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

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3. COMPONENT DESCRIPTION<br />

T [° C ]<br />

T h , i<br />

T h , o<br />

ΔT min ,r ,o<br />

T ss , o<br />

T r ,o<br />

T ws ,i<br />

˙Q[kW ]<br />

Figure 3.8: Desorber: The solution/gas temperature is assumed to be constant throughout the<br />

desorber. So the closest approach temperature difference will be between the heating water outlet<br />

<strong>and</strong> the common solution temperature.<br />

heat capacity flow:<br />

ɛ = T h,i − T h,o<br />

T h,i − T ss,o<br />

(3.30)<br />

The amount <strong>of</strong> heat to be added by the heating circuit is calculated by<br />

the energy balance, which includes a loss to the surroundings ( ˙Q loss ),<br />

which should be zero (adiabatic component) or positive (heat loss to the<br />

surroundings).<br />

Ḣ ws,i + Ḣ h,i = Ḣ r,o + Ḣ ss,o + Ḣ h,o + ˙Q loss (3.31)<br />

A mass balance is made for H 2 O as well as LiBr (total inlet = total outlet):<br />

ṁ r,o + ṁ ss,o = ṁ ws,i (3.32)<br />

ṁ ss,o · w ss,o = ṁ ws,i · w ws,i (3.33)<br />

were w is the concentration <strong>of</strong> LiBr in the solution. The pressure losses<br />

(given as a negative pressure increases) are defined as three different ∆P<br />

parameters:<br />

p r,o = p ws,i + ∆p r (3.34)<br />

p ss,o = p ws,i + ∆p ss (3.35)<br />

p h,o = p h,i + ∆p h (3.36)<br />

54

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