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Absorption and reflection techniques 325

             the intensity at a nearby region where the gas is   defined shear by the flue gas. Thus a known and
             non-absorbing  (B) are alternately measured with   fixed path length is provided.
             a single detector 40 times per  second. Any light   When measuring  opacity  the instrument mea-
             level  change,  whether  due  to  source  variation,   sures the reduction in transmission  in the visible
             darkening  of  the window, scattering by  particu-   portion of the spectrum.
             lates, water  drops, or aerosols in the gas stream   Typical ranges covered by the instrument are:
             affects both A and B, leaving the ratio unchanged.
             This ratio gives a reading that is free of interfer-   NO   0-25  ppm to 0-5000  ppm
             ences.  instrumental  drift,  etc.  Most  gases  obey   CO   0-500  ppm to 0-3000  ppm
             approximately Beer's law:                    C02  0-15%
                                                          SOz   0-25  ppm to 0-10  000 ppm
                B = ~   e  ~   ~  '                       C-H   0-25  ppm to 0-6000  pplil
                                                          H20  0-1000  ppm to 0-80%
             01
                                                          NH3  0-100ppm
                In (BIA) = -ad
             or
                                                      16.1.3  Absorption in the visible and ultraviolet
                    ln(AIB)
                c=--                                  Two instruments are worthy of note here. The first
                      a1                              is the Barringer remote sensing correlation spectro-
             where  01  is  absorption  coefficient (known),  I  is   meter designed for the quantitative measurement
             path length (fixed), and c is sample concentration   of gases such as nitrogen oxides or sulfur dioxide in
             (unknown).                               an optical path between the instrument and a suit-
               The  system  response  is  almost  instantaneous   able  source  of  visible  and  ultraviolet  radiant
             and is averaged by  damping circuits to typically   energy. The sensor is designed for maximum ver-
             one second.                              satility in the remote measurement of gas clouds in
               The stack gas is separated from the source and   the  atmosphere,  using  the  day  sky  or  ground-
             analyzer enclosures by means of optical surfaces,   reflected solar illumination as the light source. It
             such as mirrors  or windows. These windows are   may  also be  used  with  artificial sources such as
             kept  clean  by  an  air  curtain  system.  Self-con-   quartz-iodine  or  high  pressure  Xe  lamps.  Very
             tained blowers continually renew the air curtains,   simply, the sensor contains two telescopes to collect
             preventing  the  gases  from  contacting  the  win-   light from a distant source, a two-grating spectro-
             dows directly (see Figure 16.7).         meter for dispersion of the incoming light, a disc-
               The flow volume and pressure of the purge air   shaped exit mask or correlator and an electronics
             is  designed for each  application  to allow  a well   system  (see  Figure  16.8).  The  slit  arrays  are


                                       Fan
              Window                   /























                                                         Figure 16.7  EDCflue gas analyzer. Courtesy
                                     Filter              Environmental Data Corp.
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