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50th Anniversary Invited Review

Progress and prospects of calculation methods for radiation shielding

, , , &
Pages 1339-1361 | Received 26 Feb 2014, Accepted 14 Feb 2015, Published online: 27 May 2015

Figures & data

Pie charts of summarized results for questionnaire survey.

Pie charts of summarized results for questionnaire survey.

Table 1. Technological roadmap of radiation shielding field.

Figure 2. Schematic diagram of the improved statistical geometry model.

Figure 2. Schematic diagram of the improved statistical geometry model.

Figure 3. k-infinity as a function of burn-up in a MOX-fueled BWR assembly of OECD/NEA/NSC benchmark on MOX-BWR.

Figure 3. k-infinity as a function of burn-up in a MOX-fueled BWR assembly of OECD/NEA/NSC benchmark on MOX-BWR.

Figure 4. Comparison among the calculation with and without the binding effect and the measurement on scattering photon spectrum from copper at the energy of 40 keV.

Figure 4. Comparison among the calculation with and without the binding effect and the measurement on scattering photon spectrum from copper at the energy of 40 keV.

Figure 5. Current status of PHITS development and distribution.

Figure 5. Current status of PHITS development and distribution.

Figure 6. List of models used in PHITS to simulate nuclear and atomic collisions.

Figure 6. List of models used in PHITS to simulate nuclear and atomic collisions.

Figure 7. Example of Sn angular quadrature set: ωω(μ,η). ω; direction vector of particle travel. μ η, ζ = (1-μ22)1/2; direction cosine of vector ω.

Figure 7. Example of Sn angular quadrature set: ω ≡ ω(μ,η). ω; direction vector of particle travel. μ η, ζ = (1-μ2-η2)1/2; direction cosine of vector ω.

Figure 8. Calculation geometries for one-, two-, and three-dimensional discrete ordinate transport codes.

Figure 8. Calculation geometries for one-, two-, and three-dimensional discrete ordinate transport codes.

Figure 9. Particle (neutron/photon) balance.

Note: ΦLμdy+ΦBηdx-ΦRμdy-ΦTηdx-tΦCdv=Qsdv+Sdv. ΦL; left boundary flux; ΦB; bottom boundary flux; ΦR; right boundary flux; ΦT; top boundary flux; μ,η; direction cosine; ΦC; flux at the center; Σt; total cross section; Qs; scattering source; S; fixed source.

Figure 9. Particle (neutron/photon) balance.Note: ΦLμdy+ΦBηdx-ΦRμdy-ΦTηdx-∑tΦCdv=Qsdv+Sdv. ΦL; left boundary flux; ΦB; bottom boundary flux; ΦR; right boundary flux; ΦT; top boundary flux; μ,η; direction cosine; ΦC; flux at the center; Σt; total cross section; Qs; scattering source; S; fixed source.

Figure 10. Various models for within-cell flux extrapolation along X-axis. (1)  α = 0.5, linear model; (2)  α  = 1.0, step model; (3) 0.5 ≦ α ≦ 1, weighted difference model; (4) 0.5 ≦ γ(θ) ≦ α,  θ weighted difference model.

Figure 10. Various models for within-cell flux extrapolation along X-axis. (1)  α = 0.5, linear model; (2)  α  = 1.0, step model; (3) 0.5 ≦ α ≦ 1, weighted difference model; (4) 0.5 ≦ γ(θ) ≦ α,  θ weighted difference model.

Figure 11. Schematic illustration of weighted/θ-weighted difference model to determine ΦC, ΦR-, and ΦT.

Figure 11. Schematic illustration of weighted/θ-weighted difference model to determine ΦC, ΦR-, and ΦT.

Figure 12. Convergence of flux solution observed in 20 × 20 mesh problem with a source region at the corner mesh interval.

Figure 12. Convergence of flux solution observed in 20 × 20 mesh problem with a source region at the corner mesh interval.

Table 2. Effect of Bremsstrahlung to gamma-ray buildup factors. (Maximum ratio of buildup with and without Bremsstrahlung between 0.5 and 40 mfp for each energy and material)

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