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Measurand Modulation

                                                                        Measurand Modulation  217

                       perature coefficient issues of Chap. 8 addressed, this is a difficult and expensive
                       requirement.
                         Figure 10.2b shows a scheme in which the absorption coefficient is somehow
                       100 percent modulated. Synchronous detection can still be used, although the
                       detected signal is now much smaller (in this example about 10 times smaller).
                                                                                4
                       However, by making this change we have removed the requirement for unreal-
                       istic levels of source and gain stability. Measurand modulation greatly eases the
                       requirements on scale-factor stability. If the gain changes by 1 percent, this only
                       affects the measured peak-to-peak amplitude of the small modulation signal;
                       the change in static intensity is not seen. Hence, for 0.01 percent resolution of
                       the absorption, we only require that the noise of the transmitted signal is ade-
                       quately small, not that the gain is stable to 0.01 percent. This is an altogether
                       more realistic requirement. Now we will look at some of the means to modu-
                       late the measurand parameter of interest.
                         For instance we might vary the length of the transmission cell (Fig. 10.3),
                       recording the change in transmitted intensity at minimum and maximum cell
                       lengths, or even continuously as a function of sample length. Some care will be
                       required in collimating the beam, in translating the cuvette window to avoid
                       beam wobble and in choosing beam and detector sizes to avoid even small
                       changes in capture efficiency. We cannot escape the requirement to reduce
                       modulation-induced changes in detected intensity caused by these parasitic
                       effects. Synchronous intensity changes caused by such errors have to be reduced
                       to the full required relative precision, that is, to well below 0.01 percent.
                       Nevertheless, the system intrinsically downgrades slow source power and detec-
                       tor sensitivity variations, especially caused by temperature changes, to signal
                       scale-factor errors. Window contamination is also compensated.
                         The approach has been used by Horiba for in-situ absorption measurements
                       in wastewater. In an elegant design, a fixed source and a detector are immersed
                       in the fluid to be measured (Fig. 10.4). Eccentrically-mounted cylindrical silica
                       tubes then rotate together, varying the sample path-length L over a large frac-
                       tional change. The system suffers from a use of different window surfaces
                       during different parts of the measurement cycle, which opens up additional


                                     Contamination  R f


                                                 -
                                                 +A
                                                         Signal
                                              PD1
                       LED
                       source    Variable-length cell:
                                 - same contamination
                                 - different path length
                       Figure 10.3 Variable cell-length gives a modulated
                       intensity, with slow changes due to window contam-
                       ination compensated.


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