Page 443 - Handbook of Energy Engineering Calculations
P. 443

D  = 1.75 d (nN )      0.47
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                                                                      PT
                                                     o
               This  gives  the  approximate  shell  diameter  for  a  packed  floating-head
               exchanger. The diameter will differ slightly for a fixed tubesheet, U-bend, or
               a multipass shell. For greater accuracy, tube-layout tables can be used to find
               shell diameters.
                  The following shows how the design equations are developed for a heat

               exchanger  with  sensible-heat  transfer  and  Reynolds  number  10,000  on  the
               tubeside, and with sensible-heat transfer and cross-flow (flow perpendicular
               to  the  axis  of  tubes)  on  the  shellside.  Equations  with  other  heat-transfer
               mechanisms are derived similarly.
                  For  the  film  coefficient  or  conductance,  h,  and  the  heat  balance,  these

               equations apply:




















                  Since  the  resistances  involved  in  a  tube-and-shell  exchanger  are  the

               tubeside  film,  the  tube  wall,  the  scale  caused  by  fouling,  and  the  shellside
               film, then:
                                               ΔT  + ΔT  +ΔT  +ΔT  = ΔT         M
                                                   i
                                                                 s
                                                          w
                                                                        o
               therefore:
                                    ΔT /ΔT  + ΔT /ΔT  + ΔT /ΔT  + ΔT /ΔT  = 1
                                                           M
                                                                        M
                                                     w
                                                                                      M
                                                                   s
                                        i
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                                            M
               or:


                  This last equation is obtained by dividing each heat-balance equation by

               ΔT   and  solving  for  ΔT /ΔT .  The  design  equations  are  derived  by
                   M
                                                 f
                                                      M
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