Uncertainty and Sensitivity Analysis at Low Value of Determination Coefficient of Regression Analysis: Case of I-129 Release from RBMK-1500 SNF under Disposal Conditions
Abstract
:1. Introduction
1.1. Radionuclide Transport Model for RBMK-1500 SNF Disposal
1.1.1. Disposal System
- The bentonite material surrounding copper canister will be fully saturated by the groundwater by the time I-129 release from the SNF assemblies;
- As soon as a small initial canister defect becomes large, the void space within the canister (void between SNF assemblies and the channel in the canister insert) will be filled with the groundwater (app. 0.5 m3);
- Mechanisms (instant release of a part of the inventory and congruent release of the rest part of the inventory from degrading SNF matrix) take place in the canister and contribute to the radionuclide flux from the canister;
- Radionuclides released from SNF assemblies interact with a limited amount of water inside the canister, and dissolved radionuclide are transported from the canister in liquid form (mainly by diffusion);
- I-129 is released through the bentonite barrier and diffuses into the water flowing in a (conceptual) fracture intersecting the disposal tunnel.
1.1.2. Characterization of Model Behavior
2. Methodology/Approach for Extension of Sensitivity Analysis Based on CSM and CSV
2.1. Contribution to Sample Mean (CSM)
- The randomly (quasi-randomly) generated values of from its probability distribution function (PDF) are sorted in ascending order, generating the series of values , ;
- The output values corresponding to sorted input are obtained too , ;
- An ancillary variable Mi is calculated, whose values are calculated from as
- The function is obtained by normalization of , i.e., dividing the values by the sample mean of model output :
- Cumulative relative frequency (cumulative fraction) of the sorted input parameter lies in the interval [0,1] and could be calculated:
- Then, the function is plotted versus the cumulative relative frequency of . CSM also lie in the interval [0,1].
2.2. Contribution to Sample Variance (CSV)
- The output mean is computed, and each value of output is transformed by subtracting the mean value . The transformed output has zero mean value.
- The randomly (quasi-randomly) generated values of input are sorted in ascending order, generating the series of values , , and the corresponding set of the transformed outputs is obtained , .
- Function CSV is obtained as follows
- Cumulative relative frequency (cumulative fraction) of the sorted input parameter lies in the interval [0,1] and could be calculated by Equation (4).
2.3. Revised Mean and Variance Ratio Functions
- The mean of model output is computed.
- The generated values of the input Xi are sorted in ascending order, generating the series of values , , and the corresponding set of model output values , is obtained.
- Cumulative fractions of the input parameter lying in the interval [0,1] are defined:
- The mean ratio function and variance ratio function for can be estimated by the following expressions
3. Results and Discussion
3.1. CSM and CSV Plots for I-129 Flux
3.2. Effect of Parameter Range Reduction on Mean and Variance of I-129 flux
- on mean I-129 flux at time t = 5 × 104 (peak time),
- on the variance of I-129 flux at time t = 5 × 104 (peak time),
- on mean flux over time.
- impact of increasing the lower bounding value and decreasing upper bounding value,
- impact of increasing the lower bounding value while maintaining the original upper bounding value,
- impact of decreasing the upper bounding value while maintaining the original lower bounding value.
3.2.1. Mean Ratio Function
- (a)
- a plot of HM keeping the lower bounding value of input parameter at q1 = 0 and varying the upper bounding value (from q2 = 0 to q2 = 1);
- (b)
- a plot of HM keeping the upper bounding value of input parameter fixed at q2 = 1 and varying the lower bounding value (from q1 = 0 to q1 = 1).
3.2.2. Variance Ratio Function
- (a)
- reduced upper bound and
- (b)
- increased lower bound of the range of each parameter (at t5 = 5 × 104 years corresponding to the time of maximal mean flux).
3.3. Effect of Parameter Uncertainty Reduction on Mean Flux over Time
3.4. Summary of Discussion
4. Conclusions
- The CSM identified defect size enlargement time on the I-129 time-dependent flux to have greater importance relative to the effective diffusivity in bentonite and instant release fraction of I-129 (identified in regression analysis) at earlier time points (for a period of 5 × 103–5 × 104 years after the repository closure). This importance ranking overcame the results from the regression analysis.
- The importance of defect size enlargement time was confirmed with the CSV method; its largest contribution to the variance of I-129 flux into the geosphere occurred at a time from 5 × 103–104 years after repository closure.
- Soon after the onset of radionuclide release, the most significant contributing parameter to the mean flux and its variance was effective diffusivity of I-129 in bentonite. For longer periods (up to 1 Million years after repository closure), the SNF dissolution rate was observed as the most significant contributor to the mean flux and its variance. These observations were in line with the results of the regression analysis.
- At t = 5 × 104 years after repository closure (time of maximal mean flux), the most significant contributor to the mean flux was the SNF dissolution rate; however, the most significant contributor to flux variance was the defect size enlargement time.
