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                    Electrostatistic Precipitation                                            161

                    where A′ and B′ are constants for a specific gas and δ′ is the relative gas density taken
                                                                            5
                    with respect to 1 atm and 25°C. For air, the values A′ = 32.2×10 V/m and B′ = 8.46×10 4
                    V/m 1/2  are recommended. Values for other gases are reported in the literature (16).
                    Example 1
                       Find the corona-starting voltage for a duct precipitator of a 28-cm plate-to-plate spacing
                       and a 10-cm wire-to-wire spacing and a 109-mil diameter wire. Assume that the gas is air
                       at 40°C and 2 atm. Compare with a 109-mil-diameter wire in a 28-cm-diameter cylinder.
                       Solution
                       The corona-starting voltage for duct geometries is given by Eq. (13), for which E and
                                                                                          c
                       d′are required. E can be determined from Eq. (16) for which δ´ is required:
                                    c
                                              δ′=  T P  =  298  ×  2  = 190.
                                                    0
                                                   T P    313   1
                                                      0
                                                                     −
                                                                      3
                                             2r = 109  mils = 2.77 ×  10 m
                                              0
                       Thus, from Eq. (16),
                                                               846  × 10 4    
                                                                 .
                                            .
                                      E = 190  322.  × 10 5  +             12 /  
                                       c
                                                         (139.  × 10 −3  × 19 )   
                                                                          .
                                                   6
                                         = 9.25  × 10 V m
                       Now, d′ = 4b/π, where b is the wire-to-plate spacing and is assumed to be one-half of the
                       plate-to-plate spacing (i.e., the wires are assumed to be placed midway between the plates);
                       thus, b = 0.14 m. Therefore, d′ = (4)(0.14)/π= 0.178 m; thus, from Eq. (13),
                                                                      0 178   
                                                                        .
                                      V = (139  × 10 −3 )(9 25.  × 10 6  ) ln
                                            .
                                       0                                       
                                                                    139.  × 10 −3
                                         = 62.4 ×  10 V
                                                   −
                                                    3
                       The starting voltage for the cylinder is given by Eq. (8). Thus,
                                                                      014    
                                                                        .
                                            .
                                      V = (925  × 10 6 )(1 39.  × 10 −3 ) ln
                                       0                                     −3 
                                                                    139.  × 10
                                         = 59.3 ×  10 V
                                                   −
                                                    3
                       (Note that r = 0.14 m.) For equal duct width (parallel-plate spacing) and cylinder diameter
                                1
                       and identical wire size, the cylinder-starting voltage will always be lower than the duct-
                       starting voltage. In industrial precipitators, corona-starting voltages are somewhat lower
                       than calculated estimates because of irregular electrode spacing and extraneous discharges
                       from dust films, nicks, and the like on corona wires. In ducts, this is also attributable to the
                       lower starting voltage of the end wires.
                       Corona discharge is accompanied by a relatively small flow of electric current. Sparking
                    usually involves a considerably larger flow of current, which cannot be tolerated. However,
                    with suitable controls, precipitators have been operated continuously with a small amount
                    of sparking to make certain that the voltage is in the correct range to ensure corona.
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