#### Abstract

In this paper, the accelerator-driven subcritical reactor (ADSR) is simulated based on structure of the TRIGA-Mark II reactor. A proton beam is accelerated and interacts on the lead target. Two cases of using lead are considered here: firstly, solid lead is referred to as spallation neutron target and water as the coolant; secondly, molten lead is considered both as a target and as a coolant. The proton beam in the energy range from 115 MeV to 2000 MeV interacts with the lead to create neutrons. The neutron parameters as neutron yield *Y*_{n/p}, neutron multiplication factor *k*, the radial and axial distributions of the neutron flux in the core have been calculated by using MCNPX program. The results show that the neutron yield increases as the energies of the proton beam increases. When using the lead target, the differences between the neutron yield are from 4.2% to 14.2% depending on the energies of the proton beam. The proportion of uranium in the mixtures should be around 24% to produce an effective neutron multiplier factor greater than 0.9. The neutron fluxes are much higher than the same calculations for the TRIGA-Mark II reactor model using tungsten target and light water coolant.

#### 1. Introduction

The accelerator-driven subcritical reactor (ADSR) is a reactor that can generate energy and transmute radioactive wastes cleanly and safely [1]. One of the essential issues for an ADSR is that it must be designed so that it remains subcritical during operation.

For an ADSR, the neutron source used to maintain the operation of ADSR is generated by the interaction of high-energy proton beam with heavy targets, such as lead, tungsten, or a lead-bismuth mixture , as spallation neutron sources. The important parameters related to the design and operation of ADSR as neutron yield, neutron multiplication factor, or distributions of the neutron flux should be considered. ADSR can be fueled with nonenriched thorium, which is four times more abundant than uranium. In ADSR, unlike conventional uranium fuel, thorium is burnt, leaving much less radiotoxic waste and almost no plutonium. Therefore, thorium has a potential to achieve both production of electricity without emitting CO_{2} and reduction of concerns of ordinary nuclear power fueled by uranium.

There are many recent studies about features and models of the ADSR. Asuncion-Astronomo et al. [2] studied about computational design and characterization of a subcritical reactor assembly with TRIGA fuel. In this paper, the design for subcritical reactor assembly (SRA) with 44 TRIGA fuel rods is proposed. The parameters of SRA were computed by MCNP code. Vega-Carrillo et al. [3] studied about features of a subcritical nuclear reactor. In that study, the *k*_{eff} of the Universidad Autonoma de Zacatecas Subcritical Nuclear Reactor (UAZSNR) was calculated using six-factor formula and the Monte Carlo method. The ambient dose equivalents were estimated. Henry et al. [4] analyzed physical parameters of Jozef Stefan Institute (JSI) TRIGA-Mark II reactor with TRIPOLI and MCNP. A new computational model of the JSI TRIGA-Mark II reactor was built for TRIPOLI computer code and compared with existing MCNP code model. The neutron spatial flux profile measurement in compact subcritical system using miniature neutron detectors was conducted by Shukla et al. [5]. In that research, the authors presented the thermal neutron flux profile measurement in a compact subcritical system using indigenously developed miniature gas filled neutron detectors. A comparison of measured neutron flux using these detectors and simulated Monte Carlo computations was also given.

The TRIGA-Mark II reactor model is simulated and calculated neutron parameters by the MCNPX program [6, 7]. The proton beam generated from an accelerator with an intensity of 2 mA interacts on a tungsten target. A fuel mixture of UZrH (uranium zirconium hydride) with a 20% enrichment was considered. [8, 9]. The use of solid target to generate neutrons and light water as coolant in the ADSR system requires the target to be in a vacuum system and must be replaced after a period of use. To overcome this, molten lead is considered as both a coolant and a spallation neutron target. Preliminary study on this issue has been performed [10].

In this paper, with fuel as UZrH and UThO, two cases of using lead are considered: firstly, solid lead is referred to as spallation neutron target and water as the coolant; secondly, molten lead is seen as spallation neutron target and as a coolant. The percentages of components of Pb-206, Pb-207, and Pb-208 are 25.5%, 22.1%, and 52.4%, respectively. The density of solid lead is 11.34 g·cm^{−3} and that of molten lead is 10.66 g·cm^{−3}.

