The disadvantage factor for thermal neutrons in light-water moderated PuO
2-UO
2 and UO
2 square lattices were obtained from measurements of thermal neutron density distri-butions in a unit lattice cell, measured with Dy-Al wire detectors. The lattices consisted of 3.4w/0 PuO
2-UO
2 and 2.6w/0 UO
2 fuel rods, and the water-to-fuel volume ratio within the unit cell was parametrically changed. The PuO
2-UO
2 and UO
2 fuel rods were designed to realize equal fissile atomic number density.
The disadvantage factors thus measured were 1.36±0.07, 1.37±0.08, 1.40±0.06 and 1.38±0.06 in the PuO
2-UO
2 fuel lattices, and 1.30±0.06, 1.31±0.08, 1.30±0.08 and 1.33 ±O.06 in the UO
2, for water-to-fuel volume ratios, of 1.76, 2.00, 2.38 and 2.95, respec-tively. This difference in disadvantage factor between PuO
2-UO
2 and UO
2 fuel lattices corresponds to about 8%. Calculated results obtained by multigroup transport code LASER agreed well with the measured ones.
View full abstract