2018
DOI: 10.1016/j.ijheatfluidflow.2018.08.003
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Direct numerical simulation of a turbulent 90° bend pipe flow

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Cited by 42 publications
(20 citation statements)
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“…The low frequency mode that was present fort 10 has been suppressed. Since this low frequency mode is thought to originate from the large-scale structures upstream of the bend [12], one possible explanation for this observation is the turbulence-suppressing effects of stable stratification, which reduce the kinetic energy contained within the large structures. Figures 12 and 13 show contours of the normalised axial velocity 0.05D from the wall, for timest = 0 andt = 30, respectively.…”
Section: Swirl-switchingmentioning
confidence: 99%
“…The low frequency mode that was present fort 10 has been suppressed. Since this low frequency mode is thought to originate from the large-scale structures upstream of the bend [12], one possible explanation for this observation is the turbulence-suppressing effects of stable stratification, which reduce the kinetic energy contained within the large structures. Figures 12 and 13 show contours of the normalised axial velocity 0.05D from the wall, for timest = 0 andt = 30, respectively.…”
Section: Swirl-switchingmentioning
confidence: 99%
“…The DNS data are generated by a massively paralleled MPI (Message Passing Interface) code, Nek5000 (Fischer, Lottes & Kerkemeier 2008) using the spectral element method (SEM). The incompressible Navier-Stokes equations are solved in Cartesian coordinates to avoid the singularity issue associated with the cylindrical coordinates at the pipe centreline (Jung & Chung 2012;Wang et al 2018). A semi-implicit time scheme solves the viscous terms implicitly using a third-order backward differentiation (BDF3) and the nonlinear terms by a third-order extrapolation (EXT3).…”
Section: Numerical Simulationmentioning
confidence: 99%
“…Given the fact that the existence of backflow events has been established beyond doubt in canonical wall-bounded flows, in this study we aim at evaluating the effect of a nonzero cross-stream velocity distribution (i.e., secondary flow) on such backflow events. The flow through curved pipes is characterised by a strong in-plane secondary flow of Prandtl's first kind driven by the centrifugal force and accompanied by a pressure gradient, which has a strong impact on the kinematics and dynamics of the flow [34,35]. This makes the toroidal pipe a very interesting flow case regarding backflow events.…”
Section: Introductionmentioning
confidence: 99%