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4.5 Evaluation  155
                                                                Inlet







                                              Cover glass  Liquid  Slide glass



                                                                       Spacer
                                                                   Objective lens


                            Fig. 4.49. Fabricated sample chamber sealed with cover glass. When liquid is
                            dropped at the edge of the inlet it moves toward the center by surface tension


                            Tracer Method
                            Arbitrarily-shaped glass particles (n =1.51,ρ =2.54 gcm −3 ) ranging from
                            5to15 µm in size and the photoresist shuttlecock rotors (n =1.6,ρ =
                            1.16 gcm −3 )of10to30 µm in diameter were used in the experiment. They are
                            transparent to the YAG laser wavelength of 1.06 µm, which prevents optical
                            damage.
                               Tracers added to mark the flow included polystyrene, glass, gold, aluminum
                            oxide, diamond, tooth powder, pigment, a shampoo colloid and a milk fat col-
                            loid. Some of them are shown in Fig. 4.50. Polystyrene and glass are spherical,
                            but gold and aluminum have no definitive shape. The particles were dispersed
                            in water with a surface active agent, but the gold and aluminum were con-
                            densed due to electrostatic force.
                               Figure 4.51 shows the results for microflow analyzed by the tracer method
                            for the 1.0 µm glass beads in 30% glycerol solution. We recorded a 2.3-second
                            motion (71 frames) with a high-speed camera. The resolution was 640×240×8
                            bits per frame.
                               The velocity and the direction of each of beads #1 through #6 were traced
                            as the pathlines. In the figure, the following interesting characteristics of mi-
                            croflow are recognized.
                             1. The flows are strongfor tracers #2, #3, and #4, which were very close
                               at the rotor, but weak for #1, #5, and #6, which were at very distant
                               locations.
                             2. The flows expand to two to three times the rotor diameter.
                            Figure 4.52 show the variation in the tracer velocity due to the rotor and the
                            Brownian motion. Microflow and the diffusion effect will promote stirringor
                            mixingin microscale systems.
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