Issue 
EPJ Nuclear Sci. Technol.
Volume 4, 2018
Special Issue on 4th International Workshop on Nuclear Data Covariances, October 2–6, 2017, Aix en Provence, France – CW2017



Article Number  42  
Number of page(s)  7  
Section  Applied Covariances  
DOI  https://doi.org/10.1051/epjn/2018023  
Published online  14 November 2018 
https://doi.org/10.1051/epjn/2018023
Regular Article
Sensitivity and uncertainty analysis of β_{eff} for MYRRHA using a Monte Carlo technique
^{1}
Institute for Advanced Nuclear Systems, Belgian Nuclear Research Centre (SCK∙CEN),
Boeretang 200,
2400
Mol,
Belgium
^{2}
JPARC Center, Japan Atomic Energy Agency (JAEA),
24, Shirakata, Tokaimura,
Nakagun, Ibaraki
3191195,
Japan
^{3}
Data Bank, OECD Nuclear Energy Agency (NEA),
46, Quai Alphonse Le Gallo
92100
BoulogneBillancourt,
France
^{*} email: iwamoto.hiroki@jaea.go.jp
Received:
3
October
2017
Received in final form:
26
January
2018
Accepted:
14
May
2018
Published online: 14 November 2018
This paper presents a nuclear data sensitivity and uncertainty analysis of the effective delayed neutron fraction β_{eff} for critical and subcritical cores of the MYRRHA reactor using the continuousenergy Monte Carlo NParticle transport code MCNP. The β_{eff} sensitivities are calculated by the modified kratio method proposed by Chiba. Comparing the β_{eff} sensitivities obtained with different scaling factors a introduced by Chiba shows that a value of a = 20 is the most suitable for the uncertainty quantification of β_{eff}. Using the calculated β_{eff} sensitivities and the JENDL4.0u covariance data, the β_{eff} uncertainties for the critical and subcritical cores are determined to be 2.2 ± 0.2% and 2.0 ± 0.2%, respectively, which are dominated by delayed neutron yield of ^{239}Pu and ^{238}U.
© H. Iwamoto et al., published by EDP Sciences, 2018
This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
1 Introduction
To promote research and development of nuclear technology for various applications such as acceleratordriven systems, the GenerationIV reactors, and production of medical radioisotopes, the Belgian Nuclear Research Centre (SCK∙CEN) has proposed a cuttingedge research reactor combined with a proton accelerator, MYRRHA [1,2]. From the viewpoint of ensuring safety margins and reducing uncertainty in the MYRRHA design parameters, uncertainty quantification of reactor physics parameters is one of the most important tasks. To this end, nuclear data sensitivity and uncertainty (S/U) analyses have been extensively conducted for various MYRRHA core configurations using different calculation tools, geometric models, and nuclear data libraries [3–5]; these works have focused on the effective neutron multiplication factor k_{eff} as the primary neutronic safety parameter. The effective delayed neutron fraction β_{eff} can be ranked second in the list of neutronic safety parameters, because, besides of reactor kinetics, it is used to determine other design and safety parameters such as control rod worth and Doppler coefficient.
Continuousenergy Monte Carlo transport codes such as the Monte Carlo NParticle transport code MCNP [6] have been widely used in calculating not only k_{eff} but also its nuclear data sensitivities and kinetic parameters including β_{eff}. Although these codes have no capability to directly calculate the β_{eff} sensitivities owing to technical cumbersomeness, it is approximately expressed as a function of two different k_{eff} sensitivities by the socalled “kratio method [7]”; this indicates that uncertainty in β_{eff} can be quantified by the sensitivity method from the approximate β_{eff} sensitivities and evaluated covariance data of the nuclear data library. Although this method has been applied to the β_{eff} S/U analysis with a deterministic code SUSD3D for MYRRHA in the studies of Kodeli [8], within the seventh framework programme solving CHAllenges in Nuclear DAta (CHANDA) project [9], the analysis using the Monte Carlo transport code has not yet been tackled.
The kratio method itself is currently subdivided into two techniques: the prompt kratio method [7] and the modified kratio method proposed by Chiba [10,11]. Our previous study [12] by MCNP for a critical configuration of the VENUSF zeropower reactor at the SCK∙CEN site [13] demonstrated that the prompt kratio method involves large statistical uncertainty in the calculated β_{eff} sensitivities, and it would be currently difficult to reduce it only by increasing the number of neutron source histories. On the other hand, we also demonstrated that Chiba’s modified kratio method can alleviate this kind of problem.
