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Experimental and Numerical Analysis of a PCM-Supported ...

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[58] evaluated the cooling tower air-side effectiveness ζ evap in terms <strong>of</strong> a saturation<br />

specific heat capacity C s :<br />

<br />

1<br />

exp NTU 1<br />

C<br />

<br />

<br />

r,<br />

evap<br />

<br />

evap<br />

<br />

(4.70)<br />

1<br />

Cr,<br />

evap<br />

exp <br />

NTU1<br />

Cr,<br />

evap<br />

<br />

where C r,evap is the gas to water heat capacity flow ratios;<br />

<br />

C m g C<br />

min<br />

s,<br />

evap<br />

Cr, evap<br />

<br />

(4.71)<br />

<br />

Cmax<br />

mhwc<br />

w<br />

Braun [58] linearized the air saturation enthalpy over the temperature, as depicted in<br />

figure (4.8) below, for analytical determination <strong>of</strong> the exit conditions from the cooling<br />

tower. Then, he estimated an average value <strong>of</strong> saturation specific heat C s as the<br />

average slope between the inlet <strong>and</strong> outlet water states;<br />

C<br />

<br />

h<br />

h<br />

<br />

s,<br />

w2<br />

s,<br />

w1<br />

s,<br />

evap<br />

(4.72)<br />

T<br />

w2<br />

Tw<br />

1<br />

where h s,w1 is the enthalpy <strong>of</strong> saturated air at exit water conditions.<br />

Figure (4.9) [Singham (56)] illustrates the effect <strong>of</strong> water film temperature on the<br />

enthalpy difference between the bulk air <strong>and</strong> saturated air at the interface along the<br />

axial direction <strong>of</strong> a counter flow cooling tower (h s -h g ). The air operating line begins at<br />

a point having an enthalpy (h g,in ) corresponding to the inlet wet bulb temperature<br />

T WB . The vertical distance between the two operating lines represents graphically the<br />

enthalpy difference (h s -h g ) (as in the integr<strong>and</strong> <strong>of</strong> equation (D.4) in Appendix D).<br />

According to the air-side effectiveness, ζ a definition, the maximum possible air-side<br />

heat transfer would occur when the vertical distance (h s -h g ) at the air exit approaches<br />

zero.<br />

4.5.3 Dehumidifier efficiency<br />

Since the humidifier <strong>and</strong> condenser are very similar, it is not surprising that the<br />

condenser effectiveness ζ cond can be defined in a fashion similar to its counterpart<br />

evaporative cooler. When the condenser is regarded as a parallel heat exchanger,<br />

its effectiveness can be expressed as:<br />

93

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