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2010
DOI: 10.1016/j.jcp.2009.12.023
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An angular multigrid method for computing mono-energetic particle beams in Flatland

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Cited by 4 publications
(16 citation statements)
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“…Since the transport equation (2.1a) is elliptic in the θ-direction but advective in the x-and y-directions, the angular multigrid method described in [3] combines relaxation sweeps ordered parallel to the (x, y) plane with coarse-grid correction over the θ-direction. The discretization of the transport equation (2.1a) that we wish to solve can briefly be represented as…”
Section: The Angular Multigrid Methodmentioning
confidence: 99%
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“…Since the transport equation (2.1a) is elliptic in the θ-direction but advective in the x-and y-directions, the angular multigrid method described in [3] combines relaxation sweeps ordered parallel to the (x, y) plane with coarse-grid correction over the θ-direction. The discretization of the transport equation (2.1a) that we wish to solve can briefly be represented as…”
Section: The Angular Multigrid Methodmentioning
confidence: 99%
“…Table 3 shows effective convergence factors for V(0, 1)-cycles applied to the transport equation where the Downloaded 12/08/14 to 130.88.90.140. Redistribution subject to SIAM license or copyright; see http://www.siam.org/journals/ojsa.php Table 3 Effective convergence factors, i. e., fourth roots of convergence factors, per iteration in first 24 V(0, 1)-cycles for the test problem, screened Rutherford scattering, discretized using second-order upstream differencing, the three-point discretization of the Fokker-Planck operator, and effective convergence factors per iteration in first 12 V(0, 1)-cycles with Henyey-Greenstein scattering, taken from [3,Tables 5,11,12]. Table 3, i. e., effective convergence factors that do not degrade as n s and n θ increase.…”
Section: The Angular Multigrid Methodmentioning
confidence: 99%
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