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Handbook of air conditioning and refrigeration / Shan K

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Stack Effect<br />

where � � <strong>air</strong> density, lb/ft 3 . For <strong>air</strong> density � � 0.075 lb/ft 3 , if the velocity pressure p v is<br />

expressed in in. WC <strong>and</strong> the <strong>air</strong> velocity in fpm or ft/min, according to Eq. (17.9),<br />

<strong>and</strong> v � 4005 √pv pv �� (17.10)<br />

v<br />

In SI units, if v is expressed in m/s <strong>and</strong> � in kg/m 3 , then p v is in Pa, <strong>and</strong> p v can be calculated by<br />

Eq. (17.9). For SI units, g c � 1.<br />

Total Pressure. At any cross-sectional plane perpendicular to the direction <strong>of</strong> the <strong>air</strong>flow, the total<br />

pressure <strong>of</strong> the <strong>air</strong>stream p t is defined as the sum <strong>of</strong> the static pressure p s <strong>and</strong> the velocity pressure<br />

p v, that is,<br />

pt � ps � pv pv � pt � ps (17.11)<br />

From Eq. (17.11) velocity pressure pv is also a kind <strong>of</strong> pressure difference. The units <strong>of</strong> pt must be<br />

consistent with ps <strong>and</strong> pv. In I-P units, it is also indicated in inches WC or WG <strong>and</strong> in SI units in Pa<br />

absolute (abs.) or gauge (g). Substituting Eq. (17.11) into Eq. (17.7), we see that<br />

(17.12)<br />

Equation (17.12) is another primary equation that relates the pressure loss from friction <strong>and</strong> other<br />

sources, �p f, <strong>and</strong> the total pressure p t1 <strong>and</strong> p t2 at two cross sections <strong>of</strong> the <strong>air</strong> duct system.<br />

When an <strong>air</strong> duct system has an elevation difference <strong>and</strong> the <strong>air</strong> temperature inside the <strong>air</strong> duct is<br />

different from the ambient <strong>air</strong> temperature, the stack effect exists. It affects <strong>air</strong>flow at different elevations.<br />

During a hot summer day, when the density <strong>of</strong> the outdoor <strong>air</strong> is less than the density <strong>of</strong> the<br />

cold supply <strong>air</strong> inside the <strong>air</strong> duct, the pressure exerted by the atmospheric <strong>air</strong> column between z 1<br />

<strong>and</strong> z 2, as shown in Fig. 17.1, is given as<br />

where � o � mean density <strong>of</strong> the ambient <strong>air</strong>, lb/ft 3 (kg/m 3 ). And the pressure exerted by the <strong>air</strong><br />

column inside the <strong>air</strong> duct between z 1 <strong>and</strong> z 2 is<br />

where � i � mean density <strong>of</strong> the supply <strong>air</strong> inside the <strong>air</strong> duct, in lb/ft 3 (kg/m 3 ). If the differences<br />

between the densities inside the <strong>air</strong> ducts, � 1 <strong>and</strong> � i, <strong>and</strong> � 2 <strong>and</strong> � i, are ignored, substituting these<br />

relationships into Eq. (17.6) yields<br />

<strong>and</strong><br />

� v<br />

60� 2<br />

� 5.192(2p vg c)<br />

p 1 � � 1v 1 2<br />

2g c<br />

�<br />

� 2gz 2 � � 1gz 1<br />

g c<br />

� g(� o � � i)(z 2 � z 1)<br />

g c<br />

p t1 � g(� o � � i)(z 2 � z 1)<br />

g c<br />

� 5.192 � 2 � 32.2 p v<br />

0.075<br />

p t1 � p t2 ��p f<br />

p at1 � p at2 � � o g(z 2 � z 1)<br />

g c<br />

� � i g(z 2 � z 1)<br />

g c<br />

AIR SYSTEMS: AIR DUCT DESIGN 17.5<br />

4005� 2<br />

� p 2 � � 2v 2 2<br />

2g c<br />

� p t2 ��p f<br />

� 4458p v<br />

��p f<br />

(17.13)<br />

(17.14)

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