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Handbook of air conditioning and refrigeration / Shan K

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The fan power input on the fan shaft, <strong>of</strong>ten called the brake horsepower P f, can be calculated as<br />

(15. 6)<br />

When �p tf is expressed in Pa, fan volume flow rate in m 3 /s, fan total efficiency � t is the ratio <strong>of</strong> <strong>air</strong><br />

power P <strong>air</strong> to fan power input P f on the fan shaft, dimensionless, then constant C � 1, <strong>and</strong> fan<br />

power input P f is expressed in W. If �p tf is expressed in in. WC, fan volume flow rate is in cfm, fan<br />

total efficiency � t is a dimensionless ratio, then constant C � 6356 <strong>and</strong> fan power input on the shaft<br />

P is in hp.<br />

From Eq. (15.6), fan total efficiency can also be calculated as<br />

(15.7)<br />

Fan total efficiency is a combined index <strong>of</strong> aerodynamic, volumetric, <strong>and</strong> mechanical efficiencies <strong>of</strong><br />

a fan. Fan static efficiency � s is defined as the ratio <strong>of</strong> the product <strong>of</strong> the fan static pressure �p sf, in<br />

in. WC, <strong>and</strong> the fan volume flow rate to the fan power input, i.e.,<br />

Air Temperature Increase through Fan<br />

Fan Performance Curves<br />

AIR SYSTEMS: COMPONENTS—FANS, COILS, FILTERS, AND HUMIDIFIERS 15.5<br />

P f � �p tfV˙ f<br />

C� t<br />

� t � �p tf V˙ f<br />

� s � �p sf V˙ f<br />

(15.8)<br />

If <strong>air</strong> density � a � 0.075 lb/ft 3 , the specific heat <strong>of</strong> <strong>air</strong> c pa � 0.243 Btu/lb�°F, <strong>and</strong> 1 hp � 42.41<br />

Btu/min, the relationship between fan power input <strong>and</strong> the <strong>air</strong> temperature increase when it flows<br />

through the fan �T f, in °F, is given as<br />

Pf �<br />

Combining Eqs. (15.6) <strong>and</strong> (15.9), then, gives<br />

V˙<br />

f �acpa �Tf 42.41<br />

�Tf � 0.00667�ptf � 0.37�ptf � ac pa� t<br />

� �p tfV˙ f<br />

6356P f<br />

6356P f<br />

6356� t<br />

(15.9)<br />

(15.10)<br />

This <strong>air</strong> temperature rise in a fan when <strong>air</strong> flows through it is caused by the compression process<br />

<strong>and</strong> energy losses that occur inside the fan. When <strong>air</strong> flows through the <strong>air</strong> duct, duct fittings, <strong>and</strong><br />

equipment, the duct friction loss <strong>and</strong> dynamic losses cause a temperature increase as mechanical<br />

energy is converted to heat energy. However, this temperature increase in the <strong>air</strong> duct is <strong>of</strong>fset by a<br />

temperature drop caused by the expansion <strong>of</strong> <strong>air</strong> due to the reduction <strong>of</strong> static pressure along the<br />

<strong>air</strong>flow. Therefore, it is more convenient to assume that the <strong>air</strong> temperature rise occurs because <strong>of</strong><br />

the friction <strong>and</strong> dynamic losses along the <strong>air</strong>flow only when <strong>air</strong> is flowing through the fan.<br />

Fan characteristics can be described by certain interrelated parameters such as volume flow rate,<br />

pressure, power, <strong>and</strong> efficiency. These characteristics are depicted graphically by fan performance<br />

curves in Fig. 15.2.<br />

Fan characteristic curves usually set the volume flow rate , in cfm (m3 V˙<br />

/s), as the abscissa; <strong>and</strong><br />

fan total pressure �p tf, fan static pressure �p sf, fan power input P f, or fan total efficiency � t as the<br />

ordinate. In Fig. 15.2, there are three pressure-volume flow characteristic curves:<br />

� t

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