Coupled multi-physics calculations: Difference between revisions

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where <math>P^{n}</math> is the unrelaxed power distribution tallied on iteration <math>n</math>, <math>P_{\mathrm{rel}}^{n-1}</math> is the relaxed power distribution after the previous iteration, <math>s_{i}</math> is the active neutron population simulated on iteration <math>i</math> and <math>d</math> is an underrelaxation factor that can be defined by the [[Input syntax manual#set relfactor|set relfactor]] option.
where <math>P^{n}</math> is the unrelaxed power distribution tallied on iteration <math>n</math>, <math>P_{\mathrm{rel}}^{n-1}</math> is the relaxed power distribution after the previous iteration, <math>s_{i}</math> is the active neutron population simulated on iteration <math>i</math> and <math>d</math> is an underrelaxation factor that can be defined by the [[Input syntax manual#set relfactor|set relfactor]] option.
== Output ==

Revision as of 16:31, 1 December 2015

External coupling

Iteration

Power relaxation

Serpent relaxes the power distribution calculated in the iterations using the stochastic approximation based method, where the power distribution at iteration n is calculated by

Preln=Preln1sni=1nsnd(Preln1Pn),

where Pn is the unrelaxed power distribution tallied on iteration n, Preln1 is the relaxed power distribution after the previous iteration, si is the active neutron population simulated on iteration i and d is an underrelaxation factor that can be defined by the set relfactor option.

Output