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Microbubble generation in a co-flow device operated in a new regime

机译:在以新方式运行的同流装置中产生微气泡

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A new regime of operation of PDMS-based flow-focusing microfluidic devices is presented. We show that monodisperse microbubbles with diameters below one-tenth of the channel width (here w = 50 μm) can be produced in low viscosity liquids thanks to a strong pressure gradient in the entrance region of the channel. In this new regime bubbles are generated at the tip of a long and stable gas ligament whose diameter, which can be varied by tuning appropriately the gas and liquid flow rates, is substantially smaller than the channel width. Through this procedure the volume of the bubbles formed at the tip of the gas ligament can be varied by more than two orders of magnitude. The experimental results for the bubble diameter d_b as function of the control parameters are accounted for by a scaling theory, which predicts d_b/w α (μ_g/μ_l)~(1/12)(Q_g/Q_l)~(5/12). where μ_g and μ_l indicate, respectively, the gas and liquid viscosities and Q_g and Q_l are the gas and liquid flow rates. As a particularly important application of our results we produce monodisperse bubbles with the appropriate diameter for therapeutic applications (d_b ≈ 5 μm) and a production rate exceeding 10~5 Hz.
机译:提出了一种新的基于PDMS的流聚焦微流体装置的运行方式。我们显示,由于通道入口区域中的压力梯度较大,在低粘度液体中可以产生直径小于通道宽度十分之一(此处w = 50μm)的单分散微气泡。在这种新的状态下,在长而稳定的气体韧带的末端会产生气泡,其直径可以通过适当调整气体和液体的流速来改变,该直径明显小于通道宽度。通过该程序,在气体韧带的尖端处形成的气泡的体积可以变化超过两个数量级。气泡直径d_b作为控制参数的函数的实验结果由比例理论解释,该理论预测了d_b / wα(μ_g/μ_1)〜(1/12)(Q_g / Q_1)〜(5/12) 。其中,μ_g和μ_1分别表示气体和液体的粘度,Q_g和Q_1是气体和液体的流速。作为我们结果的一个特别重要的应用,我们生产出直径合适的单分散气泡(d_b≈5μm),生产速度超过10〜5 Hz。

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