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3.7. Evaporator - EVAP<br />

3.7 Evaporator - EVAP<br />

Figure 3.9: The evaporator has two sets <strong>of</strong> inlet <strong>and</strong> outlet: refrigerant (r,i <strong>and</strong> r,o) <strong>and</strong> chilled<br />

water (chill,i <strong>and</strong> chill,o).<br />

In the evaporator heat is transferred from an external circuit <strong>of</strong><br />

chilling water to the refrigerant. It is assumed that the refrigerant is in<br />

the two-phase region when it enters the evaporator. The refrigerant in<br />

the outlet can either be saturated gas or in the two-phase region.<br />

The closest approach temperature difference is defined as the temperature<br />

difference between the chilled water outlet <strong>and</strong> the refrigerant inlet,<br />

see figure 3.10.<br />

T [° C ]<br />

T chill , o<br />

T r ,i<br />

ΔT min ,r ,i<br />

T chill ,i<br />

T r ,o<br />

EVAP<br />

˙Q[kW ]<br />

Figure 3.10: Evaporator: The closest approach temperature difference is at the refrigerant inlet.<br />

∆T minr,i = T chill,o − T r,i (3.37)<br />

The effectiveness is determined by the chilled water because it has the<br />

lowest heat capacity flow; both media are water, but the refrigerant<br />

55

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