Page 195 - Defrosting for Air Source Heat Pump
P. 195

Frosting evenness coefficient                                     189

           of their FECs. In addition, the duration differences between the fin surface tempera-
           ture and the tube surface temperature are nearly the same, at 9 s for Case 1, 12 s for
           Case 2, and 10 s for Case 3, respectively.
              The energy used for the RCD comes from three sources: the power input to the
           compressor, the power input to the indoor air fan, and the thermal energy from indoor
           air. As shown in Table 6.7 and Fig. 6.39, the energy supplies for defrosting in the three
           cases were calculated, with the calculated relative standard errors listed in Table 3.3.2
           in Chapter 3. In this experimental study, the total energy used for defrosting was cal-
           culated at 781.8 kJ in Case 1, 753.2 kJ in Case 2, or 3.7% less, and 678.8 kJ in Case 3,
           or 13.2% less than that in Case 1, respectively. The main difference came from the
           thermal energy from the indoor air, with a difference of 92.3 kJ between Case 1
           and Case 3. However, the ratio of this part of the energy was kept at around
           83%–85%, without obvious changes with the energy supply decreasing.
              Defrosting efficiency can be used to evaluate the performance of a defrosting oper-
           ation. It is defined as the ratio of the actual amount of energy consumption required to
           both melt the accumulated frost and vaporize the retained melted frost to the total
           amount of energy available from an outdoor coil during an entire defrosting operation.
           In this section, the defrosting efficiencies were calculated at 45.0% in Case 1, 48.4%
           in Case 2, and 50.7% in Case 3, as shown in Table 6.7. The difference of defrosting
           efficiency between Case 1 and Case 3 was 5.7%.
              Moreover, Fig. 6.40 shows the defrosting durations and the durations of fin surface
           temperatures all reaching 24°C, the refrigerant volumetric flow rate reaching its peak
           value, and the temperature of the melted frost collected reaching its lowest value in the
           three cases, respectively. It could be found that the differences between Case 1 and
           Case 3 were 23 s for fin surface temperature all reaching 24°C, 22 s for defrosting
           duration, 22 s for the temperature of the melted frost collected reaching its lowest
           value, and 10 s for refrigerant volumetric flow rate reaching its peak value, from high
           to low. All the previous five parameters could demonstrate that the defrosting perfor-
           mance could be improved when an RCD operation starts at a higher FEC for an ASHP
           unit with a multicircuit outdoor coil.

            Table 6.7 Energy supply, energy consumption, and defrosting efficiency in three cases
            Item   Parameter                      Case 1  Case 2  Case 3   Unit

            1      The power input to compressor  120.6  112.2    114.8    kJ
            2      The power input to indoor air fan  7.4  6.8    2.5      kJ
            3      The energy from the indoor air  653.8  634.3   561.5    kJ
            4      The power input to outdoor air fan  0  0       0        kJ
            5      Total energy supply during defrosting  781.8  753.2  678.8  kJ
            6      Energy consumption on melting frost  334.0  351.4  323.6  kJ
            7      Energy consumption on vaporizing  18.1  15.9   20.5     kJ
                   the retained water
            8      Total energy consumption for   352.1  367.2    344.2    kJ
                   defrosting
            9      Defrosting efficiency          45.0%  48.8%    50.7%    –
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