B. Thilak , P. Mangarjuna Rao , Jose Varghese , B.K. Sreedhar
{"title":"中型池型SFR能量CDA下大两相燃料气泡演化的数值分析","authors":"B. Thilak , P. Mangarjuna Rao , Jose Varghese , B.K. Sreedhar","doi":"10.1016/j.pnucene.2025.105729","DOIUrl":null,"url":null,"abstract":"<div><div>The two-phase fuel bubble behavior inside the liquid sodium pool under energetic core disruptive accident (CDA) is an essential consideration in the safety analysis of sodium fast reactors (SFR). The fuel bubble expansion and the resultant reactor vessel pressurization during energetic CDA drive the enhanced actinide transport from the damaged core to the cover gas region and the liquid sodium release to the reactor containment building (RCB). A numerical model is developed to evaluate the fuel bubble behavior by considering the sodium entrainment and the fuel-sodium heat transfer in a medium-sized pool type SFR. The model is validated with relevant benchmark experimental results. Under energetic CDA conditions, the fuel bubble mass typically varies between 1000 and 3000 kg, and the initial fuel bubble temperature ranges from 4200 to 4700 K. The parametric analysis with these input values shows that the sodium entrainment at the bubble-pool interface and the fuel bubble behavior are more sensitive to the initial fuel bubble temperature or superheat than the fuel bubble mass. The time period for the fuel bubble's first expansion-compression cycle range between 600 and 800 ms. The equilibrium or quasi-static pressure under adiabatic condition (i.e. without sodium entrainment and fuel-sodium heat transfer) for the 1000 kg-4200 K case is 1.57 × 10<sup>5</sup> Pa. Results also show that the sodium vapor partial pressure dominates the total fuel bubble pressure in the 1000 kg-4200 K case when the sodium entrainment and the fuel-sodium heat transfer effects are included. As a result, the quasi-static pressure in the reactor vessel increases to 3.0 × 10<sup>5</sup> Pa. The fuel bubble-sodium pool interface velocity history which dictates the actinide upward displacement from the core region is evaluated as a function of initial fuel bubble temperature and mass. The maximum fuel bubble-sodium pool interface velocity for the input values considered is 35 ms<sup>−1</sup>. A mechanistic evaluation of the reactor vessel pressure history after the completion of bubble expansion shows that the radiation heat transfer and the fuel vapor condensation reduce the reactor vessel pressure from the quasi-static to the ambient pressure within 10 s. The evaluated velocity and pressure histories would serve as inputs for the mechanistic estimation of in-vessel and in-containment accident source terms due to the fuel bubble expansion under energetic CDA scenario in SFR.</div></div>","PeriodicalId":20617,"journal":{"name":"Progress in Nuclear Energy","volume":"185 ","pages":"Article 105729"},"PeriodicalIF":3.3000,"publicationDate":"2025-03-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Numerical analysis of a large two phase fuel bubble evolution under energetic CDA in a medium-sized pool type SFR\",\"authors\":\"B. Thilak , P. Mangarjuna Rao , Jose Varghese , B.K. Sreedhar\",\"doi\":\"10.1016/j.pnucene.2025.105729\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>The two-phase fuel bubble behavior inside the liquid sodium pool under energetic core disruptive accident (CDA) is an essential consideration in the safety analysis of sodium fast reactors (SFR). The fuel bubble expansion and the resultant reactor vessel pressurization during energetic CDA drive the enhanced actinide transport from the damaged core to the cover gas region and the liquid sodium release to the reactor containment building (RCB). A numerical model is developed to evaluate the fuel bubble behavior by considering the sodium entrainment and the fuel-sodium heat transfer in a medium-sized pool type SFR. The model is validated with relevant benchmark experimental results. Under energetic CDA conditions, the fuel bubble mass typically varies between 1000 and 3000 kg, and the initial fuel bubble temperature ranges from 4200 to 4700 K. The parametric analysis with these input values shows that the sodium entrainment at the bubble-pool interface and the fuel bubble behavior are more sensitive to the initial fuel bubble temperature or superheat than the fuel bubble mass. The time period for the fuel bubble's first expansion-compression cycle range between 600 and 800 ms. The equilibrium or quasi-static pressure under adiabatic condition (i.e. without sodium entrainment and fuel-sodium heat transfer) for the 1000 kg-4200 K case is 1.57 × 10<sup>5</sup> Pa. Results also show that the sodium vapor partial pressure dominates the total fuel bubble pressure in the 1000 kg-4200 K case when the sodium entrainment and the fuel-sodium heat transfer effects are included. As a result, the quasi-static pressure in the reactor vessel increases to 3.0 × 10<sup>5</sup> Pa. The fuel bubble-sodium pool interface velocity history which dictates the actinide upward displacement from the core region is evaluated as a function of initial fuel bubble temperature and mass. The maximum fuel bubble-sodium pool interface velocity for the input values considered is 35 ms<sup>−1</sup>. A mechanistic evaluation of the reactor vessel pressure history after the completion of bubble expansion shows that the radiation heat transfer and the fuel vapor condensation reduce the reactor vessel pressure from the quasi-static to the ambient pressure within 10 s. The evaluated velocity and pressure histories would serve as inputs for the mechanistic estimation of in-vessel and in-containment accident source terms due to the fuel bubble expansion under energetic CDA scenario in SFR.