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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 />

2. A dynamic simul<strong>at</strong>ion model for transient absorption chiller<br />

performance: Numerical results <strong>and</strong> experimental verific<strong>at</strong>ion<br />

This section describes the performance <strong>and</strong> experimental verific<strong>at</strong>ion of a dynamic<br />

absorption chiller model. In [1] the model itself was described with regard to dynamic effects,<br />

such as transport delays in the solution circuit, thermal storage <strong>and</strong> mass storage. In detail,<br />

the size of the solution sumps in absorber <strong>and</strong> gener<strong>at</strong>or, the time for the solution to flow<br />

from absorber to gener<strong>at</strong>or <strong>and</strong> vice-versa <strong>and</strong> the thermal mass of the main components<br />

has been accounted for. As a special fe<strong>at</strong>ure, the thermal mass of the components has been<br />

split into two parts, one which responds to the temper<strong>at</strong>ure of the external fluids, <strong>and</strong> the<br />

other which responds to the temper<strong>at</strong>ure of the solution <strong>and</strong> the refrigerant (internal fluids).<br />

These are the main parameters which determine the dynamic behaviour of the chiller.<br />

This second section is looking <strong>at</strong> internal consistency, sensitivity <strong>and</strong> accuracy of the model.<br />

Results of a performance analysis using ideal conditions to prove correct model behaviour<br />

are shown. A sensitivity analysis on thermal storage <strong>and</strong> solution transport delay has been<br />

performed to investig<strong>at</strong>e the influence of the dynamic parameters on the chiller performance.<br />

Finally, a model verific<strong>at</strong>ion using experimental results is also given in this paper.<br />

Nomencl<strong>at</strong>ure<br />

Symbols<br />

A area, (m 2 )<br />

A Duehring factor (deg C)<br />

B Duehring factor (-)<br />

c specific he<strong>at</strong> capacity (kJkg -1 K -1 )<br />

c number of simul<strong>at</strong>ion steps representing time constants for transport delay (-)<br />

D dew point temper<strong>at</strong>ure (deg C)<br />

g gravity constant (Nm 2 kg -2 )<br />

h<br />

height difference between gener<strong>at</strong>or outlet <strong>and</strong> absorber inlet (m)<br />

h enthalpy (kJkg -1)<br />

l specific he<strong>at</strong> of solution (kJkg -1 )<br />

m, m& mass flow r<strong>at</strong>e (kgs -1 )<br />

M<br />

p<br />

mass (kg)<br />

pressure (Pa)<br />

Q & ,Q<br />

he<strong>at</strong> flux (kW)<br />

r evapor<strong>at</strong>ion enthalpy (kJkg -1 )<br />

R gas constant for w<strong>at</strong>er vapour (Jkg -1 )<br />

T temper<strong>at</strong>ure (deg C)<br />

t<br />

time (s)<br />

UA he<strong>at</strong> transfer coefficient (kWK -1 )<br />

x Solution mass fraction (kg Salt kg -1 Sol )<br />

X mole r<strong>at</strong>io (-)<br />

z<br />

solution level in gener<strong>at</strong>or sump (m)<br />

page 79

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