Page 165 - Design and Operation of Heat Exchangers and their Networks
P. 165

Thermal design of evaporators and condensers  153


                                       2
                           2
              with α in W/m K, q in W/m , and p in bar. The validity range of Eq. (4.10)
                                       4     2       6     2
              is 0.5bar<p<20bar, and 10 W/m <q<10 W/m .
                 A widely used correlation was proposed by Cooper (1984):
                           α ¼ Cq 0:67 M  0:5  p r  0:12 0:2lgR a ½  lg p r   0:55  (4.11)
                                                        ðފ
                                       2
                           2
              with α in W/m K, q in W/m , molecular mass M in kg/kmol, and rough-
              ness R a in μm. For stainless steel C¼55, and for horizontal copper tube
              C¼93.5. We can take C¼90 for evaluation. The reduced pressure is
              defined as

                                          p r ¼ p=p cr                   (4.12)
                 For an accurate evaluation, it is suggested to use the Gorenflo correlation
              (Gorenflo, 2013):

                                                  F                      (4.13)
                                        α ¼ α 0 F q F p r w
                             n
              where F q ¼(q/q 0 ) , α 0 is the heat transfer coefficient for a specific fluid at a
                                                                             2
              reference state, α 0 ¼α(q 0 , p r0 ), the reference heat flux q 0 ¼20,000W/m ,
              and the reference reduced pressure p r0 ¼0.1. The values of α 0 for many fluids
              can be found in Table 1 of Gorenflo (2013). In the absence of data, α 0 can be
              evaluated by
                                                         2
                                                0:6
                               α 0 ¼ α 0,calc ¼ 3:58P f0  kW=m K         (4.14)
                                                   1
                                             (μmK) .
                                        ¼ p r0
              in which P f0 ¼[(dp/dT ) sat /σ] p r
                                                                              ,
                 The effects of heat flux and pressure are expressed by F q , and F p r
              respectively:
                                                  n
                                         F q ¼ q=q 0 Þ                   (4.15)
                                             ð
              For organic fluids and NH 3
                                      n ¼ 0:95 0:3p 0:3                  (4.16)
                                                   r
                                     ¼ 0:7p 0:2  +4p r +  1:4p r         (4.17)
                                  F p r    r
                                                    1 p r
              For water

                                      n ¼ 0:9 0:3p 0:15                  (4.18)
                                                   r
                                                      0:68p 2 r
                                          0:27
                                                   2
                                   ¼ 1:73p   +6:1p +                     (4.19)
                                          r        r      2
                                F p r
                                                      1 p
                                                          r
   160   161   162   163   164   165   166   167   168   169   170