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Capillary pumping independent of the liquid surface energy and viscosity

机译:毛细管泵送与液体表面能和粘度无关

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摘要

Capillary pumping is an attractive means of liquid actuation because it is a passive mechanism, i.e., it does not rely on an external energy supply during operation. The capillary flow rate generally depends on the liquid sample viscosity and surface energy. This poses a problem for capillary-driven systems that rely on a predictable flow rate and for which the sample viscosity or surface energy are not precisely known. Here, we introduce the capillary pumping of sample liquids with a flow rate that is constant in time and independent of the sample viscosity and sample surface energy. These features are enabled by a design in which a well-characterized pump liquid is capillarily imbibed into the downstream section of the pump and thereby pulls the unknown sample liquid into the upstream pump section. The downstream pump geometry is designed to exert a Laplace pressure and fluidic resistance that are substantially larger than those exerted by the upstream pump geometry on the sample liquid. Hence, the influence of the unknown sample liquid on the flow rate is negligible. We experimentally tested pumps of the new design with a variety of sample liquids, including water, different samples of whole blood, different samples of urine, isopropanol, mineral oil, and glycerol. The capillary filling speeds of these liquids vary by more than a factor 1000 when imbibed to a standard constant cross-section glass capillary. In our new pump design, 20 filling tests involving these liquid samples with vastly different properties resulted in a constant volumetric flow rate in the range of 20.96–24.76 μL/min. We expect this novel capillary design to have immediate applications in lab-on-a-chip systems and diagnostic devices.
机译:毛细管泵送是液体致动的一种有吸引力的方法,因为它是一种被动机构,即在操作过程中它不依赖外部能量供应。毛细管流速通常取决于液体样品的粘度和表面能。对于依赖于可预测的流速并且毛细管粘度未知的样品粘度或表面能的系统来说,这带来了一个问题。在这里,我们介绍了样品液体的毛细管泵送,该样品液体的流速是恒定的,并且与样品粘度和样品表面能无关。这些特征通过一种设计得以实现,在该设计中,充分表征的泵送液体被毛细管吸入泵的下游部分,从而将未知的样品液体吸入上游泵部分。下游泵的几何形状设计为施加拉普拉斯压力和流体阻力,该压力和流体阻力比上游泵的几何形状施加在样品液体上的压力大得多。因此,未知样品液体对流速的影响可以忽略不计。我们用各种样本液体对新设计的泵进行了实验测试,包括水,不同的全血样本,不同的尿液样本,异丙醇,矿物油和甘油。当吸入标准横截面恒定的玻璃毛细管时,这些液体的毛细管填充速度变化超过1000倍。在我们的新泵设计中,涉及这些性质迥异的液体样品的20次填充测试导致了恒定的体积流量,范围为20.96–24.76μL/ min。我们希望这种新颖的毛细管设计能够立即应用于芯片实验室系统和诊断设备。

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