Page 267 - Chemical Process Equipment - Selection and Design
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234  DRYERS AND  COOLING TOWERS






                                -


                   T, = 250 F                      T2=100F
                                                     =
                                                    H
                  T*=  101.5 F               - 0.043                                     = 45,455 lb/hr
                                                                                  l5Oo
                                               1  OOHIH, = 73%          Dry air =  0.043 - 0.010
                   H = 0.01 0  Ib/lb dry
                                                   V,  = 15.3 CWlb dry
                   V,  = 18.2 CWlb dry                                        -+ 45945w3.2) = 229.8 cfs,
                                                                                  3600




                  5.  The  humid  volume  is  the  volume  of  llb of  dry  air  plus  the   9.2.  RATE OF  DRYING
                    volume of  its associated water vapor,
                                                                     In a typical drying experiment,  the  moisture content  and possibly
                       V, = 0.73(1/29 + h/18)(T + 459.6)/P,          the  temperature  of  the  material  are measured  as functions of  the
                                                                     time. The inlet and outlet rates and compositions of the gas also are
                          cuft/(lb dry air).                  (9.9)   noted.  From  such  data,  the  variation  of  the  rate  of  drying with
                                                                     either the moisture content or the time is obtained by mathematical
                  6. Humid specific heat is                          differentiation.  Figure  9.3(d)  is  an  example.  The  advantage  of
                                                                     expressing drying data in the form of  rates is that their dependence
                       C, = C,  + C,H  = 0.24 + 0.45H,  Btu/(F)(lbdryair).  (9.10)   on  thermal  and  mass  transfer  driving  forces  is  more  simply
                                                                     correlated. Thus, the general drying equation may be written
                  7. The wet bulb temperature  T,  is attained by measurement under
                    standardized conditions. For water,  T,, is numerically nearly the
                    same as the adiabatic saturation temperature T,.     ---= dW  h(T,- T)=k,(P-P,)=k,(H-H,),    (9.13)
                  8.  The  adiabatic  saturation  temperature  T, is  the  temperature   A de
                    attained if  the gas were saturated by an adiabatic process.
                  9.  With heat capacity given by item 6, the enthalpy of  humid air is   where  subscript g refers  to  the  gas phase  and H  is  the  moisture
                                                                     content,  (kg/kg  dry material),  corresponding to a partial or vapor
                       h = 0.24T + (0.45T + 11OO)H.           (9.11)   pressure  P.  Since  many  correlations  of  heat  and  mass  transfer
                                                                     coefficients are  known,  the  effects of  many  changes in  operating
                  On the psychrometric chart of  Figure 9.1, values of  the saturation   conditions on drying rates may be ascertainable. Figures 9.3(g) and
                  enthalpy h, and a correction factor D are plotted. In these terms the   (h) are  experimental evidence of  the effect of  humidity of  the  air
                  enthalpy is                                        and (i) of  the effect of  air velocity on drying rates.
                                                                         Other  factors,  however,  often  complicate  drying  behavior.
                     h = h, + D.                              (9.12)   Although in some ranges of  moisture contents the  drying process
                                                                     may be  simply evaporation off  a surface, the surface may not  dry
                                                                     uniformly  and  consequently the  effective amount  of  surface may
                  In Figure 9.2, the enthalpy may be found by interpolation between
                  the lines for saturated and dry air.               change as time goes on. Also, resistance to diffusion and capillary
                     In some  periods  of  drying  certain  kinds  of  solids,  water  is   flow of  moisture may develop for which  phenomena no  adequate
                  brought  to  the  surface  quickly  so  that  the  drying  process  is   correlations  are  known.  Furthermore,  shrinkage  may  occur  on
                                                                     drying,  particularly  near  the  surface,  which  hinders  further
                  essentially  evaporation  of  water  from  the  free  surface.  In  the
                  absence  of  intentional  heat  exchange  with  the  surrounding  or   movement of  moisture outwards. In other instances, agglomerates
                  substantial heat losses, the condition of  the air will vary along the   of  particles may disintegrate on partial drying.
                  adiabatic saturation line. Such a process is analyzed in Example 9.1.   Some examples of  drying data appear in Figure 9.3. Commonly
                     For  economic  reasons,  equilibrium  conditions  cannot  be   recognized  zones  of  drying  behavior  are  represented  in  Figure
                  approached closely. In a cooling tower, for instance, the effluent air   9.3(a). Equilibrium moisture contents assumed by various materials
                  is not quite saturated, and the water temperature is not quite at the   in  contact with  air  of  particular  humidities is represented  by  (b).
                  wet  bulb  temperature.  Percent  saturation  in  the  vicinity of  90%   The  shapes  of  drying  rate  curves  vary  widely  with  operating
                  often  is  feasible.  Approach  is  the  difference  between  the   conditions and  the  physical state  of  the solid; (b)  and  others  are
                  temperatures  of  the  water  and  the  wet  bulb.  It  is  a  significant   some  examples.  No  correlations  have  been  developed or  appear
                  determinant of  cooling tower sizk as these selected data indicate:   possible whereby such data  can be predicted.  In higher ranges of
                                                                     moisture  content  of  some  materials,  the  process  of  drying  is
                    Approach ("F)    5   10    15   20    25         essentially evaporation  of  moisture  off  the  surface,  and  its  rate
                    Relativetowervolume  2.4   1.6   1.0   0.7   0.55   remains constant until  the  surface moisture is  depleted  as long as
                                                                     the condition of  the air remains the same. During this period, the
                  Other criteria for dryers and cooling towers will be cited later.   rate is independent of  the nature of  the solid. The temperature  of
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