Geometric buckling from neutron flux

Geometric buckling can be found if the neutron flux density is known as a function of position. The smaller the reactor is, more “buckled” the curvature of the neutron flux is and the higher geometric buckling of the reactor is.

Links:

  1. Wikipedia, see fourth equation.

position

position.

Symbol:

x

Latex:

\(x\)

Dimension:

length

neutron_flux

neutron_flux as a function of position

Symbol:

Phi(x)

Latex:

\(\Phi{\left(x \right)}\)

Dimension:

1/(area*time)

geometric_buckling

geometric_buckling.

Symbol:

B_g^2

Latex:

\(B_\text{g}^2\)

Dimension:

1/area

neutron_flux_laplacian

Laplacian of the neutron_flux as a function of position.

Symbol:

Laplace(Phi)(x)

Latex:

\(\nabla^{2} \Phi{\left(x \right)}\)

Dimension:

1/(length**4*time)

law

B_g^2 = -Laplace(Phi)(x) / Phi(x)

Latex:
\[B_\text{g}^2 = - \frac{\nabla^{2} \Phi{\left(x \right)}}{\Phi{\left(x \right)}}\]