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4.6 Mixer Application for µ-TAS  163
                            4.6 Mixer Application for µ-TAS

                            Because the Reynolds number in a microchannel in future µ-TAS will be small,
                            mixingdevices that increase two liquid contact areas are proposed to promote
                            the diffusion effect. Interweavingof two liquids has been achieved by adopting
                            various structure geometries in a channel, such as micronozzle arrays and
                            intersectingchannelswhich induce chaotic flow, as shown in Fig. 4.63 [4.21].
                            These mixers have been characterized as static devices. On the other hand,
                            active micromixers with pressure perturbations that are applied transversally
                            to the main stream, as shown in Fig. 4.64 have been presented [4.22]. They
                            are called cross-channel mixers [4.23], fabricated by usingMEMS technology,
                            in which chaotic-like mixingis achieved in an efficient way. The optical mixer
                            proposed in this book is another type of active mixer to stir a liquid in a
                            microchannel [4.19].
                               µ-TAS is also called a Labs-on-a-chip. The chip will have components such
                            as inlets for loadingthe sample and reagent, microfabricated fluidic channels

                                                        pw            pw
                                     A          z
                                                          Df m       Df m       h
                                                              h
                                             x
                                                  u c d  c u         u  c   d  c  u
                                      w                                           z
                                     h
                                    a h                                               y
                                         2p/q                                    x
                                     B     0 cycles:     1/2 cycle:     1 cycle:
                                         z
                                                                    Df m
                                      x
                                                 100 mm
                            Fig. 4.63. Mixing by intersecting microchannels, which induces chaotic behavior of
                            microflow [4.21]. Courtesy of A. Stroock, Cornel University, USA

                                        Flow direction      Periodic perturbation







                                                                     100 mm
                            Fig. 4.64. Chaotic mixing by using the mechanical micromixer [4.22]. Courtesy of
                            Y.K. Lee, University of California, USA
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