Sharen Herya Reafinola, Yanti Yulianti, S. Syafriadi
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摘要

利用REACT代码SRAC程序,用六角形几何模型计算了带过滤器和不带过滤器的裂变和中子捕获反应的速率。本研究使用铀235和铀238作为燃料。计算结果:材料1和材料3的裂变反应速率随铀235浓度百分比值的增加而增加。未加滤网的材料1的中子裂变反应速率最大值出现在富集1%的第二孔,为3.0747 × 10-2个反应/cm3。同时,过滤器中子捕获反应的速率随着U235含量的增加而增加,第5目富集1%,其值为9.8627 x10-2个反应/cm3。在第5个1%富集网格中,材料3上未过滤的中子裂变反应速率随着百分比的增加而增加,为9.4778 x10-2个反应/cm3。这是由于燃料销中铀235的富集百分比增加所致。而与过滤器相比,在材料1上使用百分比为1%的过滤器的捕获反应速率最高,为9.8181 x10-2个反应/cm3。
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Perhitungan Laju Reaksi Neutron Dalam Reaktor SCWR (Supercritical Water Reaktor) Model Perangkat (Assembly) Heksagonal Berbahan Bakar Uranium
Calculation of the rate of fission and neutron capture reactions with a filter and without a filter has been carried out using a hexagonal geometry model using the REACT code SRAC program. This research uses uranium-235 and uranium-238 as fuel. Calculation results The rate of fission reaction in material 1 and material 3 using a filter and without a filter increases with the increase in the percentage value of U235 enrichment. The highest value for the neutron fission reaction rate of material 1 without a filter is found in the second mesh with 1% enrichment, which is 3.0747x10-2 reactions/cm3s. Meanwhile, the rate of neutron capture reaction using a filter increases with the increase in the percentage of U235 with 1% enrichment of the 5th mesh, with a value of 9.8627 x10-2 reactions/cm3s. Then the unfiltered neutron fission reaction rate on material 3 increased along with the increasing percentage in the 5th 1% enrichment mesh, which was 9.4778 x10-2 reactions/cm3s. This is due to the increasing percentage of U235 enrichment in the fuel pin. While the rate of capture reaction using a filter on material 1 with a percentage of 1% of the second mesh has the highest value compared to the filter, which is 9.8181 x10-2 reactions/cm3s.
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