2013
DOI: 10.1016/j.jcp.2012.07.009
|View full text |Cite
|
Sign up to set email alerts
|

Parallel algorithms for transport sweeps on unstructured meshes

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
14
0

Year Published

2013
2013
2022
2022

Publication Types

Select...
9
1

Relationship

0
10

Authors

Journals

citations
Cited by 32 publications
(14 citation statements)
references
References 28 publications
0
14
0
Order By: Relevance
“…This is a similar approach to that developed in [57] ( AIR), but nAIR can offer setup-times that are orders of magnitude faster than AIR in some cases. Steady state transport is used as a model problem, which arises in large-scale simulation of neutron and radiation transport [1,5,18,30,49]. Results in Section 6 show that nAIR outperforms current state-of-the art methods, and is able to attain an order-of-magnitude reduction in residual in only 1-2 iterations, even for high-order discretizations on unstructured grids.…”
mentioning
confidence: 99%
“…This is a similar approach to that developed in [57] ( AIR), but nAIR can offer setup-times that are orders of magnitude faster than AIR in some cases. Steady state transport is used as a model problem, which arises in large-scale simulation of neutron and radiation transport [1,5,18,30,49]. Results in Section 6 show that nAIR outperforms current state-of-the art methods, and is able to attain an order-of-magnitude reduction in residual in only 1-2 iterations, even for high-order discretizations on unstructured grids.…”
mentioning
confidence: 99%
“…To decouple these functions from the equations, a functional-type iteration called the source iteration (SI) [27,36] (also referred to as the grid sweeping algorithm) has been widely used for solving the system in a Gauss-Seidel-like manner. To be specific, assuming that the -th iteration solutions I h( ) m,K (x, y, t n+1 ) (for m = 1, · · · , N a and K ∈ T h (t n+1 )) are known, we compute the new approximations I h( +1) m,K (x, y, t n+1 ) element by element in a sweeping direction [10] and through all angular directions m = 1, · · · , N a for each given element. Thus, for K ∈ T h (t n+1 ), we…”
Section: )mentioning
confidence: 99%
“…The algorithm they presented is applicable to more general cases than radiation transport problems as it uses no geometric information about the mesh. In the paper [11], the authors presented new algorithms for the sweep operation on unstructured meshes by designing algorithms that achieve overlap of communication by computations, as well as message buffering to reduce cost associated with the latency of parallel machines which are used.…”
Section: Related Workmentioning
confidence: 99%