Page 411 - Design and Operation of Heat Exchangers and their Networks
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394   Design and operation of heat exchangers and their networks


          (hot fluid) by Eq. (8.1). The measured temperature and pressure of the
          refrigerant (cold fluid) before entering the expansion valve are t 1 and p 1 ,
          and those after the expansion valve are t 2 and p 2 . Using these measured data,
          we have the enthalpy of the subcooled refrigerant before entering the expan-
          sion valve as h 1 ¼h(t 1 , p 1 ) and the enthalpy after the expansion valve h 2 ¼h 1 .
          The vapor mass fraction at the evaporator inlet can be approximately eval-
          uated by the thermodynamic vapor quality x 2 :

                                            h 2  h s,l
                                   _ x 2   x 2 ¼                       (8.9)
                                           h s,v  h s,l
             In the experiment, the outlet state of the refrigerant should be kept in the
          superheated range, that is, t 3 >t s (p 3 ). In such a case, h 3 ¼h(t 3 , p 3 ), the heat
          load can be obtained from the refrigerant side with Eq. (8.8), and the energy
          balance error can be evaluated by Eq. (8.6). If the refrigerant at the outlet of
          the evaporator lies in the two-phase region (t 3  t s,3 , h(t 3 , p 3 )<h s,v ), the out-
          let state of the refrigerant has to be determined by the energy balance
          between the refrigerant and the chilled water, which yields

                                        _ m w c p,w,m t 4  t 5 Þ
                                               ð
                               h 3 ¼ h 2 +                            (8.10)
                                              _ m r
                                            h 3  h s,l
                                   _ x 3   x 3 ¼                      (8.11)
                                           h s,v  h s,l
             In such a case, the energy balance error of the evaporator cannot be eval-
          uated. To evaporate the refrigerant completely, we can add a heater to the
          refrigerant pipe after the evaporator, as is shown in Fig. 8.2B. Neglecting the
          pressure drop and heat loss in the heater and using the measured heat duty of
                                                                   0,
          the heater Q 3 and the measured temperature after the heater t 3 we can
          express the heat load of the refrigerant flow as

                                       ð
                                     ½
                                         0
                              Q r ¼ _m r h r t 3 , p 3 Þ h 2 Š Q 3    (8.12)
          The enthalpy at the outlet of the evaporator is calculated with
                                                                      (8.13)
                                    h 3 ¼ h 2 + Q r = _m r
          The vapor mass fraction and energy balance error can then be evaluated with
          Eq. (8.11), (8.6), respectively.

          8.1.2 Measurement of heat transfer coefficient
          For the research and development purposes, people have more interest on
          experimental determination of heat transfer coefficients of different heat
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