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Contamination and Industrial Systems

            192   Chapter Nine

                          In some processes designed to precipitate chemical species, such as the
                        manganese-removal stages of drinking water treatment, highly opaque, physi-
                        cally hard and adherent films can build up on instrument windows in a few
                        hours (in this case black, highly absorbing films of manganese dioxide). Even
                        in clean drinking water supplies, nutrients and oxygen are always present,
                        allowing bacteria to grow and form “biofilms.” Again, this growth can be a fast
                        process. Ultrasmooth window surfaces of polished sapphire or highly inert
                        materials such as transparent PTFE and other fluoropolymers may delay the
                        onset of film growth, but once a few bacteria have taken hold, further growth
                        is often rapid. Films can range from predominantly transparent, sticky poly-
                        mers to hard, opaque layers with combined inorganic constituents from the
                        fluids themselves and from corrosion products of the pipe-work.
                          Reference-beam configurations, and in particular the four-beam approach
                        repeated in Fig. 9.1, are widely used to counter window fouling in these indus-
                        trial sensors. We calculate the ratio of “short” to “long” path intensities or scat-
                        tered to transmitted intensities:
                                                    È PP ˘          L L )
                                                      11 22
                                                               a
                                                Q =        =  e  - ( 11 22
                                                                LL - 12 21
                                                    Í Î PP ˚ ˙
                                                        21
                                                      12
                        which appears to be independent of source and detector window fouling. The
                        basis of the intensity compensation scheme is that the intensities measured
                        along paths L 11 and L 12 are perfectly proportional, no matter what is the level
                        of fouling, and the compensation scheme should be perfect. In practice, the



                        Sources                   Detectors
                                                    D 1        (b) Turbidity
                                      L 11
                         S 1                                   measurement
                                        a                              Source S
                                L 12                                         1

                                L 21
                                                    D 2            s
                                      L 22
                         S 2
                                                                                     D 1


                         (a) Absorption                Source S 2
                         measurement

                                                                               Detectors
                                                                        D 2
                        Figure 9.1 Four-beam compensation systems are used for (a) absorption and (b) scat-
                        tering measurements.


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