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Contamination and Industrial Systems

                                                            Contamination and Industrial Systems  205

                                                  Liquid
                        (a)
                                                  feed
                                                          Detector

                        Fiber-coupled
                        source             Hanging droplet

                        (b)


                         Optical
                         path
                                         Meniscus supported
                                         in perforated disc
                       Figure 9.13 Small liquid samples may be supported by
                       surface tension and probed in transmission without use of
                       wetted windows, either using hanging droplets or a thin film.




                       pump. Both of these pumped and immersed free-surface geometries can be used
                       for fluorescence detection and Raman spectroscopy, with similar nonfouling
                       advantages. They are also useful for reliable long-term video-based observation
                       of particles and flocs in industrial process streams.


           9.5.2 Transmission measurements and
           the bubble interface
                       The nonfouling characteristic of the liquid-air interface is equally attractive
                       for transmission-geometry measurements, although it is less obvious how to
                       arrange this. A good starting point is the hanging droplet of Fig. 9.13a. By eject-
                       ing a small droplet from a capillary, an unbounded sample is formed which can
                       be probed for optical absorption, fluorescence, etc. When small droplets (<2mm
                       diameter) are used they can be accurately spherical, and useful as a lens to focus
                       light from a small source or optical fiber onto a detector. Bigger drops become
                       more pendulous, leading to severe aberrations. Hence we are limited to rather
                       small path lengths and poor sensitivity. Total internal reflection can be used to
                       increase the path length, but this is difficult to control (Liu et al., 1995). Figure
                       9.13b shows another approach, more suitable for high viscosity liquids like oils
                       and gelatinous film emulsions. A perforated disk is dipped into a bath of the
                       sample and removed, leaving a meniscus supported in the hole. This can be used
                       for windowless optical measurements free from gross fouling. As with the
                       droplet, the path-length is rather short.
                         A more promising technique is the “holey-cup” of Fig. 9.14. Here we have
                       drilled a 0.5mm diameter hole in the base of a plastic cup, subsequently filled
                       with water. As long as the hole is not too large, and the water head not too high,
                       water will not flow through the hole, but will be retained by surface tension
                       around the hole periphery. The 0.5mm hole will support a 40mm depth of clean

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