Page 454 - Handbook of Energy Engineering Calculations
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phenolic-resin coatings, among others, protect against corrosion from cooling
               water. Electrodes may also be wound into the assembly to anodically protect
               surfaces against corrosion.
                  Spiral-plate exchangers are normally designed for the full pressure of each
               passage. Because the turns of the spiral are of relatively large diameter, each

               turn  must  contain  its  design  pressure,  and  plate  thickness  is  somewhat
               restricted—for  these  three  reasons,  the  maximum  design  pressure  is  150
                     2
               lb/in   (1033.5  kPa),  although  for  smaller  diameters  the  pressure  may
               sometimes be higher. Limitations of materials of construction govern design
               temperature.
                  The  shortcut  rating  method  for  spiral-plate  exchangers  depends  on  the
               same  technique  as  that  for  shell-and-tube  heat  exchangers  (which  were

               discussed by Lord, Minton, and Slusser in the previous procedure).
                  Primarily,  the  method  combines  into  one  relationship  the  classical
               empirical  equations  for  film  heat-transfer  coefficients  with  heat-balance
               equations  and  with  correlations  that  describe  the  geometry  of  the  heat

               exchanger. The resulting overall equation is recast into three separate groups
               that  contain  factors  relating  to  the  physical  properties  of  the  fluid,  the
               performance  or  duty  of  the  exchanger,  and  the  mechanical  design  or
               arrangement  of  the  heat-transfer  surface.  These  groups  are  then  multiplied

               together  with  a  numerical  factor  to  obtain  a  product  that  is  equal  to  the
               fraction of the total driving force—or log mean temperature difference (ΔT                  M

               or LMTD)—that is dissipated across each element of resistance in the heat-
               flow path.
                  When the sum of the products for the individual resistance equals 1, the
               trial design may be assumed to be satisfactory for heat transfer. The physical
               significance is that the sum of the temperature drops across each resistance is

               equal to the total available ΔT . The pressure drops for both fluid-flow paths
                                                    M
               must  be  checked  to  ensure  that  both  are  within  acceptable  limits.  Usually,

               several trials are necessary to get a satisfactory balance between heat transfer
               and pressure drop.
                  Table 9 summarizes the equations used with the method for heat transfer
               and pressure drop. The columns on the left list the conditions to which each

               equation  applies,  and  the  second  columns  gives  the  standard  forms  of  the
               correlations  for  film  coefficients  that  are  found  in  texts.  The  remaining
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