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                                                                    Heat Transfer                                          117

                                                          Condensate layer, outside of tube, t 2


                                                                          Scale thickness, resistance, ri
                                Warm or condensing
                                side of tube                                 Stagnant film of water, t 7
                                                        Metal wall                            t  (bulk)
                                                        thickness = L                          8
                                                                 W
                                                  t
                                                  2
                                                                                         Coolant side, cool
                                   t , t
                                    1  V
                                                t
                                                 4
                                                   ∆
                                                    m
                                                                                              t 2
                                       Direction of                                           t
                                       heat flow                                               6
                                          Process                                                  ∆
                                        Saturated                                                   Overall, t – t 8
                                                                                                              1
                                          vapor,
                                          t or t V
                                           1
                                          (bulk)
                                                                                        t , t 5
                                                                                         W
                                                                                        Water in
                                                                                        turbulent motion
                                              t 3                                       (or coolant), t
                                 Condensing side                                                      8
                                 scale, dry                 t 4

                     Figure 10-66. Condensing vapors on cooling metal (or other) wall (also see Figure 10-28). Note that t 4 and t 5 are wall temperatures and may be
                     essentially equal to t w   wall. This illustration is not for vertical tube, but represents the condensing/cooling mechanism.

                                                                           where
                             t   d o for vertical tube (perimeter), ft
                                                                                 k l   liquid thermal conductivity, Btu/(hr) (ft)(°F)
                          d o   tube outside diameter, ft
                                                                                   l   liquid density, lb/ft 3
                               mass rate of flow of condensate from lowest point on
                                                                                   v   vapor density, lb/ft 3
                               condensing surface divided by the breadth (unit      latent heat of vaporization, Btu/lb
                               perimeter), lb/(hr) (ft). For a vertical tube:
                                                                                 g   acceleration of gravity, ft/(sec) (sec)
                               w/ D.
                                                                                 L   tube length, ft
                          G    condensate loading for horizontal tubes, lb/(hr) (ft)
                                                                                T sat   saturation temperature, °F
                          G    condensate loading for vertical tubes, lb/(hr) (ft).
                                                                                T w   surface temperature, °F
                                                                                  l   liquid viscosity, lb/(ft) (hr)
                                         70
                                82
                       McAdams and Kern both suggest the same relationship
                     for condensation on the outside of vertical tubes:
                                                                               4G¿ o
                                                                            For    6 2,000                              (10-73)
                            2 1>3
                          1  f 2      14G¿2   1>3                                 t
                                                                                       3 2
                      h c         1.47                            (10-71)             k f   f g  1>3  k f   tg N t D o  1>2
                                                                                                      3 2
                           3 2
                          1k f   f g2   1  f 2                              h cm   0.945c  d    0.945c         d       (10-73A)
                                                                                        f  G o ¿          f W
                                                        8
                           g   acceleration of gravity, 4.17   10 , ft/(hr) (hr)   W
                                                                            G o ¿      , lb.>hr. 1linear foot2         (10-73B)
                                                                                  N t D o
                       Bell 172  suggests the relation:
                                                                             For 4 G o   /  f   2,000 (reference 82),the following equa-
                                3
                               3k l   l 1  l    v 2 g4  1>4                tion is usually applicable to long tubes and high flow rates;
                      h c   0.943                                 (10-72)
                                3  l L1T sat   T w 24                      the average film coefficient:
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