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                    Electrostatistic Precipitation                                            181

                       From Eqs. (45)–(48), we obtain

                         N =   Q vDH = (20 000  ) (100/  )(0 25.  )( ) =10  80  ducts
                                           ,
                           d
                         N =   r H L = (09  )( ) ( ) =10 /  3  3 sections
                                          .
                                    p
                           s
                               a
                          D =  N D = ( )(0 25 ) = 20  m
                                       80
                                            .
                                 d
                           t
                          L =  N L + ( N − ) 1  L +  L +  L out  = ( )( ) + (3  − )(0 3 ) + 4  + 4  = 17 6  m
                                                                            .
                                                                                           .
                                                              33
                                                                         1
                                        s
                           t
                                               s
                                                   in
                                s
                                  p
                                                                    2
                          A = 2HL p  N N = ( )( )( )( )( ) =14 400 m  (>14,000 m 2 )
                                           21
                                                      8
                                                       0
                                                             ,
                                                 3
                                              0
                                                   3
                                       d
                           a
                                     s
                    3.4. Electrode Systems
                       Good precipitator design provides for definite structural relationships between the
                    electrode systems: discharge electrode and collecting electrode. The type and position-
                    ing of the discharge and collecting electrodes can be major factors in the operation and
                    maintenance of an ESP. As illustrated in Fig. 6, the discharge electrode system consists
                    of a high-voltage duct, feed-through support insulator, tension support insulator, upper
                    support grid, discharge electrode vibrator and wires, lower alignment grid, and weight
                    tension. The discharge wires energized negatively are usually designed of round, 12-
                    gage steel spring wires with sharp edges to facilitate the formation of a corona around
                    them. They are reinforced at the top and bottom to ensure good electrical contact and to
                    resist mechanical and electrical erosion. The discharge wires are taut by weights and posi-
                    tioned through guides to prevent excess swaying. The wires tend to be high-maintenance
                    items. Corrosion can occur near the top of the wires because of air leakage and acid
                    condensation. Moreover, long weighted wires tend to oscillate. The middle of the wire
                    can approach the collecting plates quite closely, causing increased sparking and wear.
                    Some types of discharge wire are illustrated in Fig.10.
                       The collecting electrode system is designed to have maximum collecting surface,
                    high-sparkover voltage characteristics, no tendency to buckle or warp, resistance to
                    corrosion, and aerodynamic shielding of collecting surfaces to minimize re-entrainment
                    of the collected particles. Standard planar electrodes are usually made of cold-rolled
                    steel sheets to ensure flatness. Collecting electrode panels are grouped within the pre-
                    cipitator housing to form independently suspended and independently rapped collecting
                    electrode modules, and they are rapped periodically by electromechanical means.
                    Because the collecting electrodes are generally cleaned by the rapping and dropping
                    of collected particles by gravity, they have to be separated at a sufficient distance for
                    the free fall of the particles. This leads to widening the distance between electrodes,
                    which, in turn, requires a higher voltage to produce the desired corona discharge. The
                    dimensions of the electrode systems are fixed largely by the required voltage and area of
                    electrode surface per unit volume of gas. Some types of collecting plate are illustrated
                    in Fig.10.
                    3.5. Power Requirements
                       The power requirements for an electrostatic precipitator vary with collection effi-
                    ciency. It is important for the power supply to deliver a unidirectional current to the
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