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Minimization of Hg and trace elements during coal combustion and gasification processes  77



            Table 3.4 Trace element removal and electrostatic precipitator (%)
             Element        Removal efficiency  Element        Removal efficiency
             Antimony       81.0              Copper          99.6
             Arsenic        99.1              Manganese       99.6
             Barium         99.8              Mercury         <20.0
             Beryllium      97.4              Molybdenum      96.0
             Cadmium        99.2              Nickel          98.2
             Chromium       99.2              Phosphorous     98.0
             Cobalt         99.3              Vanadium        99.5


            Data from Easom, B.H., Smolensky, L.A., Wysk, S.R., Altman, R.F., Olen, K.R., 1998. Electrocore separator for
            particulate air emissions. In: Proceedings of the 23rd International Technical Conference on Coal Utilisation and
            Fuel Systems, Clearwater, FL, USA, 9e13 Mar 1998. Coal and Slurry Technology Association, Washington, DC,
            USA, 683e692.
           surface area on an equal mass basis. ESPs have lower capture efficiencies for ultrafine
           particles, as smaller particles are more difficult to charge to a sufficient level for elec-
           trostatic collection. Table 3.4 shows the average removal efficiency for TEs across a
           conventional ESP on an unspecified boiler (Easom et al., 1998; Sloss and Smith, 2000).
              The distribution of TEs in the inlet and outlet of an ESP system burning a bitumi-
           nous Pittsburgh coal has been investigated (Tumati and DeVito, 1993). The concentra-
           tions of several TEs were measured in the coal, bottom ash, and ash sampled at the ESP
           inlet and outlet. The ESP retention efficiency for most solid phase TEs (except Ni, Se,
           and Cd) was close to the overall particle removal efficiency (99.54%) on a mass basis
           (Table 3.5).
              The effectiveness of ESP in removing Hg from flue gases is dependent on the tem-
           perature of the gases. On average, cold-side ESP systems (downstream of the air pre-
           heater, 135e175 C) capture around 30% of the mercury in the coal, the capture rate

           ranging from 0 to over 60% depending on the coal. Hot-side ESP systems (upstream of

           the air preheater, closer to the boiler, 300e400 C) show lower mercury capture
           (average 3%) (Sloss, 2008). The longer residence time and cooler temperature in the
           cold-side systems is more conducive to mercury adsorption onto fly ash than the
           shorter, hotter conditions in the hot-side ESPs. High flue gas cooling rates between
           the air preheater inlet and the air pollution control device inlet can enhance reaction
           rates associated with oxidation by species such as chlorine (Kolker et al., 2006).
              FFs (baghouses) are the main alternative to ESP for LCPs. Baghouses are often
           considered superior to ESP for the capture of fine particles and would therefore be ex-
           pected to have higher collection efficiencies for the associated TEs. Because baghouse
           collection efficiency is not affected by the resistance of the ash, baghouses are consid-
           ered superior for use with low-sulfur coals (Rentz et al., 1996). However, baghouses
           can have problems with on-line cleaning of high air-to-cloth ratio bags due to redisper-
           sion of collected particulates. The presence of unburnt carbon in ash enhances mercury
           capture by adsorbing oxidized mercury. Studies at a Western Kentucky power plant
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