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Handbook of air conditioning and refrigeration / Shan K

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Fan Power<br />

Duct Heat Gain<br />

where T ae, T cc � temperature <strong>of</strong> entering <strong>air</strong> <strong>and</strong> conditioned <strong>air</strong> leaving coil, respectively, °F (°C).<br />

And the latent coil load Q cl, Btu/h (W), is<br />

Qcl � 60V˙<br />

s �s (wae � wcc)hfg, 32<br />

(6.45)<br />

where wae, wcc � humidity ratio <strong>of</strong> entering <strong>air</strong> <strong>and</strong> conditioned <strong>air</strong> leaving coil, respectively, lb/lb<br />

(kg/kg). Also,<br />

Qcc � Qcs � Qcl From Fig. 6.4, alternatively, the sensible cooling coil load can be calculated as<br />

(6.46)<br />

Qcs � Qrs � qs, s � qr, s � Qo, s<br />

(6.47)<br />

where qs, s, qr, s � supply <strong>and</strong> return system heat gain (as mentioned in preceding section, both are<br />

instantaneous cooling loads), Btu/h (W)<br />

Qo, s � sensible load from outdoor <strong>air</strong> intake, Btu/h (W)<br />

And the latent coil load can be calculated as<br />

Qcl � Qrl � Qo, l<br />

(6.48)<br />

where Qo, l � latent load from outdoor <strong>air</strong> intake, Btu/h (W). The supply system heat gain consists<br />

<strong>of</strong> mainly the supply fan power heat gain qsf <strong>and</strong> supply duct heat gain qsd; <strong>and</strong> the return system<br />

heat gain comprises the return fan power heat gain qrf, return duct heat gain qrd, <strong>and</strong> ceiling plenum<br />

heat gain qrp, all in Btu/h (W).<br />

In the <strong>air</strong> duct system, the temperature increase from the heat released to the <strong>air</strong>stream because <strong>of</strong><br />

frictional <strong>and</strong> dynamic losses is nearly compensated by the expansion <strong>of</strong> <strong>air</strong> from the pressure drop<br />

<strong>of</strong> the <strong>air</strong>stream. Therefore, it is usually assumed that there is no significant temperature increase<br />

from frictional <strong>and</strong> dynamic losses when <strong>air</strong> flows through an <strong>air</strong> duct system.<br />

Fan power input is almost entirely converted to heat energy within the fan. If the fan motor is<br />

located in the supply or return <strong>air</strong>stream, the temperature increase across the supply (or return fan)<br />

�T f, °F (°C), can be calculated as<br />

�T f � 0.37�p t<br />

� f� m<br />

where �p t � fan total pressure, in. WC<br />

� f,� m � total efficiency <strong>of</strong> fan <strong>and</strong> efficiency <strong>of</strong> motor<br />

LOAD CALCULATIONS 6.33<br />

(6.49)<br />

If the motor is located outside the <strong>air</strong>stream, then, in Eq. (6.49), � m � 1.<br />

The �p t <strong>of</strong> the return fan for a central hydronic <strong>air</strong> <strong>conditioning</strong> system in commercial buildings<br />

is usually 0.25 to 0.5 <strong>of</strong> the �p t <strong>of</strong> the supply fan. Therefore, the temperature increase <strong>of</strong> the return<br />

fan is far smaller than that <strong>of</strong> the supply fan. The temperature increase <strong>of</strong> the relief fan or exhaust<br />

fan affects only the relief or exhaust <strong>air</strong>stream. It is not a part <strong>of</strong> the supply <strong>and</strong> return system heat<br />

gain. A relief fan is used to relieve excess space pressure when 100 percent outdoor <strong>air</strong> is flowing<br />

through the supply fan for free cooling.<br />

Duct heat gain is the heat transfer caused by the temperature difference between the ambient <strong>air</strong> <strong>and</strong><br />

the <strong>air</strong> flowing inside the <strong>air</strong> duct. Duct heat gain is affected by this temperature difference, the

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