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The material may be graphite, beryllium, steel, tungsten carbide, gold, or other materials. A neutron reflector can make an otherwise subcritical mass of fissile material critical, or increase the amount of nuclear fission that a critical or supercritical mass will undergo.
The reflection is usually described in terms of a momentum transfer vector, denoted , which describes the change in momentum of a neutron after reflecting from the material. Conventionally the z {\displaystyle z} direction is defined to be the direction normal to the surface, and for specular reflection, the scattering vector has only a z ...
A neutron supermirror is a highly polished, layered material used to reflect neutron beams. Supermirrors are a special case of multi-layer neutron reflectors with varying layer thicknesses. [1] The first neutron supermirror concept was proposed by Ferenc Mezei, [2] inspired by earlier work with X-rays.
Moderation is the process of the reduction of the initial high speed (high kinetic energy) of the free neutron. Since energy is conserved, this reduction of the neutron speed takes place by transfer of energy to a material called a moderator. The probability of scattering of a neutron from a nucleus is given by the scattering cross section. The ...
It is used in nuclear weapon design to reduce the critical mass and to delay the expansion of the reacting material through its inertia, which delays the thermal expansion of the fissioning fuel mass, keeping it supercritical longer. Often the same layer serves both as tamper and as neutron reflector. The weapon disintegrates as the reaction ...
The HB-4 cold neutron source beam tube is situated tangential to the reactor core so that the tube points at reflector material and does not point directly at the fuel. A vacuum tube fits closely inside in-vessel section of the HB-4 beam tube all the way to the spherical end.
The critical mass can be greatly reduced by the use of a tamper. The following table lists the values for common neutron reflectors, where λ tamp is the mean free path of a neutron within the tamper material before an elastic scattering. In nuclear weapon design, natural uranium is primarily used.
In nuclear weapon design, the pit is the core of an implosion nuclear weapon, consisting of fissile material and any neutron reflector or tamper bonded to it. Some weapons tested during the 1950s used pits made with uranium-235 alone, or as a composite with plutonium. [1]