The fuel, a mixture of uranium and thorium in different proportions, is placed in the core reactor, with the different coolants. The proton beam with energies from 115 MeV to 2000 MeV, which interacts with the lead targets in solid and molten forms, was used to control the TRIGA-Mark II reactor. The parameters, as neutron yield *Y*_{n/p}, the neutron multiplication factor, and axial and radial distributions of the neutron flux along with the core, are investigated. The MCNPX [11] code has been used for the simulation and the calculations.

#### 2. Materials and Methods

##### 2.1. The TRIGA-Mark II Reactor Model

The TRIGA-Mark II subcritical reactor model was simulated as shown in Figure 1. Some characteristics of the core are shown in Table 1. The structure of the core consists of 108 fuel rods. The core is divided into 7 rings. All of these are assumed to be placed in the molten lead medium.

The detailed structure of the fuel rod is shown in Figure 2 [8].

##### 2.2. Calculations

MCNPX program has been used to simulate and calculate the neutronic parameters. The input file is constructed based on the detailed configuration of the TRIGA reactor. The neutron yield (*Y*_{n/p}) is calculated for the case of the proton beam current 2 mA interacting on the molten lead target in the core. Two options for distribution of the proton energy were considered for MCNPX code: parabolic spatial and uniform spatial distribution. Some calculations show that the differences between these options are negligible. In this study, the parabolic spatial distribution of the energy of the proton beam is chosen.

The neutron multiplication factor (*k*) is calculated from KCODE in MCNPX. The neutron flux is calculated from F4 tally in MCNPX based on the following equation:with normalization for the current of proton beam I(mA) and neutron yield *Y*_{n/p}, where C is a multiplication, (n·cm^{−2}s^{−1}) is the neutron flux, and is any combination of sums and products of energy-dependent quantities known to MCNPX [8]. The neutron flux has been determined according to the following equation [5]:with *Y*_{n/p} (*n*/*p*) being the neutron yield.

#### 3. Results and Discussion

##### 3.1. Neutron Yield *Y*_{n/P}

The neutron yield *Y*_{n/p} is the average number of neutrons produced per incident proton. In this investigation, proton beams with energies between 115 MeV and 2000 MeV were considered as the source of neutrons when they interact with lead target. Energy cross-section data from ﬁle nuclear data ENDF/B-VII.0 [12] were used. The results are shown in Table 2.

The results show that for the fixed proton current (2 mA), the neutron yields increase as energies of the incident proton beam increase. When using the lead target, the neutron yield is from 0.477 to 24.211 depending on the energies of the proton beam.

In comparison with the calculation results of references [7–9], the neutron yield of the lead target was about 4.2% higher than that of tungsten at an energy level of 115 MeV. However, the value of *Y*_{n/p} decreased by 14.2%, 8.2%, and 2.9%, respectively, corresponding to the energy of the proton beam of 300 MeV, 600 MeV, and 1000 MeV. These insignificant differences suggest that lead can be used as a suitable target to generate neutrons for ADSR.

##### 3.2. Neutron Multiplication Factor *K*

The *k* factor is calculated for fuel mixtures of uranium and thorium with different ratios. For TRIGA reactor, the previous studies [8] investigated the case of the UZrH (uranium zirconium hydride) fuel placed in the light water. In this paper, besides calculating for the fuel UZrH, the fuel mixture thorium-uranium oxide (ThUO) was also considered. Details of the ratio of components in the fuel mixture and calculation results of *k* have been presented in Table 3.

The results have been shown that for UZrH mixed fuel, the higher the ratio of uranium in the mixture, the higher the *k*. Let the *k* reach to the values higher than 0.9, then the proportion of uranium in the mixture must be greater than 24%. For ThUO mixture fuel, the results show a correlation between Th-232 and U-233 in fuel composition. As the component ratio U-233 increases, the *k* coefficient also increases. The parameter *k* reaches a value greater than 0.9 when U-233 accounts for about 29% of the mixture.

