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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 C2-A, November 9, 2009<br />

Conclusions<br />

In this paper, the performance of a dynamic model for absorption chillers has been<br />

investig<strong>at</strong>ed. General model functionality is demonstr<strong>at</strong>ed <strong>and</strong> the thermodynamics have<br />

been found to be consistent with reality. A sensitivity analysis has been performed on<br />

external <strong>and</strong> internal he<strong>at</strong> exchange rel<strong>at</strong>ed thermal mass. The analysis shows th<strong>at</strong> an<br />

increase in both external <strong>and</strong> internal thermal mass results in a slower response to the step<br />

change but also in smaller he<strong>at</strong> flow oscill<strong>at</strong>ions during the transient period. Also, the thermal<br />

mass has been found to influence the he<strong>at</strong> flow transients more significantly if alloc<strong>at</strong>ed<br />

internally. A time difference of 200s for reaching the steady st<strong>at</strong>e (response time) was<br />

observed between a complete internal <strong>and</strong> external alloc<strong>at</strong>ion of thermal mass.<br />

The transport delay in the solution cycle has been found to influence both the response time<br />

<strong>and</strong> the transients of the he<strong>at</strong> flow. A smaller transport delay leads to significantly faster<br />

response. Assuming half the value of the real transport delay in the absorption chiller leads<br />

to a 33% reduction of response time.<br />

The comparison with experimental d<strong>at</strong>a shows th<strong>at</strong> the dynamic agreement between<br />

experiment <strong>and</strong> simul<strong>at</strong>ion is very good with dynamic temper<strong>at</strong>ure devi<strong>at</strong>ions between 10<br />

<strong>and</strong> 25s. The total time to achieve a new steady-st<strong>at</strong>e after a 10K input temper<strong>at</strong>ure step<br />

amounts to approxim<strong>at</strong>ely 15 minutes for the experimental chiller. Compared to this, the<br />

present dynamic devi<strong>at</strong>ions of the model are in the magnitude of approxim<strong>at</strong>ely 1 to 3%.<br />

Steady-st<strong>at</strong>e results are being reproduced with temper<strong>at</strong>ure devi<strong>at</strong>ions between 0.7 <strong>and</strong> 3.5K<br />

in the model. Accuracy in this respect, however, was not the aim of the present study.<br />

The dynamic simul<strong>at</strong>ion model presented in this paper is a useful tool in the overall design<br />

process of absorption chillers. Technical changes in the construction of an existing<br />

absorption chiller model can be tested quickly <strong>and</strong> easily by incorpor<strong>at</strong>ing the design<br />

changes in the model. Also, new chiller designs can be tested on their performance without<br />

the need to build a prototype. The model also allows the identific<strong>at</strong>ion of transfer functions<br />

<strong>and</strong> control parameters of absorption chillers without the need to perform experiments. The<br />

model has been designed for the Phoenix 10kW chiller but can easily be adapted to other<br />

LiBr/w<strong>at</strong>er absorption chillers if the required design d<strong>at</strong>a of these chillers are available.<br />

page 91

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