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16    Cha pte r  T w o


                                    Dye 1
                         Dye 2
                                              Microchannel wall

                        Dye 3
                                                           To outlet
                        Dye 4


                                                   200 μm
                        Dye 5
                                   Dye 6
               FIGURE 2-3  Optical micrograph of laminar fl ow of six streams of different dye
               solutions in a microchannel fl owing from left to right. The height of the channel is
               100 μm. (Adapted with permission from D. B. Weibel, M. Kruithof, S. Potenta,
               S. K. Sia, A. Lee, and G. M. Whitesides, “Torque-actuated valves for
               microfluidics,” Anal. Chem., 77, (2005), 4726–4733. Copyright 2005
               American Chemical Society.)


               example of laminar flow of six different streams of solutions of dye
               flowing (from left to right) into a single channel. There is no turbulent
               mixing, and the interface between these laminar streams remains par-
               allel and distinct. Note that this interface is at dynamic steady state: a
               continuous flow of liquids is necessary to maintain this interface. As a
               result, manipulating the conditions of flow can reconfigure the shape
               and position of this interface dynamically. This feature is attractive for
               some applications in optics, and has been exploited for constructing
               optical devices; more details can be found in Chap. 3.

               2-5-2 Diffusion
               Although there is no turbulence, mixing in laminar streams still
               occurs due to diffusion. There is a transverse (in the y direction in
               Fig. 2-4) concentration gradient across laminar streams that contain
               different concentrations of solutes (or other properties, such as tem-
               perature). Transverse diffusion of solutes broadens the laminar inter-
               face, flattens the concentration gradient across the streams, and
               homogenizes the liquids. Figure 2-4 shows this idea. To visualize the
               spatial extent of transverse diffusive mixing, two nonfluorescent
               chemical species (carried separately by the two flowing solution
               streams) are used. The product of these two species is fluorescent,
               and can therefore be imaged with a confocal microscope.
                  The Péclet number (Pe ≡ vw/D) compares the typical time scale
               for diffusive transport to that for convective transport (for channel
               width w, velocity of fluid v, and diffusivity D) [32]. For solute ions
               with typical diffusivity D ~ 2 × 10 μm s  flowing through a channel
                                            3
                                               2 −1
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