摘要
介绍了HTR-10高温气冷实验堆位于反射层中的控制棒和作为第二停堆系统的硼球孔道的反应性当量计算方法。用WIMS(积分输运碰撞几率法)程序、GAM、THERMOS程序方法产生控制棒区的截面。用一维离散坐标法程序ONESN1产生泄漏谱,在控制棒区的B4C从10群截面归并为4群截面;用二维离散坐标法程序SN2DB,在控制棒区(包括B4C、空隙和部分石墨反射层)考虑空间效应做均匀化4群截面。有控制棒和无控制棒情况下的Keff本征值,是由三维扩散有限差分程序CITATION在(θ,r,z)坐标系条件下做出的,并给出控制棒的反应性当量。
This paper describes the method used in the reactivity worth calculation forthe control rod and secondary shutdown system in high temperature gas-cooled reactorHTR-10, in which the control rods and the secondary shutdown system are located at thereflector and directly near the core. WIMS, GAM and THERMOS codes are used in theusual way to produce reflector and control rod region cross sections. The one-dimensionaldiscrete-ordinate's theory code ONESN1 is used for calculating the leakage spectrum intoeach control rod zone, in order to collapse the 10 group cross sections into 4 groups, andthe two-dimensional discrete-ordinates transport theory code SN2DB is used forhomogenizing the cross sections in the region that includes control rod zone and part reflector zone. The eigenvalues K.ff for the situations with and without insertion of the controlrod are calculated using the three-dimensional diffusion theory code CITATION in (θ,r,z) coordinate system.
出处
《清华大学学报(自然科学版)》
EI
CAS
CSCD
北大核心
1994年第6期39-45,共7页
Journal of Tsinghua University(Science and Technology)
基金
国家"八六三"高科技项目
关键词
气冷堆
停堆系统
反应性
control rod worth
HTGR
homogenizing cross section