In this study, we conducted the S/U analysis of β_{eff} for two types of MYRRHA configurations (i.e. critical mode and subcritical mode) using Chiba’s modified kratio method. β_{eff} and its sensitivities were calculated using the MCNP version 6.1.1, and JENDL4.0u [14,15] was used as the nuclear data library since it contains covariance data of delayed neutron yield .
2 MYRRHA core models
MYRRHA is designed to operate both in critical mode as a leadbismuth cooled fast reactor and in subcritical mode driven by 600MeV linear proton accelerator. Figures 1 and 2 show horizontal sectional views of the MYRRHA critical and subcritical configurations, respectively, which are homogenized on assembly level. The analyses were carried out for the critical and subcritical core configurations at beginning of cycle using the assemblybased homogenized models [16]. As illustrated, the critical and subcritical cores consist of 78 and 58 fuel assemblies (FAs), respectively; these are loaded with MOX with high Pu content. Besides FAs, the cores contains inpile sections for material testing, irradiation rigs for medical isotope production, and subassemblies containing safety and control rods. More details of the MYRRHA core design are given in Van den Eynde et al. [2].
Fig. 1
Horizontal sectional view of MYRRHA critical core. 
Fig. 2
Horizontal sectional view of MYRRHA subcritical core. 
3 Methodology
3.1 The β_{eff} sensitivities
Chiba’s modified kratio method describes β_{eff} as (1) where a(≠ 0) is a scaling factor; k is the effective multiplication factor calculated using the nuclear data library JENDL4.0u; is the effective multiplication factor calculated using the library in which is multiplied with (a + 1) (Appendix A). If a = − 1, then Chiba’s modified kratio method reduces to the prompt kratio method. The statistical uncertainty in β_{eff} propagated from δk and is expressed as follows: (2)
Here correlations were disregarded for the sake of simplicity. Using the definition of the sensitivity and equation (1), the β_{eff} sensitivity to parameter x is expressed as follows: (3) (4) where and are the sensitivities of k and to the parameter x, respectively. The statistical uncertainty in is expressed as (5)where and are the statistical uncertainties in and , respectively.
3.2 The β_{eff} uncertainties
Using the sensitivity profile obtained by the abovementioned methods, the β_{eff} uncertainty (standard deviation) due to nuclear data was evaluated by the uncertainty propagation law considering covariance, which is expressed as (6) where cov(z, g ; z^{′}, g^{′}) denotes a (g, g^{′} ; z, z^{′}) component of variance–covariance matrix (g, g^{′}: energy group, z, z^{′}: reaction), which was obtained by processing covariance data stored in JENDL4.0u with NJOY [17] and ERRORJ [18]. In this analysis, we employed eight parameters: fission, neutron capture, elastic scattering, inelastic scattering, and (n, 2n) reaction cross sections for major constituent materials: U, Pu, ^{241}Am, ^{16}O, ^{56}Fe, Pb, and ^{209}Bi, as well as prompt and delayed neutron yields and prompt neutron spectra for U and Pu isotopes. Here correlations between the reactions were also considered. Absence of covariance data for delayed neutron spectrum in JENDL4.0u did not allow us to estimate the contribution to the β_{eff} and confirm the conclusion made by Kodeli [19] on its significance.
4 Results and discussion
4.1 Effective delayed neutron fraction
Figure 3 shows comparisons of the calculated β_{eff} with different scaling factors (a = − 1, 1, 5, 10, 15, 20, and 25) for critical and subcritical cores. For each case, the k_{eff} value was calculated with 2.5 × 10^{8} histories (2.5 × 10^{5} source histories per cycle times 10^{3} cycles) in the MCNP calculation flow. Here the value calculated directly by the adjoint weighting method [20] for the same number of histories for critical and subcritical cores were estimated to be 323 ± 4 and 320 ± 4 pcm, respectively. It can be seen that the calculated statistical uncertainty decreases with increase in a, which was about a times smaller than that by the prompt k ratio method (a = − 1). In addition, we see that the calculated β_{eff} values exceeding their 1σ statistical uncertainties decrease as a increases. The similar trend can be seen in the previous study conducted for the VENUSF reactor using MCNP [12] and the benchmark analysis for fast neutron systems conducted by Chiba using the deterministic transport code CBG [10,21]; this reason is linked to the approximation used in equation (1).
