Lerch Margaret A, Hoffman Michelle D, Jacobson Stephen C
Department of Chemistry, Indiana University, Bloomington, Indiana 47405-7102, USA.
Lab Chip. 2008 Feb;8(2):316-22. doi: 10.1039/b713500a. Epub 2007 Dec 5.
We report enhanced sample confinement on microfluidic devices using a combination of electrokinetic flow from adjacent control channels and electric field shaping with an array of channels perpendicular to the sample stream. The basic device design consisted of a single first dimension (1D) channel, intersecting an array of 32 or 96 parallel second dimension (2D) channels. To minimize sample dispersion and leakage into the parallel channels as the sample traversed the sample transfer region, control channels were placed to the left and right of the 1D and waste channels. The electrokinetic flow from the control channels confined the sample stream and acted as a buffer between the sample stream and the 2D channels. To further enhance sample confinement, the electric field was shaped parallel to the sample stream by placing the channel array in close proximity to the sample transfer region. Using COMSOL Multiphysics, initial work focused on simulating the electric fields and fluid flows in various device geometries, and the results guided device design. Following the design phase, we fabricated devices with 40, 80, and 120 microm wide control channels and evaluated the sample stream width as a function of the electric field strength ratio in the control and 1D channels (E(C)/E(1D)). For the 32 channel design, the 40 and 80 microm wide control channels produced the most effective sample confinement with stream widths as narrow as 75 microm, and for the 96 channel design, all three control channel widths generated comparable sample stream widths. Comparison of the 32 and 96 channel designs showed sample confinement scaled easily with the length of the sample transfer region.
我们报告了在微流控设备上实现增强的样品限制,方法是结合使用来自相邻控制通道的电动流以及通过与样品流垂直的通道阵列进行电场整形。基本的设备设计包括一个单一的一维(1D)通道,与32个或96个平行的二维(2D)通道阵列相交。为了在样品穿过样品转移区域时最小化样品扩散和泄漏到平行通道中,在1D通道和废液通道的左侧和右侧设置了控制通道。来自控制通道的电动流限制了样品流,并在样品流和2D通道之间起到缓冲作用。为了进一步增强样品限制,通过将通道阵列放置在靠近样品转移区域的位置,使电场与样品流平行整形。使用COMSOL Multiphysics,初始工作集中在模拟各种设备几何形状中的电场和流体流动,并将结果用于指导设备设计。在设计阶段之后,我们制造了具有40微米、80微米和120微米宽控制通道的设备,并评估了样品流宽度作为控制通道和1D通道中电场强度比(E(C)/E(1D))的函数。对于32通道设计而言,40微米和80微米宽的控制通道产生了最有效的样品限制效果,样品流宽度窄至75微米;对于96通道设计,所有三种控制通道宽度产生的样品流宽度相当。32通道设计与96通道设计的比较表明样品限制很容易随着样品转移区域的长度进行缩放。