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Handbook of air conditioning and refrigeration / Shan K

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15.50 CHAPTER FIFTEEN<br />

Wet Part<br />

coil Twd, m, in °F (°C), is (Twb � Twl). Unit sensible cooling capacity <strong>of</strong> each ft2 (m2 1�2 ) outer surface<br />

area <strong>of</strong> the dry part <strong>of</strong> the water cooling coil, including the tube <strong>and</strong> fins, can then be calculated as<br />

Because U o can be calculated from Eq. (15.27), the total outer surface area <strong>of</strong> the dry part <strong>of</strong> the<br />

coil A o, d, in ft 2 (m 2 ) is<br />

(15.46)<br />

As for the DX coil, the cooling <strong>and</strong> dehumidifying capacity <strong>of</strong> the wet part <strong>of</strong> a dry-wet coil Q c, w,<br />

in Btu/h (W), can be calculated as<br />

(15.47)<br />

where h s, we � enthalpy <strong>of</strong> saturated <strong>air</strong> film at chilled water entering temperature,°F (°C). The effectiveness<br />

<strong>of</strong> the wet part <strong>of</strong> the dry-wet coil (wet, the number <strong>of</strong> transfer units (NTU), <strong>and</strong> the<br />

heat capacity rates C a <strong>and</strong> C w can be similarly calculated by Eqs. (15.39), (15.40), (15.36), <strong>and</strong><br />

(15.37), respectively.<br />

Dry-Wet Coil at Part-Load Operation<br />

Selection <strong>of</strong> a Dry-Wet Coil<br />

Q cs<br />

A o, d<br />

� U o(T ad, m � T wd, m)<br />

Ao, d �<br />

Uo (Tad, m � Twd, m)<br />

Q c, w �� wet60V˙ a� a(h ab � h s,we)<br />

When the dry-wet coil <strong>of</strong> a constant-volume system is at part-load operation, the reduction <strong>of</strong> the<br />

space cooling load results in a drop in space temperature. This causes the control system to modulate<br />

the two-way valve at the inlet <strong>of</strong> the water cooling coil to reduce the mass flow rate <strong>of</strong> chilled<br />

water flowing through the coil, as shown in Fig. 15.32. Because <strong>of</strong> the reduction <strong>of</strong> the chilled water<br />

flow rate, the following conditions occur:<br />

● The velocity <strong>of</strong> chilled water inside the coil tubes is reduced, <strong>and</strong> therefore the rate <strong>of</strong> heat-transfer<br />

between the <strong>air</strong> <strong>and</strong> water decreases.<br />

● Although the reduction <strong>of</strong> the space cooling load tends to lower the temperature <strong>of</strong> conditioned<br />

<strong>air</strong> leaving the coil T al, nonetheless T al increases because <strong>of</strong> the reduction <strong>of</strong> the chilled water flow<br />

rate <strong>and</strong> has a greater influence than the drop <strong>of</strong> the space cooling load.<br />

● From the psychrometric analysis shown in Fig. 15.32, the space <strong>conditioning</strong> line sp-rp at partload<br />

operation is shorter because <strong>of</strong> the reduction <strong>of</strong> space cooling load.<br />

● The chilled water flow rate is reduced so that the <strong>of</strong>f-coil temperature T ccp <strong>and</strong> supply temperature<br />

T sp match the reduction <strong>of</strong> space cooling load <strong>and</strong> maintain a space temperature T rp at part-load<br />

operation.<br />

● The higher dry-bulb <strong>and</strong> dew point temperatures <strong>of</strong> conditioned <strong>air</strong> leaving the coil cause an<br />

increase in space relative humidity � r. Sometimes, � r may be raised to 70 percent during partload<br />

operation. This is the main disadvantage in controlling space temperature by means <strong>of</strong><br />

chilled water flow rate modulation at part-load operation.<br />

The construction <strong>of</strong> a water cooling coil, a dry-wet coil, is similar to that <strong>of</strong> a DX coil, covered in<br />

Sec. 10.2. As for a DX coil, the procedure for selecting a water cooling coil according to the manufacturer’s<br />

data is as follows:<br />

Q cs

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