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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 />

A int<br />

G int<br />

C<br />

= m&<br />

, int v,<br />

G<br />

⋅<br />

( pc)<br />

p,<br />

v<br />

( r + c ⋅ ( T − T<br />

)<br />

Q & (7)<br />

( r<br />

pc<br />

l<br />

pc<br />

c<br />

p w<br />

( TG<br />

TA<br />

)) Q&<br />

( )<br />

+<br />

( )<br />

+ ⋅ −<br />

SHX<br />

= mv,<br />

G<br />

⋅<br />

,<br />

G<br />

Q & &<br />

+<br />

, (8)<br />

( r<br />

pc<br />

l<br />

pc<br />

c<br />

p v<br />

( TG<br />

TE<br />

) c<br />

p w<br />

( TG<br />

TA<br />

) Q&<br />

( )<br />

+<br />

( )<br />

−<br />

,<br />

⋅ − + ⋅ −<br />

SHX<br />

Q & &<br />

+<br />

, (9)<br />

= mv,<br />

A<br />

⋅<br />

,<br />

C<br />

The solution he<strong>at</strong> exchanger does not exchange the maximum possible he<strong>at</strong> between its two<br />

flows. The difference between actual <strong>and</strong> ideal he<strong>at</strong> transfer can be assumed as a parasitic<br />

he<strong>at</strong> flow which has to be added to the gener<strong>at</strong>or <strong>and</strong> has to be removed <strong>at</strong> the absorber. For<br />

a constant he<strong>at</strong> exchanger effectiveness<br />

η<br />

SHX<br />

it can be calcul<strong>at</strong>ed as<br />

Q&<br />

SHX<br />

( 1 −η<br />

) ⋅ m&<br />

⋅ c ⋅ ( T − T )<br />

=<br />

SHX sol,<br />

sG p,<br />

sol,<br />

s<br />

G<br />

A<br />

.<br />

(10)<br />

In equ<strong>at</strong>ion (10),<br />

& is the mass flow r<strong>at</strong>e of the strong solution from gener<strong>at</strong>or to<br />

m<br />

sol , sG<br />

absorber [4].<br />

The dynamic performance of the absorption chiller is influenced by various time-dependent<br />

effects, caused by complex he<strong>at</strong> transfer phenomena in the internal <strong>and</strong> external he<strong>at</strong><br />

exchangers. In order to keep the model simple, not all of the dynamic effects have been<br />

taken into account. Only the three effects with the estim<strong>at</strong>ed biggest influence on chiller<br />

performance have been chosen. These include a time delay in the solution transport<br />

between gener<strong>at</strong>or <strong>and</strong> absorber, mass storage in the vessel sumps, <strong>and</strong> thermal storage in<br />

the external <strong>and</strong> internal he<strong>at</strong> exchangers. These dynamic terms are the backbone of the<br />

model <strong>and</strong> will be discussed in detail.<br />

Dynamic Modelling<br />

Both gener<strong>at</strong>or <strong>and</strong> absorber vessel have been modelled as a serial connection of a tube<br />

bundle he<strong>at</strong> exchanger <strong>and</strong> a solution sump. The tube bundle is the active part; the sump is<br />

a storage <strong>and</strong> mixing device. Solution can accumul<strong>at</strong>e in absorber <strong>and</strong> gener<strong>at</strong>or sump<br />

according to the actual load, however there is also some solution which is always stored on<br />

the tube bundle. This hold-up, usually, is small as compared to the amount of liquid in the<br />

sump because the film is less than half a millimetre thick. Moreover, the bundle should be<br />

wetted all the time with the consequence th<strong>at</strong> the amount of liquid on the bundle will not<br />

change significantly. Therefore the amount of liquid on the bundle is neglected.<br />

Due to the storage effect, we have to distinguish between the solution flow entering the<br />

vessel, the one leaving the bundle <strong>and</strong> entering the sump, <strong>and</strong> the one leaving the sump.<br />

Moreover, we have to consider different concentr<strong>at</strong>ions <strong>at</strong> the inlet of the bundle, <strong>at</strong> the exit<br />

page 66

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