Abstract
Because a large time spread in most crack initiation tests makes it a daunting task to predict the initiation time of cracking, a probabilistic model, such as the Weibull distribution, has been usually employed to model it. In this case, although it might be anticipated to develop a more reliable cracking model under ideal cracking test conditions (e.g., large number of specimen, narrow censoring interval, etc.), it is not straightforward to quantitatively assess the effects of these experimental conditions on model estimation uncertainty . Therefore, we studied the effects of some key experimental conditions on estimation uncertainties of the Weibull parameters through the Monte Carlo simulations. Simulation results suggested that the estimated scale parameter would be more reliable than the estimated shape parameter from the tests. It was also shown that increasing the number of specimen would be more efficient to reduce the uncertainty of estimators than the more frequent censoring.
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Abbreviations
- CDF:
-
Cumulative distribution function
- \( F\left( \cdot \right) \) :
-
Cumulative distribution function of Weibull distribution
- ECF:
-
End cracking fraction
- \( \hat{\eta } \) :
-
Estimator of Weibull scale parameter
- \( \hat{\beta } \) :
-
Estimator of Weibull shape parameter
- EVD:
-
Extreme value distribution
- EVDm :
-
Extreme value distribution for minima
- GEVD:
-
Generalized extreme value distribution
- iid:
-
Independent and identically distributed
- \( s_{i} \) :
-
Last censoring time of i th suspended specimen
- LCI:
-
Length of censoring interval
- \( L\left( \cdot \right) \) :
-
Likelihood function
- \( \mu \) :
-
Location parameter of generalized extreme value distribution
- \( l\left( \cdot \right) \) :
-
Log-likelihood function
- LB:
-
Lower bound
- \( c_{{j_{L} }} \) :
-
Lower bound time of censoring interval for j th cracking
- MLE:
-
Maximum likelihood estimation
- C:
-
Number of interval-censored cracked specimens
- S:
-
Number of suspended specimens
- PDF:
-
Probability density function
- \( g\left( \cdot \right) \) :
-
Probability density function of generalized extreme value distribution
- \( {\text{RE}}\left( \cdot \right) \) :
-
Relative error
- \( {\text{RE}}_{50\% } \) :
-
Relative error of median estimates
- \( {\text{RLCI}}_{90\% } \) :
-
Relative length of 90% confidence interval
- RTD:
-
Relative test duration
- \( \sigma \) :
-
Scale parameter of generalized extreme value distribution
- \( \eta \) :
-
Scale parameter of Weibull distribution
- \( \xi \) :
-
Shape parameter of generalized extreme value distribution
- \( \beta \) :
-
Shape parameter of Weibull distribution
- SCC:
-
Stress corrosion cracking
- t :
-
Time
- \( \eta_{\text{true}} \) :
-
True Weibull scale parameter
- \( \beta_{\text{true}} \) :
-
True Weibull shape parameter
- UB:
-
Upper bound
- \( c_{{j_{U} }} \) :
-
Upper bound time of censoring interval for jth cracking
- \( x \) :
-
Variable of generalized extreme value distribution
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Acknowledgements
This work was supported by the Nuclear Safety Research Program through the Korea Foundation of Nuclear Safety (KOFONS) granted financial resource from the Nuclear Safety and Security Commission (NSSC), Republic of Korea (No. 1403006), and was supported by “Human Resources Program in Energy Technology” of the Korea Institute of Energy Technology Evaluation and Planning (KETEP), who granted the financial resources from the Ministry of Trade, Industry & Energy, Korea. (No. 20164010201000).
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Park, J.P., Park, C., Bahn, C.B. (2019). A Statistical Analysis on Modeling Uncertainty Through Crack Initiation Tests. In: Jackson, J., Paraventi, D., Wright, M. (eds) Proceedings of the 18th International Conference on Environmental Degradation of Materials in Nuclear Power Systems – Water Reactors. The Minerals, Metals & Materials Series. Springer, Cham. https://doi.org/10.1007/978-3-030-04639-2_135
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DOI: https://doi.org/10.1007/978-3-030-04639-2_135
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