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atw - International Journal for Nuclear Power | 03.2020

Ever since its first issue in 1956, the atw – International Journal for Nuclear Power has been a publisher of specialist articles, background reports, interviews and news about developments and trends from all important sectors of nuclear energy, nuclear technology and the energy industry. Internationally current and competent, the professional journal atw is a valuable source of information. www.nucmag.com

Ever since its first issue in 1956, the atw – International Journal for Nuclear Power has been a publisher of specialist articles, background reports, interviews and news about developments and trends from all important sectors of nuclear energy, nuclear technology and the energy industry. Internationally current and competent, the professional journal atw is a valuable source of information.

www.nucmag.com

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<strong>atw</strong> Vol. 65 (2020) | Issue 3 ı March<br />

RESEARCH AND INNOVATION 142<br />

Neutronic Simulation of ALFRED Core<br />

Using MCNPX Code<br />

Korosh Rahbari, Darush Masti, Kamran Serpanloo and Ehsan Zarifi<br />

Introduction Throughout history, energy has played a fundamental role in human’s progress living. To promote<br />

nuclear power to meet the future energy needs, ten countries including Argentina, South Africa, the United States, the<br />

United Kingdom, Brazil, Japan, Switzerland, France, Canada and Korea in a global ef<strong>for</strong>t (Generation IV <strong>International</strong><br />

Forum – GIF) have agreed to investigate the next generation of nuclear energy systems known as 4 th generation [1].<br />

These reactors are expected to enter the market after 2030. Fundamental changes in the configuration of the systems<br />

and the <strong>for</strong>ms of the old reactors have led to the production of new reactors, which require basic research and<br />

development, careful examination, and the construction of semi-industrial units. The capabilities of fourth-generation<br />

reactors are seawater desalination, and thermal applications in addition to the production of electricity. In 2000, the<br />

founding countries of GIF <strong>for</strong>med their first meeting to discuss the need <strong>for</strong> conduct research on the design of<br />

next-generation reactors. Subsequently, a strategy was put <strong>for</strong>ward to direct the activities, and the implementation<br />

responsibility was assigned to the US Department of Energy. In this research, we investigate the neutron behavior of the<br />

advanced reactor core with lead coolant ALFRED. The purpose of the neutron calculations of the core of a reactor is to<br />

calculate the distribution of neutron flux in the center and to calculate the effective reproduction coefficient. Given the<br />

necessity of per<strong>for</strong>ming lattice pitch neutron calculations, it is initially required to determine the real geometry of the<br />

core, as well as the order and fuel richness, the lattice pitch the grid, the radius and height of the fuel rods, the<br />

composition and location of the fuel absorbents, the types and locations of the control rods, the fuel complex<br />

arrangement, and radial and axial peaking factor. The MCNPX code is used to per<strong>for</strong>m neutron calculations.<br />

This calculation is done by the MCNPX<br />

code using the Monte Carlo statistical<br />

method. The following six reactors<br />

have been categorized as the 4 th<br />

generation reactors:<br />

1. Gas-Cooled Fast Reactor (GFR)<br />

2. Lead-Cooled Fast Reactor (LFR)<br />

3. Molten Salt Reactor (MSR)<br />

4. Sodium-Cooled Fast Reactor (SFR)<br />

5. Supercritical Water-Cooled Reactor<br />

(SCWR)<br />

6. Very High-Temperature Reactor<br />

(VHTR)<br />

LFR is one of the six advanced 4 th<br />

generation reactors. In recent years,<br />

this kind of reactor has attracted a lot<br />

of attention of the world, and specially<br />

recently countries such as Russia,<br />

America and Germany have always<br />

Parameter Unit Values<br />

Thermal power MW 300<br />

Active height cm 60<br />

Pellet hollow diameter mm 2<br />

Pellet radius mm 4.5<br />

Gap thickness mm 0.15<br />

Clad thickness mm 0.6<br />

Pin diameter mm 10.5<br />

Wrapper thickness mm 4<br />

Distance between 2 wrappers mm 5<br />

Coolant velocity m s -1 ~1.4<br />

Lattice pitch (hexagonal) mm 13.86<br />

Pins per FA - 127<br />

Inner vessel radius cm 165<br />

| Tab. 1.<br />

Main specifications of ALFRED reactor [3].<br />

| Fig. 1.<br />

View of the ALFRED reactor [3].<br />

been interested in this topic. LFR<br />

systems have excellent material<br />

handling capabilities due to the use of<br />

a fast neutron spectrum, and they use<br />

a closed fuel cycle to convert more<br />

efficiently the enriched uranium.<br />

It can also, as an actinide burner,<br />

consume the spent fuel of light water<br />

reactors (LWRs) or be used as an<br />

adiabatic reactor (able to burn off its<br />

produced actinide wastes).<br />

Method and material<br />

1 Technical description<br />

of ALFRED reactor<br />

As stated, the program of the ALFRED<br />

reactor is within the framework of<br />

the LEADER project. The purpose of<br />

the ALFRED project is to analyze<br />

the various aspects of lead cooling<br />

technology in fast reactors. This<br />

project has, there<strong>for</strong>e, a significant<br />

role as ETDR (European Technology<br />

Demonstrator Reactor) in the technology<br />

chain. The ALFRED reactor<br />

design includes a 125 MW electric<br />

power reactor with lead coolant.<br />

Figure 1 shows a schematic illustration<br />

of this reactor.<br />

Some geometric parameters of the<br />

ALFRED reactor are shown in Table 1.<br />

The core of this reactor has a hexagonal<br />

grid of 171 fuel assemblies (FA),<br />

12 control bars (CR), four safety bars<br />

(SR) and 108 empty bars. A schematic<br />

illustration of the core of this reactor is<br />

shown in Figure 2.<br />

Research and Innovation<br />

Neutronic Simulation of ALFRED Core Using MCNPX Code ı Korosh Rahbari, Darush Masti, Kamran Serpanloo and Ehsan Zarifi

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