This page contains a Flash digital edition of a book.
of approximately 5.0. This is an ideal efficiency – it can be approached, but never achieved because of losses in the refrigeration cycle. If the temperature source reduces further below


0C, the COP reduces further, by roughly 3% per each 1C reduction in heat source temperature in line with the principle quoted earlier. The decrease in efficiency for an air-source heat pump is actually worse at these air temperatures. This is because as the receiving coil temperature reduces below 0C, ice forms on the coil from water in the air, preventing thermal transfer to the refrigerant. This then requires a reversal in the cycle or an electric heater to defrost using more energy, and further reducing efficiency and therefore moving away from the simple 3% principle quoted. This is a particular problem in the UK, which is a maritime climate, where the relative humidity of the air is close to saturation and water, and therefore ice can form with relative small changes in temperature. Together, these effects can reduce actual air-source


COPs substantially. In some cases, equipment at these higher temperatures operates at actual COPs of 2 to 2.5. This means we are not even approaching the lines shown in Figure 1. An engineer can manage this by moving to a source


www.cibsejournal.com


with a more constant temperature: the ground, or possibly a water supply (sea/lake/river). This is why these systems tend to have a higher COP in comparison with air systems. However, there is also a greater capital cost for the ground loop. To achieve the best heat pump efficiencies, a hybrid


heat pump system is required. This draws energy from the ground in winter and from the air in the summer, switching systems from the higher temperature source as the season changes to minimise the temperature difference and maximise efficiency. These systems also provide an opportunity for ground temperatures to recover over the summer season.


Combined heat and power Professor MacKay uses a graph (see Figure 2) to show that current combined cycle gas turbine generation with heat pumps operating at COPs of 3 and 4 are better than CHP. In this graph, CHP is better than a heat pump if the CHP points are to the right of the green line which represents the heat pump efficiency. MacKay states: ‘The main thing to notice in this


diagram is that the electrical efficiencies of the CHP systems are significantly smaller than the 49% efficiency delivered by single-minded electricity-only >


August 2010 CIBSE Journal 35


A heat pump increases the efficiency of electrical heating by transferring heat from one source to another using a refrigerant cycle


Simon Weir www.simonweir.com


Page 1  |  Page 2  |  Page 3  |  Page 4  |  Page 5  |  Page 6  |  Page 7  |  Page 8  |  Page 9  |  Page 10  |  Page 11  |  Page 12  |  Page 13  |  Page 14  |  Page 15  |  Page 16  |  Page 17  |  Page 18  |  Page 19  |  Page 20  |  Page 21  |  Page 22  |  Page 23  |  Page 24  |  Page 25  |  Page 26  |  Page 27  |  Page 28  |  Page 29  |  Page 30  |  Page 31  |  Page 32  |  Page 33  |  Page 34  |  Page 35  |  Page 36  |  Page 37  |  Page 38  |  Page 39  |  Page 40  |  Page 41  |  Page 42  |  Page 43  |  Page 44  |  Page 45  |  Page 46  |  Page 47  |  Page 48  |  Page 49  |  Page 50  |  Page 51  |  Page 52  |  Page 53  |  Page 54  |  Page 55  |  Page 56  |  Page 57  |  Page 58  |  Page 59  |  Page 60  |  Page 61  |  Page 62  |  Page 63  |  Page 64  |  Page 65  |  Page 66  |  Page 67  |  Page 68
Produced with Yudu - www.yudu.com