This scientifi c and technical communication examines the physical mechanisms of the change in the isotopic composition of regenerated uranium recycled in VVER-1000 and -1200 fuels. Modeling of the Multiple Recycling of Regenerated Uranium. An approach based on matched modeling of the neutron-physical processes occurring during the irradiation of fuel in a reactor and molecular-selective mass transfer in separative cascades of gas centrifuges for the enrichment of uranium is used to investigate the mechanisms. The approach is very similar to that used in [1, 2]. Aside from the asymptotic case, where multiple recycling of regenerated uranium with dilution of natural uranium is accomplished without restrictions on the U content in low-enriched uranium, scenarios in the presence of such restrictions are analyzed. The following recycling sequence is considered [3]. The fuel in the initial load with prescribed enrichment of U fabricated from natural uranium is irradiated in the reactor core, allowed to decay for 10 yr, and reprocessed. Natural uranium is the second feed stream of the cascade, making it possible to dilute the regenerated uranium and lower the content of U in the product. The fuel obtained in this manner is once again irradiated, after which it is allowed to decay and then reprocessed. Next, the cycle is repeated. In all, fi ve successive recycles of the regenerated uranium are considered. Multiple recycling of regenerated uranium by burnup to 48 MW·days/kg with different restrictions on the U content in low-enrichment uranium was analyzed fi rst. Three cases were considered. The U concentration did not exceed 2·10 wt.% in the fi rst case and 5·10 wt.% in the second; there were no restrictions on the U concentration in the third. The effect of U was compensated by additional enrichment with U and reactivity compensation factor 0.29 [3, 4]. The restriction on the U concentration in low-enrichment uranium at the level 0.1% was examined separately; compensation of the parasitic absorption of neutrons by this isotope is not required below this level. The burnup considered in the present work corresponds to the maximum unfavorable situation from the standpoint of the content of U and U in the regenerated uranium. For example, burnup 48 MW·days/kg with 4% enrichment is reached only in individual fuel assemblies. The average burnup with such enrichment equals 43 MW·days/kg. A model of a quasi-ideal cascade, widely used in the theory of separation of multicomponent isotopic mixtures, is used for numerical modeling of the enrichment of regenerated uranium in a cascade with two feed streams (natural uranium and regenerated uranium) [5]. This model is used as a replacement for an ideal cascade, often used in the evaluation of the parameters of cascades for enrichment of natural uranium, because regenerated uranium, in contrast to natural uranium, cannot be regarded as a binary mixture, since it contains, aside from U, a fourth component – U, U, U, or U [6]. The neutron physical processes were calculated by the Monte Carlo method using the MCNP5 code (USA).
Read full abstract