文章摘要
姚亮,程仁山,吴璐,张伟,梅瑞斌,潘虎成.LOCA条件下包壳材料感应和电阻加热温升行为的对比研究[J].包装工程,2020,41(9):91-99.
YAO Liang,CHENG Ren-shan,WU Lu,ZHANG Wei,MEI Rui-bin,PAN Hu-cheng.Comparative Study on the Temperature Rise of the Cladding Material during Induction and Resistance Heating under LOCA Condition[J].Packaging Engineering,2020,41(9):91-99.
LOCA条件下包壳材料感应和电阻加热温升行为的对比研究
Comparative Study on the Temperature Rise of the Cladding Material during Induction and Resistance Heating under LOCA Condition
投稿时间:2019-03-02  修订日期:2020-05-10
DOI:10.19554/j.cnki.1001-3563.2020.09.014
中文关键词: LOCA  包壳材料  感应加热  电阻加热  温升行为
英文关键词: LOCA  cladding material  induction heating  resistance heating  temperature rise
基金项目:国防基础科研计划(JCKY2017201C016)
作者单位
姚亮 1.中国核动力研究设计院第一研究所成都 610041 
程仁山 2.东北大学 材料科学与工程学院沈阳 1108193.东北大学 材料各向异性与织构教育部重点实验室沈阳 110819 
吴璐 1.中国核动力研究设计院第一研究所成都 610041 
张伟 1.中国核动力研究设计院第一研究所成都 610041 
梅瑞斌 2.东北大学 材料科学与工程学院沈阳 110819 
潘虎成 2.东北大学 材料科学与工程学院沈阳 1108193.东北大学 材料各向异性与织构教育部重点实验室沈阳 110819 
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中文摘要:
      目的 使有限元模拟技术成为一种切实有效的研究方法,进而为高性能反应堆包壳材料的设计以及可能发生的LOCA(Loss of Coolant Accident)事故下的应急措施等提供理论依据。方法 基于COMSOL软件模拟分析典型锆合金核材料在LOCA条件下分别经感应加热和电阻加热后的温升行为。结果 感应加热条件下,锆材的体积内最高温度、体积平均温度与表面中心点温度的差值随着温度上升逐渐增大,在1200 ℃瞬时温度下,温度差值最高,约为41 ℃。电阻加热条件下,锆材的体积内最高温度、体积内中心温度与表面中心点温度在加热的整个阶段近乎重合,最大差值约为3 ℃;锆材的体积平均温度、表面平均温度与表面中心点温度的差值出现负值,最大差值约为30 ℃。结论 电阻加热和感应加热虽均适用于堆外研究反应堆失水事故下包壳材料所面临的超高温度及超快升温速率的工况模拟,但限于实际工况下电阻加热速率的滞后性,推荐使用感应加热进行后续的模拟研究工作。相关结果可为高性能反应堆包壳材料的设计提供必要的理论依据。
英文摘要:
      The work aims to enable the finite element simulation technology to become a practical and effective research method, and then provide the theoretical basis for the design of high-performance reactor cladding materials and possible emergency measures under the LOCA (Loss of Coolant Accident). Based on COMSOL software, the temperature rise of typical zirconium alloy nuclear materials after induction heating and resistance heating under LOCA conditions was simulated herein. The results showed that the difference between the highest temperature, the average volume temperature and the surface center temperature increased with the rise of temperature. At transient temperature of 1200 ℃, the temperature difference was the highest, about 41 ℃. Under the condition of resistance heating, the highest temperature in volume, the center temperature in volume and the surface center temperature of the zirconium material almost coincided with one another in the whole heating stage, with the maximum difference of about 3 ℃. The difference between the average volume temperature, the average surface temperature and the surface center temperature of zirconium material was negative, and the maximum difference was about 30 ℃. It is found that both resistance heating and induction heating are suitable for the simulation of ultra-high temperature and ultra-fast temperature rise rate for cladding materials under LOCA conditions. However, due to the lag of resistance heating rate under actual working conditions, induction heating is recommended for subsequent simulation experiments. The relevant results can provide necessary theoretical basis for the design of high-performance reactor cladding materials.
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