 | ||
+ | 25055.03c -0.0184579 | ||
+ | 14000.03c -0.0092290 | ||
+ | 24000.03c -0.1753505 | ||
+ | |||
+ | mat bottom_plate -7.184 moder lwtr 1001 | ||
+ | |||
+ | 1001.03c -0.0011505 | ||
+ | 8016.03c -0.0091296 | ||
+ | 5010.03c -3.70915E-6 | ||
+ | 5011.03c -1.68974E-5 | ||
+ | 26000.03c -0.6828925 | ||
+ | 28000.03c -0.0890729 | ||
+ | 25055.03c -0.0197940 | ||
+ | 14000.03c -0.0098970 | ||
+ | 24000.03c -0.1880429 | ||
+ | |||
+ | mat bottom_nozzle -2.53 moder lwtr 1001 | ||
+ | |||
+ | 1001.03c -0.0245014 | ||
+ | 8016.03c -0.1944274 | ||
+ | 5010.03c -7.89917E-5 | ||
+ | 5011.03c -3.59854E-4 | ||
+ | 26000.03c -0.5386364 | ||
+ | 28000.03c -0.0702569 | ||
+ | 25055.03c -0.0156126 | ||
+ | 14000.03c -0.0078063 | ||
+ | 24000.03c -0.1483202 | ||
+ | |||
+ | mat top_nozzle -1.746 moder lwtr 1001 | ||
+ | |||
+ | 1001.03c -0.0358870 | ||
+ | 8016.03c -0.2847761 | ||
+ | 5010.03c -1.15699E-4 | ||
+ | 5011.03c -5.27075E-4 | ||
+ | 26000.03c -0.4682990 | ||
+ | 28000.03c -0.0610825 | ||
+ | 25055.03c -0.0135739 | ||
+ | 14000.03c -0.0067869 | ||
+ | 24000.03c -0.1289519 | ||
+ | |||
+ | mat top_plate -4.28 moder lwtr 1001 | ||
+ | |||
+ | 1001.03c -0.0086117 | ||
+ | 8016.03c -0.0683369 | ||
+ | 5010.03c -2.77638E-5 | ||
+ | 5011.03c -1.26481E-4 | ||
+ | 26000.03c -0.6367991 | ||
+ | 28000.03c -0.0830607 | ||
+ | 25055.03c -0.0184579 | ||
+ | 14000.03c -0.0092290 | ||
+ | 24000.03c -0.1753505 | ||
+ | |||
+ | mat bottom_fa -3.044 moder lwtr 1001 | ||
+ | |||
+ | 1001.03c -0.0162913 | ||
+ | 8016.03c -0.1292776 | ||
+ | 5010.03c -5.25228E-5 | ||
+ | 5011.03c -2.39272E-4 | ||
+ | 40000.03c -0.8541393 | ||
+ | |||
+ | mat top_fa -1.762 moder lwtr 1001 | ||
+ | |||
+ | 1001.03c -0.0292856 | ||
+ | 8016.03c -0.2323919 | ||
+ | 5010.03c -9.44159E-5 | ||
+ | 5011.03c -4.30120E-4 | ||
+ | 40000.03c -0.7377980 | ||
+ | |||
+ | % --- Thermal scattering data | ||
+ | |||
+ | therm lwtr lwj3.00t | ||
+ | |||
+ | % ----------------------------------------------------------------------------- | ||
+ | % --- Depletion history ------------------------------------------------------- | ||
+ | |||
+ | % --- Decay and fission yield libraries: | ||
+ | |||
+ | set declib "/xs/sss_jeff31.dec" | ||
+ | set nfylib "/xs/sss_jeff31.nfy" | ||
+ | |||
+ | % --- Irradiation cycle: | ||
+ | |||
+ | set powdens 40.0E-3 | ||
+ | |||
+ | dep butot | ||
+ | |||
+ | 0.10 | ||
+ | 0.50 | ||
+ | 1.00 | ||
+ | 1.50 | ||
+ | 2.00 | ||
+ | 2.50 | ||
+ | 3.00 | ||
+ | 3.50 | ||
+ | 4.00 | ||
+ | 4.50 | ||
+ | 5.00 | ||
+ | 5.50 | ||
+ | 6.00 | ||
+ | 6.50 | ||
+ | 7.00 | ||
+ | 7.50 | ||
+ | 8.00 | ||
+ | 8.50 | ||
+ | 9.00 | ||
+ | 9.50 | ||
+ | 10.00 | ||
+ | 10.50 | ||
+ | 11.00 | ||
+ | 11.50 | ||
+ | 12.00 | ||
+ | 12.50 | ||
+ | 13.00 | ||
+ | 13.50 | ||
+ | 14.00 | ||
+ | 14.50 | ||
+ | 15.00 | ||
+ | 17.50 | ||
+ | 20.00 | ||
+ | 22.50 | ||
+ | 25.00 | ||
+ | 27.50 | ||
+ | 30.00 | ||
+ | 32.50 | ||
+ | 35.00 | ||
+ | 37.50 | ||
+ | 40.00 | ||
+ | |||
+ | % --- Isotope list for inventory calculation: | ||
+ | |||
+ | set inventory all | ||
+ | |||
+ | % --- Depletion output: | ||
+ | |||
+ | set depout 2 | ||
+ | |||
+ | % --- Material volumes: | ||
+ | |||
+ | set mcvol 10000000000 | ||
+ | |||
+ | % ----------------------------------------------------------------------------- | ||
+ | % --- Domain decomposition ---------------------------------------------------- | ||
+ | |||
+ | % --- Divide fuel into depletion zones: | ||
+ | |||
+ | div fuel sep 1 | ||
+ | |||
