Abstract

This work presents the results of the exact computation of (180)3 = 5,832,000 third-order mixed sensitivities of the leakage response of a polyethylene-reflected plutonium (PERP) experimental benchmark with respect to the benchmark’s 180 microscopic total cross sections. This computation was made possible by applying the Third-Order Adjoint Sensitivity Analysis Methodology developed by Cacuci. The numerical results obtained in this work revealed that many of the 3rd-order sensitivities are significantly larger than their corresponding 1st- and 2nd-order ones, which is contrary to the widely held belief that higher-order sensitivities are all much smaller and hence less important than the first-order ones, for reactor physics systems. In particular, the largest 3rd-order relative sensitivity is the mixed sensitivity of the PERP leakage response with respect to the lowest energy-group (30) total cross sections of 1H (“isotope 6”) and 239Pu (“isotope 1”). These two isotopes are shown in this work to be the two most important parameters affecting the PERP benchmark’s leakage response. By comparison, the largest 1st-order sensitivity is that of the PERP leakage response with respect to the lowest energy-group total cross section of isotope 1H, having the value , while the largest 2nd-order sensitivity is . The 3rd-order sensitivity analysis presented in this work is the first ever such analysis in the field of reactor physics. The consequences of the results presented in this work on the uncertainty analysis of the PERP benchmark’s leakage response will be presented in a subsequent work.

Highlights

  • The accompanying Part I [1] has reported the exact mathematical expressions of the 3rd-order sensitivities of the leakage response of the OECD/NEA subcritical polyethylene-reflected plutonium metal fundamental physics benchmark [2] with respect to the benchmark’s group-averaged microscopic total cross sections

  • The numerical results obtained in this work revealed that many of the 3rd-order sensitivities are significantly larger than their corresponding 1st- and 2nd-order ones, which is contrary to the widely held belief that higher-order sensitivities are all much smaller and less important than the first-order ones, for reactor physics systems

  • The consequences of the results presented in this work on the uncertainty analysis of the polyethylene-reflected plutonium (PERP) benchmark’s leakage response will be presented in a subsequent work

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Summary

Introduction

The accompanying Part I [1] has reported the exact mathematical expressions of the 3rd-order sensitivities of the leakage response of the OECD/NEA subcritical polyethylene-reflected plutonium (acronym: PERP) metal fundamental physics benchmark [2] with respect to the benchmark’s group-averaged microscopic total cross sections. This work will present the numerical results obtained by using the formulas derived in [1] for the (180) third-order mixed sensitivities of the PERP’s leakage response with respect to the benchmark’s 180 group-averaged microscopic total cross sections. This work is organized as follows: Section 2 reports the numerical results for the 180 third-order “unmixed” sensitivities of the PERP’s leakage response with respect to the microscopic total cross sections, comparing them with the corresponding 1st- and 2nd-order sensitivities.

Methods
Results
Conclusion

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