Homogeneous Infinite-Medium Solver
Homogeneous infinite reactor eigenvalue solver.
Solves for the neutron spectrum and k-infinity in an infinite homogeneous medium. The transport equation reduces to:
(diag(Σ_t) − Σ_s0^T − 2·Σ₂^T) · φ = χ · P / k
where P = (Σ_p + 2·colsum(Σ₂)) · φ is the total production rate.
The solver satisfies the EigenvalueSolver protocol from
numerics.eigenvalue and can be used with the generic
power_iteration function.
See also
Homogeneous Infinite-Medium Reactor — Key Facts, eigenvalue equations, scattering convention.
- class orpheus.homogeneous.solver.HomogeneousResult(k_inf, flux, eg_mid, de, du, sig_prod, sig_abs, mixture)[source]
Bases:
objectResult of a homogeneous infinite reactor calculation.
- Parameters:
- k_inf: float
- flux: ndarray
- eg_mid: ndarray
- de: ndarray
- du: ndarray
- sig_prod: float
- sig_abs: float
- mixture: Mixture
- property flux_per_energy: ndarray
- property flux_per_lethargy: ndarray
- class orpheus.homogeneous.solver.HomogeneousSolver(mix)[source]
Bases:
objectEigenvalue solver for an infinite homogeneous medium.
The removal matrix A = diag(Σ_t) − Σ_s0^T − 2·Σ₂^T absorbs both scattering and (n,2n) into the LHS, so
solve_fixed_sourceis a single sparse direct solve per iteration.- Parameters:
mix (Mixture)
- compute_fission_source(flux_distribution, keff)[source]
- solve_fixed_source(fission_source, flux_distribution)[source]
- orpheus.homogeneous.solver.solve_homogeneous_infinite(mix, n_iter=5)[source]
Solve the eigenvalue problem for an infinite homogeneous reactor.