+ | % --- Domain decomposition (1 = simple, 2 = sector, 3 = sector + center) | ||
+ | |||
+ | set dd 3 | ||
+ | |||
+ | % -----------------------------------------------------------------------------</nowiki> | ||
+ | |||
+ | </div> | ||
+ | </div> | ||
+ | |||
+ | == References == | ||
+ | |||
+ | <references/> | ||
[[Category:Input]] | [[Category:Input]] | ||
[[Category:Theory]] | [[Category:Theory]] | ||
[[Category:Tutorials]] | [[Category:Tutorials]] |
Latest revision as of 17:31, 11 October 2024
Domain decomposition is used for saving computer memory by spatially dividing large burnup calculation problems between multiple calculation nodes. Each node handles particle transport only within its own domain, and particles crossing the domain boundaries are sent to another node to complete the history. The implementation in Serpent relies on a collision-based approach[1], i.e. the transfer is invoked when the particle undergoes a collision in a material which belongs to another domain. The decomposition affects only burnable materials divided into depletion zones using the div card. The most typical domain decomposition case is a full-core burnup calculation, in which the fuel is decomposed into separate domains to save memory. Interaction data for the other materials is shared by all parallel tasks.
The current implementation in Serpent 2 is relatively simple, and mainly designed for reactor cores. The number of domains is determined by the number of MPI tasks, and the division using the set dd input option. There are three division types:
- simple, based on depletion zone index, MODE 1.
- geometry-based division into sectors, MODE 2.
- geometry-based division into sectors and a central zone, MODE 3.
Notes:
- The methodology was implemented in version 2.1.31.
- The domain decomposition methodology allows the use of the restart capability from Serpent 2.1.32 version. The multiple restart files generated within a domain decomposition simulation can be read either in a subsequent domain decomposition simulation or within an automated depletion sequence, e.g., group-constant generation (matching the number of MPI tasks).
- From Serpent 2.1.32 version and on, the associated depletion output file in a domain decomposition simulation is not limited to parent materials.
Full-core example
The method is illustrated by a full-core example, where the depletion zone division and domain decomposition is defined by input lines:
% --- Domain decomposition ---------------------------------------------------- % --- Divide fuel into depletion zones: div fuel sep 1 % --- Domain decomposition (1 = simple, 2 = sector, 3 = sector + center) set dd 3 % -----------------------------------------------------------------------------
When the calculation is run with 5 MPI tasks, it produces the following output:
sss2 -mpi 5 core (...) ividing materials into depletion zones... Material fuel: - 63624 cells - 63624 depletion zones in total Sorting lists (this may take a while)... OK. Counting cells... OK. Decomposing 63624 divided materials into 5 domains: Domain 1: 12744 materials (20.0%) Domain 2: 12720 materials (20.0%) Domain 3: 12720 materials (20.0%) Domain 4: 12720 materials (20.0%) Domain 5: 12720 materials (20.0%) (...)
and a geometry plot that shows the domains in different colors (switching the current setup from MODE 3, to MODE 2, to MODE 1, respectively):
(a) sector-wise division plus central zone (MODE 3), (b) sector-wise division (MODE 2), (c) index-based division (MODE 1).
