It is well known that each reactor core is surrounded by a neutron reflector or reactor core baffle. The reflector reduces the non-uniformity of the power distribution in the peripheral fuel assemblies, reduces neutron leakage, and reduces a coolant flow bypass of the core. The neutron reflector is a non-multiplying medium, whereas the reactor core is a multiplying medium.
The neutron reflector scatters back (or reflects) into the core many neutrons that would otherwise escape (i.e., reduces the neutron leakage). By reducing neutron leakage, the reflector increases keff and reduces the amount of fuel necessary to maintain the reactor critical for a long period. In LWRs, the neutron reflector is installed for the following purposes:
The neutron flux distribution is “flattened”, i.e., the ratio of the average flux to the maximum flux is increased. Therefore reflectors reduce the non-uniformity of the power distribution.
- Because of the higher flux at the edge of the core, there is much better utilization in the peripheral fuel assemblies. In the outer regions of the core, this fuel now contributes much more to the total power production.
- The neutron reflector scatters back (or reflects) into the core many neutrons that would otherwise escape. The neutrons reflected back into the core are available for a chain reaction. This means that the minimum critical size of the reactor is reduced. Alternatively, if the core size is maintained, the reflector makes additional reactivity available for higher fuel burnup. The decrease in the critical size of a core required is known as reflector savings.
- Neutron reflectors reduce neutron leakage, i.e., to reduce the neutron fluence on a reactor pressure vessel.
- Neutron reflectors reduce a coolant flow bypass of a core.
- Neutron reflectors serve as a thermal and radiation shield of a reactor core.
The reflector’s efficiency is measured by the ratio of the number of neutrons reflected back into the reactor to the number entering the reflector. This ratio is called the albedo or the reflection coefficient. The albedo can be expressed in terms of neutron currents as:
The value of the albedo will depend on the composition and thickness of the reflector. An infinite reflector will have the maximum albedo. Still, in all practical cases, the geometry of a reflector must conform to the geometry of a reactor core and a reactor pressure vessel. For sufficiently thick reflectors, it can be derived that albedo becomes:
where Drefl is the diffusion coefficient in the reflector, and the Lrefl is the reflection’s diffusion length.
Materials and Types of Neutron Reflectors
There are a variety of materials that are used as a reflecting medium for neutrons in nuclear reactors. In general, reflector materials are normally not fissionable and have high scattering cross-section and low absorption cross-section. Since main differences among reactor types arise from differences in their neutron energy spectra, we must specify whether we mean reflectors in fast reactors or thermal reactors. Since the moderation of neutrons is undesirable in fast reactors, they use only high Z materials.
Its material must possess the following properties to be an effective reflector.
- Low absorption cross-section
- High reflection coefficient
- Radiation stability – Radiation stability is a very important property of reflectors because the reflector material will be exposed to high levels of radiation (especially gamma radiation and fast neutrons)
- Resistance to Oxidation – The reflector is often situated in a chemically aggressive environment (especially in fast reactors). Therefore the material should not get oxidized.
Essentially, for thermal reactors, a good moderator is also a good reflector because most moderators also possess the properties mentioned above of a good reflector. Water, heavy water, beryllium, or graphite are commonly used as reflectors. In pressurized water reactors, water serves as an axial reflector. This axial reflector does not form any special device, and the neutrons are simply reflected by the core inlet and outlet coolant.
On the other hand, common water volume cannot be used as a reflector in radial direction because it is of the highest importance to maintain high flow rates in the core and not bypass fuel assemblies. Therefore the neutron reflectors are installed in PWR and BWR reactor cores. The design of neutron reflectors may vary, but we can distinguish between two basic types:
- Core Baffle. Core baffle consists of the baffle and former assembly consisting of vertical plates called baffles, and horizontal support plates called formers. This assembly forms the interface between the core and the core barrel, and there is water between the baffle and the core barrel. Since the coolant flow in the former region is significantly reduced by the former, the high flow rate through fuel assemblies is maintained. A secondary benefit is that water in the former region reduces the neutron flux on the pressure vessel, which causes irradiation embrittlement of pressure vessel material.
Heavy Reflector. A heavy reflector is a structure that is installed inside a core barrel (similarly to a core baffle). But the heavy reflector is a wall made of stainless steel slabs stacked vertically surrounding the reactor core. Due to higher atomic number density, heavy reflectors reduce neutron leakage (especially of fast neutrons) from the core more efficiently than the core baffle. This provides additional protection of the reactor vessel from irradiation embrittlement, caused especially by fast neutrons. While acting as a neutron shield, the heavy reflector is heated due to the absorption of gamma radiation. The heat in the reflector is removed by water flowing through cooling channels drilled through the reflector to avoid overheating.
In fast reactors, moderation of neutrons is undesirable. Therefore reflectors are not composed of moderating materials. In fast breeder reactors, the core is surrounded by a radial core reflector. The radial core reflector is usually composed of fuel assemblies with natural uranium (so-called the radial blanket zone). The diffusion coefficient is about the same as that of the core. This reflector improves the radial flux distribution, reduces the fissile inventory, and increases the internal breeding ratio.