Fig. 3
Comparison of the β_{eff} values for different scaling factors calculated using Chiba’s modified kratio method and that derived using the adjoint weighting method. The error bars and the band with pale blue color indicate 1σ statistical uncertainty. 
4.2 Sensitivity
Figures 4 and 5 show comparisons of the β_{eff} sensitivity profiles of ^{239}Pu fission and elastic scattering cross sections and ^{239}Pu and for the critical core with different scaling factors, respectively. As demonstrated in Iwamoto et al. [12], the statistical uncertainty at a = 1 is very large for all parameters except ; this is caused by the small difference between and (Appendix A). In contrast, the statistical uncertainty for is negligibly small for all the selected a values; this is owing to an approximation of (Appendix A). In addition, as with the β_{eff} values, decrease as a increases. However, it should be noted that the β_{eff} sensitivities change within about 1σ statistical uncertainties, while the nominal values of β_{eff} tend to exceed their 1σ statistical uncertainties. This indicates that the influence of the change in the β_{eff} sensitivities that results from increasing a on the uncertainty quantification of β_{eff} is expected to be small.
Figures 6 and 7 show the β_{eff} sensitivity profiles with respect to ^{239}Pu and ^{238}U reaction parameters for the critical core with a = 20, respectively, in which the statistical uncertainties appear to be sufficiently small. Table 1 summarizes the major β_{eff} sensitivities together with 1σ statistical uncertainties which were calculated with a = 20. As expected from the definition of β_{eff}, of major fuel materials (i.e. ^{239}Pu and ^{238}U) shows positive high sensitivities; in contrast, demonstrates negative sensitivities.
Fig. 4
Comparisons of β_{eff} sensitivity profile of ^{239}Pu fission (left) and elastic scattering (right) cross sections for the critical core with different scaling factors. The pale blue color around the blue line indicates 1σ statistical uncertainty. 
Fig. 5
Comparisons of β_{eff} sensitivity profile of ^{239}Pu (left) and (right) for the critical core with different scaling factors. The pale blue color around the blue line indicates 1σ statistical uncertainty. 
Fig. 6
^{239}Pu sensitivity profile for the critical core (a = 20). 
Fig. 7
^{238}U sensitivity profile for the critical core (a = 20). 
Major β_{eff} sensitivities with 1σ statistical uncertainities (a = 20, top 15).
4.3 Uncertainty
Table 2 lists the β_{eff} uncertainties due to nuclear data with different scaling factors for the critical and subcritical cores. Small scaling factors produce large both uncertainty values and their statistical uncertainties. This arises from the large sensitivities with large statistical uncertainties in the sensitivity profile as mentioned above; these statistical uncertainties can be reduced by increasing a. In addition, we see from Table 2 that, as a increases, the calculated total β_{eff} uncertainties for the critical and subcritical cores approach values of 2.2% and 2.0%, respectively.
Table 3 summarizes top 15 contributors to the β_{eff} uncertainty together with 1σ statistical uncertainties. Overall, the statistical uncertainties are small enough to identify the main contributors; namely, it can be concluded that the β_{eff} uncertainty is dominated by , followed by the elastic and inelastic scattering cross sections, for both cores.
Calculated β_{eff} uncertainty with different scaling factors.
Major contributors to the β_{eff} uncertainty with 1σ statistical uncertainties (a = 20, top 15).
5 Conclusion
We have conducted the nuclear data S/U analysis of β_{eff} for critical and subcritical cores of the MYRRHA reactor using the MCNP code. The β_{eff} sensitivities were calculated by Chiba’s modified kratio method. Although the nominal β_{eff} values appear to worsen as a increases, comparing the β_{eff} sensitivities and their statistical uncertainties calculated with different scaling factors shows that the β_{eff} sensitivities are more stable to the a change than the nominal β_{eff} values, and that a value of a = 20 is the most suitable for the uncertainty quantification. Using the calculated β_{eff} sensitivities and the JENDL4.0u covariance data, the β_{eff} uncertainties for the critical and subcritical cores have been determined to be 2.2 ± 0.2% and 2.0 ± 0.2%, respectively, which are dominated by of ^{239}Pu and ^{238}U.
