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首页> 外文期刊>Langmuir: The ACS Journal of Surfaces and Colloids >Control of initiation, rate, and routing of spontaneous capillary-driven flow of liquid droplets through microfluidic channels on slipchip
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Control of initiation, rate, and routing of spontaneous capillary-driven flow of liquid droplets through microfluidic channels on slipchip

机译:通过滑片上微流体通道控制毛细管自发驱动的液滴的流动的起始,速率和路径

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This Article describes the use of capillary pressure to initiate and control the rate of spontaneous liquid-liquid flow through microfluidic channels. In contrast to flow driven by external pressure, flow driven by capillary pressure is dominated by interfacial phenomena and is exquisitely sensitive to the chemical composition and geometry of the fluids and channels. A stepwise change in capillary force was initiated on a hydrophobic SlipChip by slipping a shallow channel containing an aqueous droplet into contact with a slightly deeper channel filled with immiscible oil. This action induced spontaneous flow of the droplet into the deeper channel. A model predicting the rate of spontaneous flow was developed on the basis of the balance of net capillary force with viscous flow resistance, using as inputs the liquid-liquid surface tension, the advancing and receding contact angles at the three-phase aqueous-oil-surface contact line, and the geometry of the devices. The impact of contact angle hysteresis, the presence or absence of a lubricating oil layer, and adsorption of surface-active compounds at liquid-liquid or liquid-solid interfaces were quantified. Two regimes of flow spanning a 10 ~4-fold range of flow rates were obtained and modeled quantitatively, with faster (mm/s) flow obtained when oil could escape through connected channels as it was displaced by flowing aqueous solution, and slower (micrometer/s) flow obtained when oil escape was mostly restricted to a micrometer-scale gap between the plates of the SlipChip ("dead-end flow"). Rupture of the lubricating oil layer (reminiscent of a Cassie-Wenzel transition) was proposed as a cause of discrepancy between the model and the experiment. Both dilute salt solutions and complex biological solutions such as human blood plasma could be flowed using this approach. We anticipate that flow driven by capillary pressure will be useful for the design and operation of flow in microfluidic applications that do not require external power, valves, or pumps, including on SlipChip and other droplet- or plug-based microfluidic devices. In addition, this approach may be used as a sensitive method of evaluating interfacial tension, contact angles, and wetting phenomena on chip.
机译:本文介绍了如何使用毛细管压力来启动和控制通过微流体通道的自发性液-液流动速率。与外部压力驱动的流体相反,毛细管压力驱动的流体主要受界面现象的影响,并且对流体和通道的化学成分和几何形状极为敏感。通过使包含水性液滴的浅通道滑入与填充有不混溶油的稍深通道接触,可在疏水性SlipChip上开始逐步改变毛细作用力。该作用引起液滴自发流入更深的通道。基于净毛细作用力与粘性流动阻力之间的平衡,建立了一个预测自发流速的模型,该模型以液-液表面张力,三相水-油在油中的前进和后退接触角为输入。表面接触线以及设备的几何形状。量化了接触角滞后,润滑油层存在与否以及液-液或液-固界面处表面活性化合物吸附的影响。获得了两种流率范围为10〜4倍的流态并对其进行了定量建模,当油因流动的水溶液而被驱替时,油可以通过连接的通道逸出时获得的流速更快(mm / s),而速度更低(微米) / s)时,逸出的油大部分被限制在SlipChip板之间的微米级间隙(“死端流动”)。润滑油层破裂(让人联想到卡西-温泽尔转变)被认为是模型与实验之间差异的原因。稀盐溶液和复杂的生物溶液(例如人血浆)都可以使用此方法流动。我们预计,在不需要外部动力,阀门或泵的微流体应用中,由毛细管压力驱动的流体将对流的设计和运行非常有用,包括在SlipChip和其他基于液滴或塞子的微流体设备上。另外,该方法可用作评估界面张力,接触角和芯片上润湿现象的灵敏方法。

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