首页> 外文会议>International Symposium NUCEF >Calculation of OECD/NEA source convergence benchmark problem no.1 by using MCNP and solving fission matrix equation
【24h】

Calculation of OECD/NEA source convergence benchmark problem no.1 by using MCNP and solving fission matrix equation

机译:通过MCNP和求解裂变矩阵方程计算OECD / NEA源收敛基准问题No.1

获取原文

摘要

The OECD/NEA source convergence benchmark problem 1: checkerboard storage of assemblies is calculated by using the MCNP-4B continuous energy Monte Carlo code and JENDL3.2 library, Calculated results show that the fission source distributions for the thirty-six cases with various calculation conditions required in the benchmark are affected by the initial source distributions, and not converged because of the weak neutron coupling between fuel assemblies. In order to approximately estimate the converged source distribution, the fission matrix equation for the checkerboard storage is solved with the deterministic method of iterative calculations, where the multiplication factors for the isolated single assembly and the neutron interactions between two assemblies are calculated and applied to the matrix elements. Then we calculate the special case, that is, the assembly-averaged source levels are set to the fission matrix solution and the distributions inside assemblies are assumed to be cosine-like shapes as the initial fission source. Most of the source levels of the major assemblies for this case do not change at all as the generations increase. Thus the fission source distribution is obtained as almost converged.
机译:OECD / NEA源收敛基准测试1:通过使用MCNP-4B连续能量蒙特卡罗代码和JENDL3.2库来计算组件的棋盘存储。计算结果表明,裂变源分布为三十六例具有各种计算的案例基准测试中所需的条件受初始源分布的影响,并且由于燃料组件之间的弱中子耦合而不会收敛。为了大致估计会聚源分布,通过迭代计算的确定方法来解决棋盘存储器的裂变矩阵方程,其中计算和应用两个组件之间的倍增因子和两个组件之间的中子相互作用。矩阵元素。然后,我们计算特殊情况,即,组装平均源电平被设置为裂变矩阵溶液,并且假设组件内的分布是余弦形状作为初始裂变源。这种情况下主要组件的大多数源电平完全不会随着代层而改变。因此,获得裂变源分布几乎融合。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号