Page 201 - Defrosting for Air Source Heat Pump
P. 201

The influence of refrigerant distribution on defrosting           195

           vary the refrigerant flow to each circuit, according to the tube surface temperature at
           the exit of each circuit.
              Experimental work was then carried out at two experimental cases, as listed in
           Table 7.1, so that the system performances under different refrigerant distribution
           evenness values (RDEVs) can be comparatively and quantitatively analyzed. In this
           study, to easily distinguish the two experimental cases, similar with the FEC, the
           RDEV was defined as the ratio of the minimum refrigerant distribution into three cir-
           cuits to the maximum one. In Case 1, all the stop valves on the three circuits were fully
           open; therefore, the opening degrees of each stop valve were kept constant. Refriger-
           ant was kept at a fixed RDEV, lower than 100%, due to gravity and tube internal resis-
           tance. In Case 2, a series of trial-and-error manual adjustments of the opening degree
           of the stop valves was carried out to realize how to adjust the refrigerant flow into each
           circuit evenly, according to the tube surface temperature at the exit of each circuit.
           Finally, at the start of the defrosting experiment, a suite of suitable degrees was
           obtained and fixed for the three circuits. The refrigerant could be fixed at an RDEV
           around 100%.
              Figs. 7.1 and 7.2 show the measured tube surface temperatures at the exits of the
           three refrigerant circuits on defrosting mode without any frost accumulated on the sur-
           face of the outdoor coil in two cases. As shown in Fig. 7.1, when three stop valves were
           fully open in Case 1, the temperatures of the three circuits were always different from
           each other, from 0 to 110 s into the defrosting operation. It is demonstrated that the
           tube surface temperature of Circuit 1 was the highest, and that of Circuit 2 the lowest.
           This phenomenon suggests that the amount of refrigerant flowing into Circuit 1 was
           the highest due to the smallest circuit internal resistance, and that flowing into Circuit
           2 was the least due to the biggest circuit internal resistance. In addition, it is clearly


            Table 7.1 Results of two experimental cases

            Item   Parameter             Case 1              Case 2
            1      Stop valves state     Fully open          Evenly adjusted
            2      RDEV                  <100%               ¼100%
            3      Trays during frosting  Without            Without
            4      Trays during defrosting  With             With
            5      Melted frost from     325 g               311 g
                   Circuit 1
            6      Melted frost from     322 g               324 g
                   Circuit 2
            7      Melted frost from     302 g               309 g
                   Circuit 3
            8      Total melted frost    949 g               944 g
                   collected
            9      FEC                   92.9%               95.4%
            10     Defrosting duration   185 s               172 s
            11     Results shown in      Figs. 7.1, 7.3, 7.5, 7.7,  Figs. 7.2, 7.3, 7.6, 7.8,
                                         7.9                 7.9
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