High-burnup Structure Formation¶
This model describes the formation of the high-burnup structure (HBS) through a
restructuring (phase transformation) law expressed in terms of effective
burnup. The model updates the Restructured volume fraction and is enabled
through the input option iHighBurnupStructureFormation.
The implementation follows Simulation::HighBurnupStructureFormation().
Activation¶
The model is executed only if:
iHighBurnupStructureFormation> 0
Option summary¶
0: not considered (no restructuring).
1: HBS formation model from Barani et al. (2020).
Inputs¶
The model uses:
iHighBurnupStructureFormation(input option)Effective burnup(sciantix variable): used as the independent variable for restructuringEffective burnupincrement: used as the integration increment
Main output:
Restructured volume fraction(sciantix variable)
Model formulation (case 1)¶
For option 1, the model defines two constants:
Avrami constant: \(A = 3.54\)
Transformation rate: \(k = 2.77 \times 10^{-7}\)
Two additional parameters are defined in the code:
resolution_layer_thickness= \(1.0\times 10^{-9}\) mresolution_critical_distance= \(1.0\times 10^{-9}\) m
Note
In the current implementation of Simulation::HighBurnupStructureFormation(),
the two “resolution” parameters are stored in the model parameter vector but are
not used in the restructuring update.
Restructuring rate¶
A burnup-dependent coefficient is computed as:
where \(B_{\mathrm{eff}}\) is the effective burnup (Effective burnup).
Update equation¶
The restructured volume fraction \(\alpha_r\) is updated using
solver.Decay(...) with effective burnup increment \(\Delta B_{\mathrm{eff}}\):
In other words, the evolution is written in a “decay + source” form with equal coefficients for the decay and source terms, as implemented in the solver.
Reference¶
Barani et al., Journal of Nuclear Materials 539 (2020) 152296. https://doi.org/10.1016/j.jnucmat.2020.152296