Resolution of the Generalized Eigenvalue Problem in the Neutron Diffusion Equation Discretized by the Finite Volume Method

<table class="table-group" id="tab18"><tr><td><table class="table"><tr><td class="thead-hr" colspan="3"><hr/></td></tr><tr class="thead"><td align="left"> </td><td align="center" colspan="2">Structured mesh</td></tr><tr class="thead"><td align="left"> </td><td align="center">10 cm</td><td align="center">5 cm</td></tr><tr><td class="thead-hr" colspan="3"><hr/></td></tr><tr><td align="left">CELL+</td><td align="center">0:0:25.69</td><td align="center">0:10:54.5</td></tr><tr><td align="left">CELL−</td><td align="center">0:0:25.68</td><td align="center">0:11:23.11</td></tr><tr><td align="left">HOM</td><td align="center">0:0:25.77</td><td align="center">0:10:55.77</td></tr><tr><td align="left">LIN</td><td align="center">0:0:25.73</td><td align="center">0:10:43.59</td></tr><tr class="table-tr"><td colspan="3"><hr class="tbody-hr"/></td></tr></table></td></tr></table>

Langenbuch reactor computational time (h:min:s).

Abstract and Applied Analysis

tab18

Table 18

Table 18: Resolution of the Generalized Eigenvalue Problem in the Neutron Diffusion Equation Discretized by the Finite Volume Method 