</div></div>\",\"PeriodicalId\":20617,\"journal\":{\"name\":\"Progress in Nuclear Energy\",\"volume\":\"185 \",\"pages\":\"Article 105729\"},\"PeriodicalIF\":3.3000,\"publicationDate\":\"2025-03-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Progress in Nuclear Energy\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0149197025001271\",\"RegionNum\":3,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"NUCLEAR SCIENCE & TECHNOLOGY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Progress in Nuclear Energy","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0149197025001271","RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"NUCLEAR SCIENCE & TECHNOLOGY","Score":null,"Total":0}
Numerical analysis of a large two phase fuel bubble evolution under energetic CDA in a medium-sized pool type SFR
The two-phase fuel bubble behavior inside the liquid sodium pool under energetic core disruptive accident (CDA) is an essential consideration in the safety analysis of sodium fast reactors (SFR). The fuel bubble expansion and the resultant reactor vessel pressurization during energetic CDA drive the enhanced actinide transport from the damaged core to the cover gas region and the liquid sodium release to the reactor containment building (RCB). A numerical model is developed to evaluate the fuel bubble behavior by considering the sodium entrainment and the fuel-sodium heat transfer in a medium-sized pool type SFR. The model is validated with relevant benchmark experimental results. Under energetic CDA conditions, the fuel bubble mass typically varies between 1000 and 3000 kg, and the initial fuel bubble temperature ranges from 4200 to 4700 K. The parametric analysis with these input values shows that the sodium entrainment at the bubble-pool interface and the fuel bubble behavior are more sensitive to the initial fuel bubble temperature or superheat than the fuel bubble mass. The time period for the fuel bubble's first expansion-compression cycle range between 600 and 800 ms. The equilibrium or quasi-static pressure under adiabatic condition (i.e. without sodium entrainment and fuel-sodium heat transfer) for the 1000 kg-4200 K case is 1.57 × 105 Pa. Results also show that the sodium vapor partial pressure dominates the total fuel bubble pressure in the 1000 kg-4200 K case when the sodium entrainment and the fuel-sodium heat transfer effects are included. As a result, the quasi-static pressure in the reactor vessel increases to 3.0 × 105 Pa. The fuel bubble-sodium pool interface velocity history which dictates the actinide upward displacement from the core region is evaluated as a function of initial fuel bubble temperature and mass. The maximum fuel bubble-sodium pool interface velocity for the input values considered is 35 ms−1. A mechanistic evaluation of the reactor vessel pressure history after the completion of bubble expansion shows that the radiation heat transfer and the fuel vapor condensation reduce the reactor vessel pressure from the quasi-static to the ambient pressure within 10 s. The evaluated velocity and pressure histories would serve as inputs for the mechanistic estimation of in-vessel and in-containment accident source terms due to the fuel bubble expansion under energetic CDA scenario in SFR.
期刊介绍:
Progress in Nuclear Energy is an international review journal covering all aspects of nuclear science and engineering. In keeping with the maturity of nuclear power, articles on safety, siting and environmental problems are encouraged, as are those associated with economics and fuel management. However, basic physics and engineering will remain an important aspect of the editorial policy. Articles published are either of a review nature or present new material in more depth. They are aimed at researchers and technically-oriented managers working in the nuclear energy field.
Please note the following:
1) PNE seeks high quality research papers which are medium to long in length. Short research papers should be submitted to the journal Annals in Nuclear Energy.
2) PNE reserves the right to reject papers which are based solely on routine application of computer codes used to produce reactor designs or explain existing reactor phenomena. Such papers, although worthy, are best left as laboratory reports whereas Progress in Nuclear Energy seeks papers of originality, which are archival in nature, in the fields of mathematical and experimental nuclear technology, including fission, fusion (blanket physics, radiation damage), safety, materials aspects, economics, etc.
3) Review papers, which may occasionally be invited, are particularly sought by the journal in these fields.