2020
DOI: 10.1007/s00419-020-01716-0
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Topology of corner vortices in the lid-driven cavity flow: 2D vis a vis 3D

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Cited by 7 publications
(3 citation statements)
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“…After a critical value of [p 2 /p 1 ] ≥ 1.5, the Mach type of shock reflection increases the shock loading on the cavity, and the overall wall-static pressure increases, rapidly. The first bucket or drop-in [p/p ∞ ] between 0 ≤ [s/D] ≤ 1 marks the presence of multiple corner vortices 69 (see label-13 in Figure 6) that are conventionally seen in subsonic corner flows. Due to [p 2 /p 1 > 1], the corner vortices disappear, and the suction level flattens.…”
Section: Rear Wallmentioning
confidence: 99%
“…After a critical value of [p 2 /p 1 ] ≥ 1.5, the Mach type of shock reflection increases the shock loading on the cavity, and the overall wall-static pressure increases, rapidly. The first bucket or drop-in [p/p ∞ ] between 0 ≤ [s/D] ≤ 1 marks the presence of multiple corner vortices 69 (see label-13 in Figure 6) that are conventionally seen in subsonic corner flows. Due to [p 2 /p 1 > 1], the corner vortices disappear, and the suction level flattens.…”
Section: Rear Wallmentioning
confidence: 99%
“…Mendu and Das [4] simulated lid-driven cavity flow with a periodically oscillating lid. Biswas and Kalita [5] gained some physical insights of the topology of corner vortices in 2D vis a 3D vis driven cavity. Dalai and Laha [6] interpreted the conservative solutions of Navier-Stokes equations (NSEs) in the stream function-vorticity form.…”
Section: Introductionmentioning
confidence: 99%
“…The lid-driven cavity flow as a benchmark problem has attracted much attention in PINNs [13] . The Reynolds number Re is the characteristic parameter of the cavity flow, and it is widely accepted that the cavity flow is steady when Re < 5 000 [14] . It is the ideal model for validating and studying the accuracy and efficiency of numerical methods as well as PINNs.…”
Section: Introductionmentioning
confidence: 99%