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integration of solid oxide fuel cells and ... - Ea Energianalyse

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5. SIMULATION AND RESULTS<br />

Figure 5.12: A: Efficiencies <strong>and</strong> COP. B: The red <strong>and</strong> purple curves show the temperature before<br />

<strong>and</strong> after heat supply to the absorption unit. The brown curve shows how much heat the high<br />

temperature desorber receives, <strong>and</strong> the green curve shows how much heat DES1 receives (from<br />

COND2).<br />

Desorber 1<br />

The temperature <strong>of</strong> the low pressure desorber (DES1) is somewhat<br />

restricted by the temperature <strong>of</strong> the high pressure desorber (DES2).<br />

When T DES2 =150 ◦ C, T DES1 must be between 68 ◦ C <strong>and</strong> 88 ◦ C for the system<br />

to operate. From figure 5.13A it can be seen that the optimum <strong>of</strong> the blue<br />

COP curve is rather flat though, so the exact temperature is not so critical<br />

for the performance.<br />

In the st<strong>and</strong>ard configuration, the temperature <strong>of</strong> DES1 is not given<br />

explicitly since the system will not be able to run if e.g. T DES2 is altered<br />

too much while T DES1 remains constant. Instead the ratio <strong>of</strong> the mass<br />

flow rate <strong>of</strong> the refrigerant out <strong>of</strong> the desorber <strong>and</strong> the mass flow rate <strong>of</strong><br />

solution into the desorber is set equal for the two desorbers:<br />

ṁ 50<br />

ṁ 58<br />

= ṁ70<br />

ṁ 78<br />

(5.1)<br />

This is the same as saying that the difference between the strong<br />

<strong>and</strong> weak LiBr-solution is the same for two desorbers. And figure<br />

124

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