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