2019 IEEE 21st International Conference on High Performance Computing and Communications; IEEE 17th International Conference On 2019
DOI: 10.1109/hpcc/smartcity/dss.2019.00153
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Large-Scale Lattice Boltzmann Method Simulations of Stenosed Carotid Bifurcation

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(2 citation statements)
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“…The LBM model described by Equations (1)–(6) is referred to as the single‐relaxation‐time LBM, due to the single relaxation parameter, τ. This is the approach applied here, in common with other LBM studies relating to the carotid artery 29,31,32,36 due to its efficient computation; however, it is worth noting that it does have some disadvantages. In particular, it can experience stability issues at high Reynolds number flows, where a multi‐relaxation‐time (MRT) 40,41 model can be applied.…”
Section: Methodsmentioning
confidence: 99%
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“…The LBM model described by Equations (1)–(6) is referred to as the single‐relaxation‐time LBM, due to the single relaxation parameter, τ. This is the approach applied here, in common with other LBM studies relating to the carotid artery 29,31,32,36 due to its efficient computation; however, it is worth noting that it does have some disadvantages. In particular, it can experience stability issues at high Reynolds number flows, where a multi‐relaxation‐time (MRT) 40,41 model can be applied.…”
Section: Methodsmentioning
confidence: 99%
“…The simulations were focussed at micro‐channels, but could also be applied at the scale of the carotid artery, and would be particularly relevant when a high level of stensosis is present. Ge et al 32 considered details of velocity and WSS fields for a number of pre‐determined carotid artery geometries including an unstenosed artery. As well as focussing on the velocity and WSS from their patient specific arteries, they also considered aspects of parallel implementation required to provided a detailed 3D representation.…”
Section: Introductionmentioning
confidence: 99%