In a nuclear reactor, criticality is achieved when the rate of neutron production is equal to the rate of neutron losses, including both neutron absorption and neutron leakage. Geometric buckling is a measure of neutron leakage, while material buckling is a measure of neutron production minus absorption. Thus, in the simplest case of a bare, homogeneous, steady state reactor, the geometric and material buckling must be equal.
Contents
Derivation
Both buckling terms are derived from the diffusion equation:
where k is the criticality eigenvalue,
In addition, the diffusion length is defined as:
Rearranging the terms, the diffusion equation becomes:
The left side is the material buckling and the right side of the equation is the geometric buckling.
Geometric Buckling
The geometric buckling is an eigenvalue problem that can be solved for different geometries. The table below lists the geometric buckling for some common geometries.
Since the diffusion theory calculations overpredict the critical dimensions, an extrapolation distance δ must be subtracted to obtain an estimate of actual values. The buckling could also be calculated using actual dimensions and extrapolated distances using the following table.
Expressions for Geometric Buckling in Terms of Actual Dimensions and Extrapolated Distances.
Material Buckling
Materials buckling is the buckling of a homogeneous configuration with respect to material properties only. If we redefine
As stated previously, the geometric buckling is defined as:
Solving for k (in the fundamental mode),
thus,
Assuming the reactor is in a critical state (k = 1),
This expression is in purely material properties; therefore, this is called the materials buckling:
Critical Reactor Dimensions
By equating the geometric and material buckling, one can determine the critical dimensions of a one region nuclear reactor.