complete full-core input
% ----------------------------------------------------------------------------- set title "Monte Carlo performance benchmark" % Based on revision 1.2 (July 2011) of Monte Carlo performance benchmark: % % http://www.oecd-nea.org/dbprog/MonteCarloPerformanceBenchmark.htm % ----------------------------------------------------------------------------- % --- Neutron population and criticality cycles: set pop 500000 1000 200 set opti 1 % --- Plot: plot 3 1000 1000 0 -187.6 187.6 -187.6 187.6 % --- Thermal flux / fission rate mesh: mesh 2 996 904 mesh 3 996 996 % ----------------------------------------------------------------------------- % ----- Geometry -------------------------------------------------------------- % --- Cross section library file path: set acelib "sss_jeff31u.xsdata" % --- Boundary between hot and cold: surf 1 pz 0.0 % -- Water layers: cell 31 3 cold_water -1 cell 32 3 hot_water 1 % --- Fuel pin: pin 1 fuel 0.41 clad 0.475 fill 3 % --- Guide tube: pin 2 fill 3 0.56 clad 0.62 fill 3 % --- Pin lattice: lat 110 1 0.0 0.0 17 17 1.26 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 1 1 2 1 1 2 1 1 1 1 1 1 1 1 2 1 1 1 1 1 1 1 1 1 2 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 1 1 2 1 1 2 1 1 2 1 1 2 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 1 1 2 1 1 2 1 1 2 1 1 2 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 1 1 2 1 1 2 1 1 2 1 1 2 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 1 1 1 1 1 1 1 1 1 2 1 1 1 1 1 1 1 1 2 1 1 2 1 1 2 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 % --- assembly data: surf 1000 inf cell 110 4 fill 110 -1000 % --- Radial reflector: cell 51 5 lower_radial_refl -1 cell 52 5 upper_radial_refl 1 % --- Core lattice: lat 211 1 0.0 0.0 17 17 21.42 5 5 5 5 5 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 5 5 5 4 4 4 4 4 4 4 5 5 5 5 5 surf 211 sqc 0.0 0.0 182.07 cell 211 210 fill 211 -211 cell 212 210 lower_radial_refl 211 -1 cell 213 210 upper_radial_refl 211 1 % --- Core geometry: surf 11 pz -229.0 surf 12 pz -199.0 surf 13 pz -193.0 surf 14 pz -183.0 surf 15 pz 183.0 surf 16 pz 203.0 surf 17 pz 215.0 surf 18 pz 223.0 surf 20 cyl 0.0 0.0 187.6 surf 21 cyl 0.0 0.0 209.0 surf 22 cyl 0.0 0.0 229.0 surf 23 cyl 0.0 0.0 249.0 cell 1 0 bottom_plate -22 11 -12 cell 2 0 bottom_nozzle -20 12 -13 cell 3 0 bottom_fa -20 13 -14 cell 4 0 lower_radial_refl 20 -21 12 -14 cell 5 0 fill 210 -21 14 -15 cell 6 0 upper_radial_refl 20 -21 15 -17 cell 7 0 top_fa -20 15 -16 cell 8 0 top_nozzle -20 16 -17 cell 9 0 cold_water 21 -22 12 -17 cell 10 0 top_plate -22 17 -18 cell 11 0 vessel 22 -23 11 -18 cell 666 0 outside 23 11 -18 cell 667 0 outside -11 cell 668 0 outside 18 % ----------------------------------------------------------------------------- % --- Materials --------------------------------------------------------------- mat fuel -10.062 burn 1 92234.03c 4.9476E-6 92235.03c 4.8218E-4 92236.03c 9.0402E-5 92238.03c 2.1504E-2 93237.03c 7.3733E-6 94238.03c 1.5148E-6 94239.03c 1.3955E-4 94240.03c 3.4405E-5 94241.03c 2.1439E-5 94242.03c 3.7422E-6 95241.03c 4.5041E-7 95242.03c 9.2301E-9 95243.03c 4.7878E-7 96242.03c 1.0485E-7 96243.03c 1.4268E-9 96244.03c 8.8756E-8 96245.03c 3.5285E-9 42095.03c 2.6497E-5 43099.03c 3.2772E-5 44101.03c 3.0742E-5 44103.03c 2.3505E-6 47109.03c 2.0009E-6 54135.03c 1.0801E-8 55133.03c 3.4612E-5 60143.03c 2.6078E-5 60145.03c 1.9898E-5 62147.03c 1.6128E-6 62149.03c 1.1627E-7 62150.03c 7.1727E-6 62151.03c 5.4947E-7 62152.03c 3.0221E-6 