IEA Solar Heating and Cooling Programm - NachhaltigWirtschaften.at
IEA Solar Heating and Cooling Programm - NachhaltigWirtschaften.at IEA Solar Heating and Cooling Programm - NachhaltigWirtschaften.at
IEA SHC Task 38 Solar Air Conditioning and Refrigeration Subtask A Report, Date:… 5.2 Analysis of Typical Days 25.06.2009 30 1200 25 1000 Temperature (T) [ °C ] 20 15 10 800 600 400 Irradiation (G) [ W/m² ] 5 200 0 00:00 02:00 04:00 06:00 08:00 10:00 12:00 14:00 16:00 18:00 20:00 22:00 00:00 0 T_ambient G_collector 25.06.2009 Temperature (T) [°C] 80 70 60 50 40 30 20 2400 2100 1800 1500 1200 900 600 Volume flow (V) [l/h] 10 300 0 00:00 02:00 04:00 06:00 08:00 10:00 12:00 14:00 16:00 18:00 20:00 22:00 00:00 0 T_collector_out T_drive V_collector Absorption chiller 1, 25.06.2009 80 16 COP [ % ]; Temperature (T) [ °C ] 70 60 50 40 30 20 10 0 00:00 02:00 04:00 06:00 08:00 10:00 12:00 14:00 16:00 18:00 20:00 22:00 00:00 14 12 10 8 6 4 2 0 Power (P) [ kW ] COP (20 min moav) T_hot_storage_top T_chilled_water T_drive P_chilling Figure 7: From the irradiation on the collector plane up to the cold production: Cooling with the absorption chiller 1 on June 25 th 2009. (Values based on one minute average; just the thermal COP is based on the moving average of 20 minutes for a better visibility.) Source: Fraunhofer ISE
IEA SHC Task 38 Solar Air Conditioning and Refrigeration Subtask A Report, Date:… Often it can be observed that the chillers run continuously for several hours thereby taking advantage of the big range in the driving temperature. Figure 7 shows an exemplary day with cooling operation of absorption chiller 1. In contrast to the relatively steady temperature in the upper part of the storage the driving temperature to the chiller oscillates periodically in a stronger manner. This oscillations correlate exactly with the collector outlet temperature and the periodical pump operation in the collector circuit (“bucket principle”). It is still not clear why the driving temperature is evened by the storage just on a small scale. The measuring point of the upper storage temperature shows clearly a temperature course which is more straightened. In contrast to the pump in the collector circuit the pump in the driving circuit of the chiller runs continuously from 9:00 until 17:00 with a short interruption before 12:00. Altogether with the low driving temperature chilling capacities between 6 and 8 kW are achieved. According to the temperature and capacity oscillations in the hot water circuit of the chiller the thermal COP varies strongly as well. 5.3 Detailed Analysis Figure 8 shows the frequency distribution of driving, cooling water and chilled water temperatures of both chillers in serial connection in 2010. The frequency maximum for the driving temperature of chiller 1 lies between 65°C and 70°C. Temperatures greater than 83°C appear rarely. Chiller 1 produces most frequen tly chilled water temperatures in the range of 13°C to 15°C. The chilled water range of c hiller 2 is widely distributed and on a higher temperature level as well. The driving temperature level of chiller 2 is shifted about 10 K downwards. The maxima of the cooling water temperatures are relatively clear. However, the values differ with 4 K from each other. The frequency distributions show just values when the pumps in the three circuits are in operation. Though, the first operation minutes after the chiller starts can for example show higher chilled water temperatures until a steady operation is reached. However, these values are not filtered out from the shown graphics. 1200 1000 Frequency 800 600 400 Intput Driving Heat AbCH1 Intput Driving Heat AbCH2 200 0 50 52 54 56 58 60 62 64 66 68 70 72 74 76 78 80 82 84 86 88 90 Temperature [°C]
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<strong>IEA</strong> SHC Task 38 <strong>Solar</strong> Air Conditioning <strong>and</strong> Refriger<strong>at</strong>ion<br />
Subtask A Report, D<strong>at</strong>e:…<br />
Often it can be observed th<strong>at</strong> the chillers run continuously for several hours thereby taking<br />
advantage of the big range in the driving temper<strong>at</strong>ure. Figure 7 shows an exemplary day with<br />
cooling oper<strong>at</strong>ion of absorption chiller 1. In contrast to the rel<strong>at</strong>ively steady temper<strong>at</strong>ure in<br />
the upper part of the storage the driving temper<strong>at</strong>ure to the chiller oscill<strong>at</strong>es periodically in a<br />
stronger manner. This oscill<strong>at</strong>ions correl<strong>at</strong>e exactly with the collector outlet temper<strong>at</strong>ure <strong>and</strong><br />
the periodical pump oper<strong>at</strong>ion in the collector circuit (“bucket principle”). It is still not clear<br />
why the driving temper<strong>at</strong>ure is evened by the storage just on a small scale. The measuring<br />
point of the upper storage temper<strong>at</strong>ure shows clearly a temper<strong>at</strong>ure course which is more<br />
straightened.<br />
In contrast to the pump in the collector circuit the pump in the driving circuit of the chiller runs<br />
continuously from 9:00 until 17:00 with a short interruption before 12:00. Altogether with the<br />
low driving temper<strong>at</strong>ure chilling capacities between 6 <strong>and</strong> 8 kW are achieved. According to<br />
the temper<strong>at</strong>ure <strong>and</strong> capacity oscill<strong>at</strong>ions in the hot w<strong>at</strong>er circuit of the chiller the thermal<br />
COP varies strongly as well.<br />
5.3 Detailed Analysis<br />
Figure 8 shows the frequency distribution of driving, cooling w<strong>at</strong>er <strong>and</strong> chilled w<strong>at</strong>er<br />
temper<strong>at</strong>ures of both chillers in serial connection in 2010. The frequency maximum for the<br />
driving temper<strong>at</strong>ure of chiller 1 lies between 65°C <strong>and</strong> 70°C. Temper<strong>at</strong>ures gre<strong>at</strong>er than<br />
83°C appear rarely. Chiller 1 produces most frequen tly chilled w<strong>at</strong>er temper<strong>at</strong>ures in the<br />
range of 13°C to 15°C. The chilled w<strong>at</strong>er range of c hiller 2 is widely distributed <strong>and</strong> on a<br />
higher temper<strong>at</strong>ure level as well. The driving temper<strong>at</strong>ure level of chiller 2 is shifted about<br />
10 K downwards. The maxima of the cooling w<strong>at</strong>er temper<strong>at</strong>ures are rel<strong>at</strong>ively clear.<br />
However, the values differ with 4 K from each other.<br />
The frequency distributions show just values when the pumps in the three circuits are in<br />
oper<strong>at</strong>ion. Though, the first oper<strong>at</strong>ion minutes after the chiller starts can for example show<br />
higher chilled w<strong>at</strong>er temper<strong>at</strong>ures until a steady oper<strong>at</strong>ion is reached. However, these values<br />
are not filtered out from the shown graphics.<br />
1200<br />
1000<br />
Frequency<br />
800<br />
600<br />
400<br />
Intput Driving<br />
He<strong>at</strong> AbCH1<br />
Intput Driving<br />
He<strong>at</strong> AbCH2<br />
200<br />
0<br />
50 52 54 56 58 60 62 64 66 68 70 72 74 76 78 80 82 84 86 88 90<br />
Temper<strong>at</strong>ure [°C]