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Research Articles

Space-Dependent Calculation of the Multiplicity Moments for Shells With the Inclusion of Scattering

ORCID Icon, ORCID Icon & ORCID Icon
Pages 2030-2046 | Received 20 Sep 2022, Accepted 01 Feb 2023, Published online: 09 Mar 2023

Figures & data

Fig. 1. Illustration of the neutron paths for μ>μcr and for μ<μcr in the shell with a central cavity.

Fig. 1. Illustration of the neutron paths for μ>μcr and for μ<μcr in the shell with a central cavity.

Fig. 2. First, second, and third moments of the number of neutrons emitted from a solid sphere for a distributed source (dashed lines, blue) and a central point source (solid lines, red) as functions of the outer radius R.

Fig. 2. First, second, and third moments of the number of neutrons emitted from a solid sphere for a distributed source (dashed lines, blue) and a central point source (solid lines, red) as functions of the outer radius R.

TABLE I Input Parameters Used in the Calculations

Fig. 3. First, second, and third moments of the number of neutrons emitted from a solid sphere (blue lines, marked with circles) and a shell with an inner radius r0=0.1 mean free path (red lines, marked with triangles), both with a central source. Reff is the outer radius in optical units for both cases.

Fig. 3. First, second, and third moments of the number of neutrons emitted from a solid sphere (blue lines, marked with circles) and a shell with an inner radius r0=0.1 mean free path (red lines, marked with triangles), both with a central source. Reff is the outer radius in optical units for both cases.

Fig. 4. The first three factorial moments as functions of the radius of a pure 235U sphere, with varying degrees βs of elastic scattering being included. Left column: full range (R between 0 and 7 cm); right column: half range (R between 0 and 3.5 cm).

Fig. 4. The first three factorial moments as functions of the radius of a pure 235U sphere, with varying degrees βs of elastic scattering being included. Left column: full range (R between 0 and 7 cm); right column: half range (R between 0 and 3.5 cm).

Fig. 5. Comparison of measured and calculated first, second, and third moments of the number of neutrons emitted from the Rocky Flats Shells for four different outer radii and with an inner radius of 2.0126 cm.

Fig. 5. Comparison of measured and calculated first, second, and third moments of the number of neutrons emitted from the Rocky Flats Shells for four different outer radii and with an inner radius of 2.0126 cm.

TABLE II Macroscopic Cross Sections of the Rocky Flats Shells at 1 MeV*

TABLE III Factorial Moments of the Rocky Flats Shells at 1 MeV

Fig. 6. Comparison of measured and calculated first, second, and third moments of the number of neutrons emitted from the Rocky Flats Shells for four different outer radii and with an inner radius of 2.0126 cm. In the calculated values, the material properties correspond to those of the isotopic composition of the Rocky Flats Shells at a neutron energy of 1 MeV.

Fig. 6. Comparison of measured and calculated first, second, and third moments of the number of neutrons emitted from the Rocky Flats Shells for four different outer radii and with an inner radius of 2.0126 cm. In the calculated values, the material properties correspond to those of the isotopic composition of the Rocky Flats Shells at a neutron energy of 1 MeV.