Page 106 - Defrosting for Air Source Heat Pump
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98                                          Defrosting for Air Source Heat Pump

         temperature of the melted frost when it was downward flowing, were hardly impos-
         sible to be measured. Third, some parameters were easy to measure, but not accurate
         due to their fluctuations, such as the temperature of the air around the outdoor coil. In
         the experimental study, this type of parameter was always measured by many sensors
         and/or tested many times. Therefore, the following modeling study takes the respon-
         sibility to measure the previous three types of parameters.


         4.3.1.2 Modeling study

         The development of the validated semiempirical model at the setting of without using
         water-collecting trays between circuits for the experimental ASHP unit was separately
         introduced previously. However, for the completeness of the current section, it is
         briefly described here. The prototype of this model was Case 1 in the previous exper-
         imental study. Details of the vertical three-circuit outdoor coil without a water-
         collecting tray installed between circuits were shown in Fig. 4.18A, and a conceptual
         model for the airside of the three-circuit outdoor coil is shown in Fig. 4.19. Before the
         model was built, a series of assumptions were given, such as the frost at the surface of
         each circuit was even, the refrigerant mass flow was evenly distributed, and so on. At
         the same time, as mentioned previously, some of experimental results obtained were
         used as known parameters when the model was developed.
            In this model, a defrosting process on the airside of the outdoor coil was divided
         into four stages: (1) preheating, (2) frost melting without water flowing away from a
         circuit, (3) frost melting with water flowing away from a circuit, and (4) water layer
         vaporizing. The schematics of mass and energy flows in the four defrosting stages
         were shown in Fig. 4.2. Moreover, as part of the entire setup of the three-circuit out-
         door coil, a mathematical submodel for the heat and mass flows on a water-collecting
         tray and a water-collecting cylinder was also developed and used together with the
         model. As shown in Fig. 4.4, there were three steps for the process of the mass and
         energy flows in a water-collecting tray during defrosting.

                                     Outdoor coil (air side)
                 Refrigerant in
                                                        Thermal-couple

                          m w,j–1T w,j–1  Circuit 1

                           m w,jT w,j  m f,j  Circuit 2


                           m w, j+1T w,j+1  Circuit 3  Water collecting tray C
                                                     Refrigerant out
                      C  Water collecting cylinder C


         Fig. 4.19 Conceptual model for the airside of the three-circuit outdoor coil.
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