2005
DOI: 10.1016/j.anucene.2005.07.004
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A nodal collocation method for the calculation of the lambda modes of the PL equations

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Cited by 22 publications
(50 citation statements)
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“…Since P L equations (13) have a diffusive form, their spatial discretization can be done using a nodal collocation method, previously used for the neutron diffusion equation (Hébert, 1987;Verdú et al, 1994) and generalized for eigenvalue problems in multidimensional rectangular geometries (Capilla et al, 2005(Capilla et al, , 2008(Capilla et al, , 2012. We will only apply the method when the source term in Eq.…”
Section: The Nodal Collocation Methods For An Isotropic Sourcementioning
confidence: 99%
See 2 more Smart Citations
“…Since P L equations (13) have a diffusive form, their spatial discretization can be done using a nodal collocation method, previously used for the neutron diffusion equation (Hébert, 1987;Verdú et al, 1994) and generalized for eigenvalue problems in multidimensional rectangular geometries (Capilla et al, 2005(Capilla et al, , 2008(Capilla et al, , 2012. We will only apply the method when the source term in Eq.…”
Section: The Nodal Collocation Methods For An Isotropic Sourcementioning
confidence: 99%
“…Furthermore, if X e (u 1 , u 2 , u 3 ) denotes the previously defined vector of l even moments that appears in Eq. (13) for node e, it is assumed that vector X e can be expanded in terms of (orthonormal) Legendre polynomials P k (u) (Capilla et al, 2005) up to a certain finite order M ,…”
Section: The Nodal Collocation Methods For An Isotropic Sourcementioning
confidence: 99%
See 1 more Smart Citation
“…Inserting these expansions into equation (2.1) and with the aid of the orthogonality relations for the Legendre polynomials and the addition theorem for the associated Legendre functions we obtain the standard P L approximation in one-dimensional 24 2.1 One-dimensional geometries geometries [8,35] …”
Section: Spectral Element Methods (Sem)mentioning
confidence: 99%
“…We consider a homogeneous slab of length 2 cm [35], in the approximation of one group of energy and vacuum boundary conditions, that is, α − = 1, α + = 1, β − = 2 and β + = −2. The nuclear cross sections for this problem are: D = 1 3 , Σ a = 0.1, and νΣ f = 0.25.…”
Section: Homogeneous Eigenvalue Problemmentioning
confidence: 99%