“…Different from the nozzle of millimeter scale, a special coalescence bubbling regime was observed for the micron‐sized nozzle, where some subsequent small bubbles (trailing bubbles) grew rapidly and merged into the detached larger bubble (leading bubble). This phenomenon was firstly reported by Xie et al 19 and also found by Ata et al, 20 Quinn and Finch 21 in experiments. Qu et al 22 and Zhang et al 23 investigated the effect of nozzle diameter and gas flow rate on this coalescence behavior with upward‐pointing capillary nozzles.…”
Bubble formation from a downward‐pointing capillary nozzle was investigated in this study. The experiments were conducted at gas flow rate of 40–5,400 ml/h and inner nozzle radius of 0.030–0.255 mm. Experimental results show that microbubbles are formed continuously at moderate Weber number, which was not reported in pervious investigations with injecting gas through an upward‐pointing capillary nozzle. High‐speed visualization indicates that the formation of microbubbles arises from the convergence of the capillary waves induced by the partial coalescence of larger bubbles. A bubbling regime map is given to identify the critical conditions for the formation of microbubbles. In the present air‐water experiments, the generated microbubbles are 20–170 μm in diameter. From experimental data, a scaling law for microbubble size is proposed as a function of Weber and Bond numbers.
“…Different from the nozzle of millimeter scale, a special coalescence bubbling regime was observed for the micron‐sized nozzle, where some subsequent small bubbles (trailing bubbles) grew rapidly and merged into the detached larger bubble (leading bubble). This phenomenon was firstly reported by Xie et al 19 and also found by Ata et al, 20 Quinn and Finch 21 in experiments. Qu et al 22 and Zhang et al 23 investigated the effect of nozzle diameter and gas flow rate on this coalescence behavior with upward‐pointing capillary nozzles.…”
Bubble formation from a downward‐pointing capillary nozzle was investigated in this study. The experiments were conducted at gas flow rate of 40–5,400 ml/h and inner nozzle radius of 0.030–0.255 mm. Experimental results show that microbubbles are formed continuously at moderate Weber number, which was not reported in pervious investigations with injecting gas through an upward‐pointing capillary nozzle. High‐speed visualization indicates that the formation of microbubbles arises from the convergence of the capillary waves induced by the partial coalescence of larger bubbles. A bubbling regime map is given to identify the critical conditions for the formation of microbubbles. In the present air‐water experiments, the generated microbubbles are 20–170 μm in diameter. From experimental data, a scaling law for microbubble size is proposed as a function of Weber and Bond numbers.
“…The most peculiar observation from Figure 13 is the spontaneous formation of a bi-modal distribution in the presence of both samples of pure HPMC molecules. It is known that pure water exhibits a bimodal bubble size distribution, which has been connected to different bubblebubble interactions (Quinn and Finch, 2012). According to the current frother knowledge, the distribution always progresses towards a uni-modal distribution when the frother concentration approaches its CCC, as is observed in the case of pure NF240 (Finch et al, 2008;Jàvor, 2014).…”
“…example. The distribution in pure water is of a bi-modal nature, which was previously attributed to bubble-bubble interactions by Quinn and Finch [54]. It has been generally observed that such bi-modal distribution progresses towards a uni-modal distribution as the frother concentration approaches its critical coalescence concentration (CCC) value [14,55].…”
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