# Difference between revisions of "Variance reduction"

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== Test case == | == Test case == | ||

− | The test case is comprised of an isotropic, point-wise, low-energy neutron source, enclosed inside two cylindrical | + | The test case is comprised of an isotropic, point-wise, low-energy neutron source, enclosed inside two cylindrical shells made of steel and concrete. The geometry is in 2D for the sake of simplicity, but the same procedures apply to 3D problems as well. The geometry plot and complete input listing are provided below (click Expand to show). |

[[File:VR_Ref_geom1.png|frameless|200px]] | [[File:VR_Ref_geom1.png|frameless|200px]] | ||

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</div> | </div> | ||

+ | Notes on the input: | ||

+ | *Group constant generation is on by default in neutron transport simulations. This is switched off by [[#set_gcu|set gcu -1]]. | ||

== References == | == References == |

## Revision as of 15:21, 4 October 2019

Variance reduction in Serpent is based on standard weight-window techniques.^{[1]} The weight window mesh and additional parameters are defined using the wwin card. Serpent supports two mesh types:

- Weight-window mesh generated using the built-in response matrix method-based solver (see the wgen card).
- MCNP WWINP format weight window-mesh.
^{[2]}

This tutorial demonstrates the basic functionality of the built-in solver. The methodology is described in the related publications.^{[3]}^{[4]}

## Test case

The test case is comprised of an isotropic, point-wise, low-energy neutron source, enclosed inside two cylindrical shells made of steel and concrete. The geometry is in 2D for the sake of simplicity, but the same procedures apply to 3D problems as well. The geometry plot and complete input listing are provided below (click Expand to show).

**Completely made-up neutron shielding problem**

% --- Geometry (nested cylinders) surf 1 cyl 0.0 0.0 100.0 surf 2 cyl 0.0 0.0 120.0 surf 3 cyl 0.0 0.0 200.0 surf 4 cyl 0.0 0.0 300.0 surf 5 sqc 0.0 0.0 400.0 cell 1 0 air -1 cell 2 0 steel 1 -2 cell 3 0 air 2 -3 cell 4 0 concrete 3 -4 cell 5 0 air 4 -5 cell 6 0 outside 5 % --- Materials mat steel -8.00000E+00 rgb 100 100 100 6000.03c -4.00000E-04 14000.03c -5.00000E-03 15031.03c -2.30000E-04 16000.03c -1.50000E-04 24000.03c -1.90000E-01 25055.03c -1.00000E-02 26000.03c -7.01730E-01 28000.03c -9.25000E-02 mat air -1.20500E-03 rgb 255 255 220 6000.03c -1.24000E-04 7014.03c -7.55268E-01 8016.03c -2.31781E-01 18040.03c -1.28270E-02 mat concrete -2.30000E+00 rgb 180 180 180 1001.03c -1.00000E-02 8016.03c -5.32000E-01 11023.03c -2.90000E-02 13027.03c -3.40000E-02 14000.03c -3.37000E-01 20000.03c -4.40000E-02 26000.03c -1.40000E-02 % --- Source src 1 sp 0 0 0 se 1E-6 % Isotropic 1 eV point source set srcrate 1 % Normalize to unit source rate % --- Run parameters set nps 200000 50 set gcu -1 % Group constant generation off % --- Geometry plot: plot 3 500 500 % --- Mesh plot (flux) det F1 % Flux detector mesh 8 -4 F1 3 500 500 % Plot detector scores % --- Detectors det d1 dc 3 % Flux in airspace between walls surf s2 cyl 0.0 160.0 5.0 det d2 dtl s2 % Flux at y = 160 (between the walls) surf s3 cyl 0.0 350.0 5.0 det d3 dtl s3 % Flux at y = 350 (outside the concrete wall)

Notes on the input:

- Group constant generation is on by default in neutron transport simulations. This is switched off by set gcu -1.

## References

- ^ Lux, I. and Koblinger, L.
*"Monte Carlo Particle Transport Methods: Neutron and Photon Calculations."*CRC-Press, 1991. (available on-line). - ^ D. Pelowitz (ed.),
*“MCNP6 User’s Manual: Appendix C Mesh-Based WWINP, WWOUT, and WWONE File Format,”*LA-CP-13-00634, Los Alamos National Laboratory (2013). - ^ J. Leppänen
*"Response Matrix Method–Based Importance Solver and Variance Reduction Scheme in the Serpent 2 Monte Carlo Code."*Nucl. Technol. (in press) - ^ J. Leppänen and M. Jokipii.
*"Global Variance Reduction Scheme with Self-Adaptive Weight-Window Mesh in the Serpent 2 Monte Carlo Code."*In Proc. M&C2019, Portland, OR, Aug. 25-29, 2019.