To account for the optimal a value more clearly, further investigation, especially for nonlinear effects on and , is needed. Moreover, it would be of interest to compare our results with those previously performed using the deterministic code within the ongoing CHANDA project [8].
Appendix A Chiba’s modified kratio method
In equation (1), the effective neutron multiplication factor k_{eff} is obtained by solving the following neutron transport equation: (A.1) where is the angular neutron flux at position r with direction Ω and energy E; , , and are the transport, scattering, and fission operators, respectively, which are expressed as follows: (A.2) (A.4)
Here , , and represent the macroscopic total, scattering, and fission cross sections, respectively; χ and are total fission neutron spectrum and fission neutron yield, respectively. The effective multiplication factor in equation (1) is obtained by solving a fictitious neutron transport equation below: (A.5) where is the fictitious angular neutron flux obtained from equation (A.5); is a fission operator defined as follows: (A.6)
Using the relationship between prompt, delayed, and total neutrons: (A.7)
Equation (A.6) can be rewritten as (A.8)
It is noted that a corresponds to the fractional change of and that, if a = − 1 is adopted, only prompt neutrons are taken into account; in this case, Chiba’s modified kratio method reduces to the prompt kratio method [22]. In the MCNP calculation, is obtained using a nuclear data library in which is multiplied with (a + 1).
According to the adjointbased perturbation theory, the sensitivity of k to parameter x is expressed as [23] (A.9) where the bracket 〈 , 〉 represents integration over the phase space; is the adjoint function of ψ; λ = 1/k; Σ_{x} is the macroscopic cross section corresponding to parameter x; is the scattering operator for parameter x; is the fission operator for parameter x.
As an example of parameters except for , let us consider neutron capture cross section σ_{cap}. Since σ_{cap} involves neither scattering nor fission, the sensitivity of k to σ_{cap} is written by (A.10)
Further, the sensitivity of to σ_{cap} is written by (A.11) where and Σ_{cap} represents the macroscopic capture cross section. We see from equation (A.6) that, if a approaches zero, becomes ℱ; and hence , , and become ψ, , and k, respectively. Namely, if a small value is chosen for a, the difference between equations (A.10) and (A.11) is also small.
Similarly, the sensitivities of k and k to are written by (A.12) and (A.13)respectively. As with the case of other parameters, as a approaches zero, the limit of equation (A.13) of a equals equation (A.12). If a particular value is chosen for a to the extent that the approximations of , , and are applicable, equation (A.13) can be expressed as follows: (A.14)
Thus, if a = 1 is used, then is about twice as large as ; namely, it follows that there is a large difference between the two.
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Cite this article as: Hiroki Iwamoto, Alexey Stakovskiy, Luca Fiorito, Gert Van den Eynde, Sensitivity and uncertainty analysis of β_{eff} for MYRRHA using a Monte Carlo technique, EPJ Nuclear Sci. Technol. 4, 42 (2018)
All Tables
Major β_{eff} sensitivities with 1σ statistical uncertainities (a = 20, top 15).
Major contributors to the β_{eff} uncertainty with 1σ statistical uncertainties (a = 20, top 15).
All Figures
Fig. 1
Horizontal sectional view of MYRRHA critical core. 

In the text 
Fig. 2
Horizontal sectional view of MYRRHA subcritical core. 

In the text 
Fig. 3
Comparison of the β_{eff} values for different scaling factors calculated using Chiba’s modified kratio method and that derived using the adjoint weighting method. The error bars and the band with pale blue color indicate 1σ statistical uncertainty. 

In the text 
Fig. 4
Comparisons of β_{eff} sensitivity profile of ^{239}Pu fission (left) and elastic scattering (right) cross sections for the critical core with different scaling factors. The pale blue color around the blue line indicates 1σ statistical uncertainty. 

In the text 
Fig. 5
Comparisons of β_{eff} sensitivity profile of ^{239}Pu (left) and (right) for the critical core with different scaling factors. The pale blue color around the blue line indicates 1σ statistical uncertainty. 

In the text 
Fig. 6
^{239}Pu sensitivity profile for the critical core (a = 20). 

In the text 
Fig. 7
^{238}U sensitivity profile for the critical core (a = 20). 

In the text 
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