- The effect of decreased mean flux before t = 5 × 104 years after repository closure was observed from reduced defect size enlargement time uncertainty: if the lowest bounding value of the defect size enlargement time is increased to be 4.6 × 104 years (parameter value at q1 = 0.65), then the mean flux at t = 5 × 103–2 × 104 years would be lower. Almost no effect on the mean flux would occur at t = 5 × 104 years after repository closure. If such input parameter range is not justified, then the increase to q1 < 0.65 would lead to a lower mean at earlier time points and an increased mean (to some extent) at t = 5 × 104 years after repository closure.
- If justification of the upper bounding value of the defect size enlargement time would lead to a value less than 4.6 × 104 years (parameter value at q2 less than 0.65), this would result in a decreased mean flux at t = 5 × 104 years after the repository closure would be expected; however, this would cause increase in the mean flux at earlier time points. Fixing the upper bounding value of Tlarge to a value at q2 = 0.6 would lead to the lower mean flux at t = 5 × 104 years, but at earlier time t = 1 × 104 years, t = 2 × 104 years, the mean of flux would be greater by a factor of ~ 1.5.
- The effect of decreased mean flux in the long-term (up to 1 million years after closure) was observed in case of a justified reduction of the upper bound of the SNF dissolution rate only. Reducing parameter SNF DR uncertainty range from [10−8, 10−6] 1/year to [10−8, 5.7 × 10−7] 1/year (q2 = 0.8) would lead to a decrease of mean flux by at least a factor of 1.14.
- CSM, CSV plots, and derived mean (variance) ratios have the potential to be applied more widely in the context of radioactive waste disposal as a means of complementing regression-based sensitivity analyses.
Author Contributions
Funding
Conflicts of Interest
References
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Parameter | PDF 1 | PDF Type | ||
---|---|---|---|---|
Nominal Value (Reference Value) | Lower Bound | Upper Bound | ||
Defect size enlargement time (Tlarge) (years) [30] | 104 | 103 | 105 | Triangular |
SNF matrix dissolution rate (SNF DR) (1/year) [31] | 10−7 | 10−8 | 10−6 | Triangular |
Equivalent groundwater flow rate around the canister (Qeq) (m3/year) [32] | 9 × 10−4 | 9 × 10−4 (p = 0.9) | 4 (p = 0.1) | Discrete |
Instant release fraction (IRF) of I-129 inventory (%) [31] | 2 | 0 | 5 | Triangular |
Effective diffusivity of I-129 in bentonite (De) (m2/s) [33] | 1 × 10−11 | 3 × 10−12 (p = 0.15) 1 × 10−11 (p = 0.7) 3 × 10−11 (p = 0.15) | Discrete |
Time, Years | Most Important Parameters by Regression Analysis [21] | Most Important Parameters by CSM | Most Important Parameters by CSV | Notes |
---|---|---|---|---|
t1 = 1 × 103 years | De, IRF | De, IRF | De | IRF, Qeq are also significant based on CSV |
t2 = 5 × 103 years | De, IRF | Tlarge, De, IRF | Tlarge, Qeq, De, IRF | Small Qeq values and De, IRF, are important to some extent |
t3 = 104 years | De, IRF, Tlarge | Tlarge, IRF | Tlarge, IRF | The same for both (CSM and CSV) methods |
t4 = 2 × 104 years | Tlarge, De | Tlarge | Tlarge | Low importance of SNF DR, De, IRF |
t5 = 5 × 104 years | SNF DR, Tlarge | Tlarge, SNF DR, IRF | Tlarge | Ranking of the most important parameter is the same for both (CSM and CSV) methods |
t6 = 105 years | SNF DR, Tlarge | SNF DR, Tlarge | Tlarge | Ranking of the most important parameter differs |
t7 = 2×105 years | SNF DR | SNF DR | SNF DR | Based on CSM, the rest parameters are non-influential and could be assigned a fixed value without influence on the mean flux for this time. Smallest and largest values of SNF DR are more contributing to flux variance; low importance of Tlarge based on CSV |
t8 = 5 × 105 years | SNF DR | SNF DR | SNF DR | |
t9 = 106 years | SNF DR | SNF DR | SNF DR |
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Narkuniene, A.; Poskas, P.; Justinavicius, D. Uncertainty and Sensitivity Analysis at Low Value of Determination Coefficient of Regression Analysis: Case of I-129 Release from RBMK-1500 SNF under Disposal Conditions. Minerals 2019, 9, 521. https://doi.org/10.3390/min9090521
Narkuniene A, Poskas P, Justinavicius D. Uncertainty and Sensitivity Analysis at Low Value of Determination Coefficient of Regression Analysis: Case of I-129 Release from RBMK-1500 SNF under Disposal Conditions. Minerals. 2019; 9(9):521. https://doi.org/10.3390/min9090521
Chicago/Turabian StyleNarkuniene, Asta, Povilas Poskas, and Darius Justinavicius. 2019. "Uncertainty and Sensitivity Analysis at Low Value of Determination Coefficient of Regression Analysis: Case of I-129 Release from RBMK-1500 SNF under Disposal Conditions" Minerals 9, no. 9: 521. https://doi.org/10.3390/min9090521