63153.03c 2.6209E-6 64155.03c 1.5369E-9 8016.03c 4.5737E-2 mat clad -5.77 rgb 100 100 100 40000.03c 1.0 mat cold_water -0.74 moder lwtr 1001 rgb 100 150 200 1001.03c 2.000 8016.03c 1.000 5010.03c 6.490E-4 5011.03c 2.689E-3 mat hot_water -0.66 moder lwtr 1001 rgb 100 150 200 1001.03c 2.000 8016.03c 1.000 5010.03c 6.490E-4 5011.03c 2.689E-3 mat vessel -7.9 rgb 50 50 50 26000.03c -96.3 28000.03c -1.0 25055.03c -1.0 42000.03c -0.6 14000.03c -0.4 24000.03c -0.25 6000.03c -0.25 29000.03c -0.2 mat lower_radial_refl -4.32 moder lwtr 1001 rgb 100 100 100 1001.03c -0.0095661 8016.03c -0.0759107 5010.03c -3.08409E-4 5011.03c -1.40499E-5 26000.03c -0.6309028 28000.03c -0.0822917 25055.03c -0.0182870 14000.03c -0.0091435 24000.03c -0.1737269 mat upper_radial_refl -4.28 moder lwtr 1001 rgb 100 100 100 1001.03c -0.0086117 8016.03c -0.0683369 5010.03c -2.77638E-5 5011.03c -1.26481E-4 26000.03c -0.6367991 28000.03c -0.0830607 25055.03c -0.0184579 14000.03c -0.0092290 24000.03c -0.1753505 mat bottom_plate -7.184 moder lwtr 1001 1001.03c -0.0011505 8016.03c -0.0091296 5010.03c -3.70915E-6 5011.03c -1.68974E-5 26000.03c -0.6828925 28000.03c -0.0890729 25055.03c -0.0197940 14000.03c -0.0098970 24000.03c -0.1880429 mat bottom_nozzle -2.53 moder lwtr 1001 1001.03c -0.0245014 8016.03c -0.1944274 5010.03c -7.89917E-5 5011.03c -3.59854E-4 26000.03c -0.5386364 28000.03c -0.0702569 25055.03c -0.0156126 14000.03c -0.0078063 24000.03c -0.1483202 mat top_nozzle -1.746 moder lwtr 1001 1001.03c -0.0358870 8016.03c -0.2847761 5010.03c -1.15699E-4 5011.03c -5.27075E-4 26000.03c -0.4682990 28000.03c -0.0610825 25055.03c -0.0135739 14000.03c -0.0067869 24000.03c -0.1289519 mat top_plate -4.28 moder lwtr 1001 1001.03c -0.0086117 8016.03c -0.0683369 5010.03c -2.77638E-5 5011.03c -1.26481E-4 26000.03c -0.6367991 28000.03c -0.0830607 25055.03c -0.0184579 14000.03c -0.0092290 24000.03c -0.1753505 mat bottom_fa -3.044 moder lwtr 1001 1001.03c -0.0162913 8016.03c -0.1292776 5010.03c -5.25228E-5 5011.03c -2.39272E-4 40000.03c -0.8541393 mat top_fa -1.762 moder lwtr 1001 1001.03c -0.0292856 8016.03c -0.2323919 5010.03c -9.44159E-5 5011.03c -4.30120E-4 40000.03c -0.7377980 % --- Thermal scattering data therm lwtr lwj3.00t % ----------------------------------------------------------------------------- % --- Depletion history ------------------------------------------------------- % --- Decay and fission yield libraries: set declib "/xs/sss_jeff31.dec" set nfylib "/xs/sss_jeff31.nfy" % --- Irradiation cycle: set powdens 40.0E-3 dep butot 0.10 0.50 1.00 1.50 2.00 2.50 3.00 3.50 4.00 4.50 5.00 5.50 6.00 6.50 7.00 7.50 8.00 8.50 9.00 9.50 10.00 10.50 11.00 11.50 12.00 12.50 13.00 13.50 14.00 14.50 15.00 17.50 20.00 22.50 25.00 27.50 30.00 32.50 35.00 37.50 40.00 % --- Isotope list for inventory calculation: set inventory all % --- Depletion output: set depout 2 % --- Material volumes: set mcvol 10000000000 % ----------------------------------------------------------------------------- % --- Domain decomposition ---------------------------------------------------- % --- Divide fuel into depletion zones: div fuel sep 1 % --- Domain decomposition (1 = simple, 2 = sector, 3 = sector + center) set dd 3 % -----------------------------------------------------------------------------
References
- ^ García, M., Leppänen, J. and Sánchez-Espinoza, V. "A Collision-based Domain Decomposition scheme for large-scale depletion with the Serpent 2 Monte Carlo code." Ann. Nucl. Energy 152 (2021) 108026.