Difference between revisions of "Stochastic Implicit Euler burnup scheme"
(→Noteworthy things) |
|||
Line 3: | Line 3: | ||
== Background == | == Background == | ||
− | The theoretical background of the SIE scheme is described in <ref name=" | + | The theoretical background of the SIE scheme is described in <ref name="DufekANE13"/> |
== Implementation == | == Implementation == | ||
Line 14: | Line 14: | ||
== References == | == References == | ||
<references> | <references> | ||
− | <ref name=" | + | <ref name="DufekANE13">Dufek, J., Kotlyar, D. and Shwageraus, E. "''The stochastic implicit Euler method – A stable coupling scheme for Monte Carlo burnup calculations''", Ann. Nucl. Energy, [http://www.sciencedirect.com/science/article/pii/S0306454913002703 60 (2013) 295-300]</ref> |
</references> | </references> |
Revision as of 16:02, 26 September 2017
The Stochastic Implicit Euler (SIE) burnup scheme is an alternative burnup scheme that can be used if the traditional predictor-corrector burnup schemes in Serpent exhibit unstable behavior.
Background
The theoretical background of the SIE scheme is described in [1]
Implementation
Usage
Noteworthy things
- No neutron transport solution is actually calculated using the final concentrations for a certain point.
References
- ^ Dufek, J., Kotlyar, D. and Shwageraus, E. "The stochastic implicit Euler method – A stable coupling scheme for Monte Carlo burnup calculations", Ann. Nucl. Energy, 60 (2013) 295-300