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Methodology for the Evaluation of Natural Ventilation in ... - Cham

Methodology for the Evaluation of Natural Ventilation in ... - Cham

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There are several equations that have been developed to describe pressure difference due tow<strong>in</strong>d-driven flow. The equations below describe a case with a constant w<strong>in</strong>d speed creat<strong>in</strong>g asituation where w<strong>in</strong>d pressure does not fluctuate with time. However, <strong>for</strong> s<strong>in</strong>gle-sided ventilationfluctuations <strong>in</strong> w<strong>in</strong>d speed may be important. A diagram portray<strong>in</strong>g w<strong>in</strong>d-driven ventilation, <strong>the</strong>airflow direction and result<strong>in</strong>g pressure versus height is presented <strong>in</strong> Figure 8. If <strong>the</strong> open<strong>in</strong>gs onopposite sides are identical, <strong>the</strong> pressure differences across <strong>the</strong> open<strong>in</strong>gs are equal to half <strong>the</strong>pressure difference across <strong>the</strong> build<strong>in</strong>g when it is assumed that <strong>the</strong>re is negligible pressuredifferential through <strong>the</strong> <strong>in</strong>terior <strong>of</strong> <strong>the</strong> build<strong>in</strong>g. The Bernoulli equation applied between a po<strong>in</strong>tat some distance from <strong>the</strong> face <strong>of</strong> <strong>the</strong> build<strong>in</strong>g conta<strong>in</strong><strong>in</strong>g <strong>the</strong> w<strong>in</strong>dow and <strong>the</strong> façade <strong>the</strong>nreduces to <strong>the</strong> ideal equation:Pw2U POO O(2.10)2where P w is <strong>the</strong> pressure due to w<strong>in</strong>d at <strong>the</strong> façade and P O is <strong>the</strong> pressure away from <strong>the</strong> build<strong>in</strong>g,and U O is a reference velocity away from <strong>the</strong> build<strong>in</strong>g. Any height differential <strong>for</strong> flow along aparticular streaml<strong>in</strong>e is neglected, so both gz terms are zero, and <strong>the</strong> velocity at <strong>the</strong> face <strong>of</strong> <strong>the</strong>build<strong>in</strong>g is zero as it is <strong>the</strong> stagnation po<strong>in</strong>t. A pressure coefficient, c p , is used <strong>in</strong> <strong>the</strong> actual case,and is a function <strong>of</strong> w<strong>in</strong>d direction and location <strong>of</strong> <strong>the</strong> measurement on <strong>the</strong> build<strong>in</strong>g façade. Theresult<strong>in</strong>g equations are:2UPOw PO CPO2(2.11)CQ CPdAUO2(2.12)where Q is <strong>the</strong> flow enter<strong>in</strong>g or leav<strong>in</strong>g through <strong>the</strong> open<strong>in</strong>gs. The value <strong>of</strong> c p depends on <strong>the</strong>geometry <strong>of</strong> <strong>the</strong> build<strong>in</strong>g and <strong>the</strong> location on <strong>the</strong> façade, and values are <strong>of</strong>ten obta<strong>in</strong>ed through<strong>the</strong> use <strong>of</strong> w<strong>in</strong>d tunnel experiments (Orme 1999). The pressure on <strong>the</strong> exterior <strong>of</strong> <strong>the</strong> build<strong>in</strong>g <strong>in</strong>Figure 8 is assumed to not vary significantly with height.Figure 8. W<strong>in</strong>d Driven <strong>Ventilation</strong>: Airflow Direction and Pressure versus Height29

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