Wageningen University, Food Process Engineering Group, Bornse Weilanden 9, 6708 WG, Wageningen, the Netherlands.
Wageningen University, Food Process Engineering Group, Bornse Weilanden 9, 6708 WG, Wageningen, the Netherlands.
J Colloid Interface Sci. 2022 Sep 15;622:218-227. doi: 10.1016/j.jcis.2022.04.115. Epub 2022 Apr 26.
The interplay of interface evolution and surfactant adsorption determines the formation and stabilization of bubbles, and can be controlled by the liquid phase properties.
We studied bubble formation in an Edge-based Droplet GEneration (EDGE) microfluidic device at relevant length and time scale, allowing investigation of sub-events in a single bubble formation cycle. We vary the properties of the continuous phase that contains whey proteins and study a range of trans-pore pressures (P).
The shallow pores highlight the crucial role of the Laplace pressure and dynamic adsorption of proteins to the meniscus. Bubble formation is divided into two regimes by the Laplace pressure of the bare meniscus inside the pore. At P<1400 mbar, pre-adsorption of proteins is required to lower the Laplace pressure; the bubble formation frequency f increases with increasing protein concentration and is hardly affected by velocity and viscosity. At P≥1400 mbar, bubble formation immediately occurs upon applying pressure, and f mainly decreases with increasing viscosity. In both regimes, the initial bubble size d mainly increases with the viscosity (~η). Bubble coalescence is only observed at P≥1400 mbar and can be effectively suppressed by raising protein concentration and viscosity within certain boundaries, yet ultimately this is at the cost of higher polydispersity of the bubbles. Our insights into the formation dynamics of micrometer-sized bubbles at time scales down to tens of microseconds can be used for effective control of bubble formation and stabilization in practical applications.
界面演化和表面活性剂吸附的相互作用决定了气泡的形成和稳定,并且可以通过液相性质来控制。
我们在相关的长度和时间尺度上研究了基于边缘的液滴生成(EDGE)微流控装置中的气泡形成,允许在单个气泡形成循环中研究子事件。我们改变了含有乳清蛋白的连续相的性质,并研究了一系列跨孔压力(P)。
浅孔突出了 Laplace 压力和蛋白质在弯月面的动态吸附的关键作用。气泡形成由孔内裸弯月面的 Laplace 压力分为两个区域。在 P<1400 毫巴下,需要预吸附蛋白质以降低 Laplace 压力;气泡形成频率 f 随蛋白质浓度的增加而增加,并且几乎不受速度和粘度的影响。在 P≥1400 毫巴下,施加压力后立即发生气泡形成,并且 f 主要随粘度的增加而降低。在这两种情况下,初始气泡尺寸 d 主要随粘度(~η)而增加。仅在 P≥1400 毫巴下观察到气泡聚结,并且可以通过在一定范围内提高蛋白质浓度和粘度来有效地抑制气泡聚结,但最终这是以气泡的更高多分散性为代价的。我们对数十微秒时间尺度下微米级气泡形成动力学的深入了解可用于有效控制实际应用中的气泡形成和稳定。