1969
DOI: 10.1080/18811248.1969.9732925
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A Numerical Method for Solving the Neutron Transport Equation in Finite Cylindrical Geometry

Abstract: A method is presented which provides a numerical solution to the steady state, energy dependent neutron transport equation for finite cylindrical geometry, with anisotropic treatment of elastic scattering and isotropic treatment of inelastic scattering. The main characteristic features of the method are the use of quasi-cartesian coordinates and the application of discrete ordinate numerical integration. A difference form of the Boltzmann equation is derived as the final expression for machine computation.Comp… Show more

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Cited by 9 publications
(5 citation statements)
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“…Takeuchi has used the method of characteristics in Cartesian, spherical, and twodimensional (r-θ) cylindrical geometries to solve the transport equation for deep penetration shielding problems. 27,28 In this approach, fluxes are computed at the vertices of a cell. In a two-dimensional problem, it is assumed that the source is known at all four vertices and that the angular flux is known at three vertices.…”
Section: Characteristics Methods In Shielding Applicationsmentioning
confidence: 99%
“…Takeuchi has used the method of characteristics in Cartesian, spherical, and twodimensional (r-θ) cylindrical geometries to solve the transport equation for deep penetration shielding problems. 27,28 In this approach, fluxes are computed at the vertices of a cell. In a two-dimensional problem, it is assumed that the source is known at all four vertices and that the angular flux is known at three vertices.…”
Section: Characteristics Methods In Shielding Applicationsmentioning
confidence: 99%
“…To solve the Eqs. ( 19) ray tracing techniques (aka the method of long characteristics) are applied [85,86,87,88,89,90,91,92]. In sum, the data-driven VEF model for TRT is constructed with:…”
Section: Variable Eddington Factor Model For Trt With Diffusion-based...mentioning
confidence: 99%
“…Note that if one applies weak condition for the currents and strong conditions for the scalar fluxes, it results in interface relationships that are not valid for the scalar fluxes varying linearly along cell interfaces [49]. For example, in 2D, if the left face of i-th cell is a common face with the m-th and p-th cells, then we define strong continuity conditions for the normal components of the currents 30) and the weak continuity condition for the face-average scalar fluxes 31) where h iω is the cell-edge length.…”
Section: Interface Continuity Conditionsmentioning
confidence: 99%
“…(3.37) and (3.38). We define a small parameter ε, introduce the scaled cross sections and sources 42) and the following ansatz:…”
Section: Asymptotic Diffusion Analysismentioning
confidence: 99%
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