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IEA Solar Heating and Cooling Programm - NachhaltigWirtschaften.at

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<strong>IEA</strong> SHC Task 38 <strong>Solar</strong> Air Conditioning <strong>and</strong> Refriger<strong>at</strong>ion Subtask C1 Report, 31 October 2010<br />

The he<strong>at</strong> r<strong>at</strong>io <strong>and</strong> the COP thermal for the various applic<strong>at</strong>ions of an absorption refriger<strong>at</strong>ion<br />

process depend on the kind of working fluid <strong>and</strong> the applic<strong>at</strong>ion of the process.<br />

2.2.3.2 Design of an absorption refriger<strong>at</strong>ion process<br />

The design of an absorption process will be demonstr<strong>at</strong>ed for the working fluid pair ammonia<br />

as refrigerant <strong>and</strong> w<strong>at</strong>er as the absorbent. The thermodynamic properties for the ammonia<br />

w<strong>at</strong>er mixture are well known. The tool for process configur<strong>at</strong>ion is the lgp,1/T-diagram for<br />

the basic process definition <strong>and</strong> the table of Merkel-Bosnjakovic for process design <strong>at</strong> a<br />

higher accuracy. A basic process definition is shown with the help of the lgp,1/T-diagram in<br />

Figure 5.<br />

Figure 5: Basic design of a single stage, continuous absorption refriger<strong>at</strong>ion process in the<br />

lgp,1/T-diagram for working fluids with positive he<strong>at</strong> of the chemical reaction.<br />

The following items have to be determined for the basic design of a refriger<strong>at</strong>ion process:<br />

- Working pair (NH3/H2O; H2O/LiBr)<br />

- Evapor<strong>at</strong>ion temper<strong>at</strong>ure (To)<br />

- Temper<strong>at</strong>ure of cooling w<strong>at</strong>er (he<strong>at</strong> rejected <strong>at</strong> Ta,Tc)<br />

The process starts in Figure 5 <strong>at</strong> point 4. The working fluid, an ammonia/w<strong>at</strong>er mixture, is<br />

pumped out of the absorber (30 … 40°C) <strong>at</strong> a pressure of about 3 to 4 bars to a pressure of<br />

10 to 13 bars into the gener<strong>at</strong>or with the temper<strong>at</strong>ure T g,in . In the gener<strong>at</strong>or the temper<strong>at</strong>ure<br />

rises to T g,st <strong>and</strong> the working fluid starts boiling. The refrigerant (NH3) is separ<strong>at</strong>ed from the<br />

working fluid by boiling from point 1 (T g,st ) to 6 (T g,e ). At point 6 the WF boils <strong>at</strong> the highest<br />

temper<strong>at</strong>ure T g,e <strong>and</strong> the concentr<strong>at</strong>ion reaches ξ w . With the help of a pressure reduction<br />

valve (WFCV) the working fluid leaves the gener<strong>at</strong>or <strong>at</strong> point 6 <strong>and</strong> is reduced to the low<br />

pressure stage <strong>at</strong> point 5. On its way from 5 to 4 the weak WF absorbs the refrigerant, which<br />

comes from the evapor<strong>at</strong>or 3 in the absorber 4. The absorber has to be cooled continuously.<br />

The refrigerant (NH3) is separ<strong>at</strong>ed from the working fluid in the gener<strong>at</strong>or between point 1<br />

<strong>and</strong> 6, <strong>and</strong> is condensed in the condenser (point 2) on cooled surfaces <strong>at</strong> the high pressure<br />

stage. After condensing, a pressure reduction valve reduces the pressure of the liquid<br />

refrigerant before entering the evapor<strong>at</strong>or <strong>at</strong> 3. The refrigerant receives he<strong>at</strong> <strong>at</strong> the low<br />

temper<strong>at</strong>ure (+5 … -30 °C) in the evapor<strong>at</strong>or 2 <strong>and</strong> can now boil <strong>and</strong> evapor<strong>at</strong>e <strong>at</strong> low<br />

temper<strong>at</strong>ure. The vapour of the refrigerant enters the absorber <strong>at</strong> point 4 <strong>and</strong> meets the weak<br />

working fluid. Further inform<strong>at</strong>ion on th<strong>at</strong> m<strong>at</strong>ter is offered in Niebergall [2] <strong>and</strong> Bogard [3].<br />

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