##### 3.3. Distributions of the Neutron Flux

On the basis of fuel composition data of UZrH and ThUO fuel given in Table 3, the neutron flux distributions on the height and the radius of the core with the light water coolant were calculated.

###### 3.3.1. The Case of UZrH Fuel and Light Water Coolant

The neutron flux distributions have been calculated for the case of the mixture of UZrH fuel, placed in light water, similar to the calculated models given in the previous studies [7–9]. To compare the neutron flux distribution as using solid lead and solid tungsten target, the differences of the neutron yield are considered. The axial distributions of the neutron flux have been calculated. These results are shown in Figure 3.

The results show that, with the same neutron multiplication factor, neutron flux distributions depend on the neutron yields. They depend on the properties of the target with the reactions of spallation and (p, n). Calculation results show that the neutron yield of solid lead is higher than that of tungsten. With *k* = 0.91, the maximum neutron flux is about 2.8 × 10^{13} n·cm^{−2}s^{−1} for a solid lead target and from 1.3 × 10^{13} to 1.4 × 10^{13} n·cm^{−2}s^{−1} for a tungsten target, as shown in the previous studies [7–9]. For case of *k* = 0.97, the maximum neutron flux is about 1.6 × 10^{13} n·cm^{−2}s^{−1}, compared with about 7.5 × 10^{12} to 7.6 × 10^{12} n·cm^{−2}s^{−1} for a tungsten target.

###### 3.3.2. The Case of UZrH Fuel and Molten Lead Coolant

The calculation of neutron flux along the height of the core with the UZrH mixture fuel placed in molten lead as target and coolant is already underway. Results are shown in Figure 4. The maximum and minimum values of neutron flux calculated by this work and previous publications are given in Table 4.

Results show that the neutron flux along the height of the core was maximum in the center and decreased to the core edge. The results in Table 4 show that with the same *k* value, the neutron flux of the fuel configuration UZrH in molten lead as the coolant and spallation neutron target (Case 1) has the highest value. The lowest value of the neutron flux belongs to the fuel profile UZrH in light water and the neutron generated by the tungsten target (Case 3). For *k* equal to 0.91 and 0.97, the neutron flux in Case 1 is about 8–11 and 6–9 times greater than in Case 3, respectively. The maximum-to-minimum ratio of neutron flux also shows that neutron flux in Case 1 is more uniform than in the other cases. Results in Case 2 also show that solid lead could be used as spallation neutron target for UZrH fuel immersed in light water.

###### 3.3.3. The Case of ThUO Fuel and Molten Lead Coolant

The composition ratios of ThUO fuel are given in Table 3. The axial and radial distributions of the neutron flux have been calculated for ThUO fuel placed in the molten lead. The results in Figure 5 show that the axial distribution of the neutron flux is symmetrical at the center of fuel pin and peaks at that position.

Results of the calculation of the radial distribution of the neutron flux are given in Table 5 and Figure 6. These results differ from the published results [6–8]. The neutron fluxes in this study peak at a position of about 3–5 cm along the radius from the center of the reactor core, while they are in the 8–10 cm range as shown in the references. The results also show that, compared with the reference results [6–8], the value of the maximum flux in this study is about 4.8 and 3.7 times greater than that of *k* equal to 0.91 and 0.97, respectively.

The study results suggest that lead in solid or molten form should be considered for use in designing ADSR systems with the UZrH or ThUO fuel . The use of molten lead as both spallation neutron target and as a coolant with ThUO fuel results in a high neutron flux, and the design and operation of the ADSR system will be simpler.

#### 4. Conclusions

The basic structure of the TRIGA-Mark II reactor has been simulated using the MCNPX program. The basic neutron parameters have been calculated, such as the neutron yields, the effective neutron multiplication factor, and the axial and radial distribution of the neutron flux. The above study results have shown that, in the ADSR system, molten lead should be considered both as target and as a coolant. The possibility of using molten lead as both target and coolant, using thorium fuel in combination with uranium, is a very promising ADSR system.

The results show that the investigation of the neutronic parameters related to the fuel, target, and coolant plays an important role in the design and economical operation of an ADSR system.

#### Data Availability

The previous studies (and datasets) are cited at relevant places within the article as references.

#### Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this paper.