Transition to entrainment in downward annular gas-liquid flow: Study through flow control

• Published in: International journal of multiphase flow 2025-03, Vol.184, Article 105109
• Main Authors: Cherdantsev, Andrey, Isaenkov, Sergey, Markovich, Dmitry
• Format: Article
• Language: English
• Subjects: Annular flow; Disturbance waves; Entrainment; Flow control; Flow patterns; Inlet forcing
• ISSN: 0301-9322
• DOI: 10.1016/j.ijmultiphaseflow.2024.105109

•Film structure near transition to disturbance waves is studied experimentally.•To create a disturbance wave, a strong localized perturbation is required.•To maintain a disturbance wave, enough liquid above viscous sub-layer is needed.•The conclusions are supported by imposing low-frequency inlet forcing.•The inlet forcing helps widening the area of disturbance wave existence. Formation of disturbance waves and entrainment of liquid droplets drastically enhances pressure drop and heat and mass transfer in annular flow. Here we investigate the transition to entrainment by analyzing spatiotemporal records of film thickness in the vicinity of the transition border. Two branches of the border: “vertical”, with high gas speeds and low liquid flow rates, and “horizontal”, with low gas speeds and large liquid flow rates, are analyzed separately. In both cases, low-frequency pulsations of liquid flow rate are applied in attempt to expand the regime area of entrainment and learn more about the transition. It was found that two conditions are necessary for creation of a disturbance wave: strong localized perturbations able to create the initial hump of liquid and enough spare liquid in excess of the viscous sub-layer to fill and maintain this hump. Below the “vertical” branch, the disturbance waves do not occur due to lack of spare liquid. Below the “horizontal” branch, no sources of strong perturbations are present. Both “vertical” and “horizontal” branches can be shifted towards lower values of liquid flow rate and gas speed, respectively, using low-frequency oscillations of liquid flow rate. However, the mechanisms of creating these artificial disturbance waves are different. For “vertical” branch, the pulsations create patches of larger liquid flow rate, where disturbance waves can be created in a “natural” manner. For “horizontal” branch, each pulsation period creates a single disturbance wave, provided that the excitation frequency belongs to appropriate range. [Display omitted]