4.5 Article

Direct numerical simulation of turbulent bubbly down flow using an efficient CLSVOF method

Journal

INTERNATIONAL JOURNAL OF MULTIPHASE FLOW
Volume 135, Issue -, Pages -

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.ijmultiphaseflow.2020.103500

Keywords

Turbulent bubbly flow; Level-set; Volume-of-fluid; Direct numerical simulation

Categories

Funding

  1. SURF Cooperative

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The presence of bubbles in vertical channels flowing downward causes turbulent modulation, resulting in significant modification of the mean velocity profile and accumulation of bubbles in the core region with a bubble-free layer near the wall. The presence of bubbles also promotes turbulence in the core region, enhancing turbulent kinetic energy. Additionally, the size of bubbles affects the velocity fluctuations, with wall-normal and spanwise fluctuations decreasing for smaller bubbles in the near-wall region.
We use direct numerical simulations (DNS) to investigate the turbulent modulation due to the presence of bubbles in vertical channels flowing downward. The Reynolds number for single-phase flow based on half channel height h* and friction velocity is Re-tau = 180. A density and viscosity ratio of rho(d)*/rho(c)* = 0.01 and mu(d)*/mu(c)* = 0.018 is chosen for two void fractions of epsilon = 1.2% and epsilon = 2.4%. For each void fraction three different bubble sizes are simulated: D/h =0.2130, 0.2684 and 0.3382, where D denotes the diameter of the bubbles. Numerical simulations are based on multiple markers Coupled Level-Set/Volume-of-Fluid (CLSVOF) method. To improve the efficiency of this method, a fast pressure-correction method is used in order to enable the simulation to exploit a constant coefficient Poisson equation which can be solved with FFT-based technique. Extensive verification and validation were performed and perfect accuracy and agreement are obtained. In all the simulations performed in this work, the new Poisson solver showed a minimum speedup of 22 times. Accumulation of bubbles in the core region of the channel for all cases is observed, which forms a bubble-free layer in the near-wall region. The presence of bubbles resulted in considerable modification in the mean velocity profile compared to single-phase flow. Another common observation is that all the components of velocity fluctuations in the near-wall region decrease with increasing void fraction and decreasing wall layer thickness. The opposite happens in the core region, where the presence of bubbles favours turbulence. With respect to the bubble size, the wall-normal and spanwise velocity fluctuations decrease in the near-wall region for smaller bubbles, however, the streamwise velocity fluctuations remained almost unaffected. The investigation of turbulent kinetic budgets shows that, unlike single-phase flow, the dissipation terms rises to large values in the core region of the channel. This behaviour is referred to the presence of bubbles and hence enhancement of turbulent kinetic energy in the core region. (C) 2020 Elsevier Ltd. All rights reserved.

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