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

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temperature <strong>of</strong> <strong>the</strong> air was <strong>the</strong> same as <strong>the</strong> temperature leav<strong>in</strong>g <strong>the</strong> south half <strong>of</strong> <strong>the</strong> model. Thisimplied that some <strong>of</strong> <strong>the</strong> air from <strong>the</strong> atrium entered <strong>the</strong> second floor and warmer air exited at <strong>the</strong>ceil<strong>in</strong>g level. The data presented are <strong>for</strong> <strong>the</strong> stacks open case, which expla<strong>in</strong>s why <strong>the</strong>re wassignificantly warmer air at <strong>the</strong> ceil<strong>in</strong>g measurement po<strong>in</strong>t. In <strong>the</strong> heated zone, <strong>the</strong> temperaturepattern was similar <strong>for</strong> all <strong>of</strong> <strong>the</strong> w<strong>in</strong>d speeds used (Figure 79). For each case, coolertemperatures were recorded at <strong>the</strong> mid-height <strong>of</strong> <strong>the</strong> heated zone. The actual temperaturecorresponded to <strong>the</strong> temperature <strong>of</strong> <strong>the</strong> exit<strong>in</strong>g air from <strong>the</strong> ground and first floor south zones.S<strong>in</strong>ce <strong>the</strong>re were no heat<strong>in</strong>g loads <strong>in</strong> <strong>the</strong> atrium space, <strong>the</strong> air exit<strong>in</strong>g <strong>the</strong> south zones was driven<strong>in</strong>to <strong>the</strong> two zones on <strong>the</strong> north half <strong>of</strong> <strong>the</strong> model by <strong>the</strong> w<strong>in</strong>d <strong>for</strong>ce. The air from <strong>the</strong> atriumspilled over <strong>the</strong> rail<strong>in</strong>g <strong>in</strong>to <strong>the</strong> heated zones on <strong>the</strong> north half <strong>of</strong> <strong>the</strong> build<strong>in</strong>g, while warmer airexited at <strong>the</strong> ceil<strong>in</strong>g level <strong>for</strong> both floors (Figure 69). Airflow visualization carried out <strong>for</strong>several different w<strong>in</strong>d speeds verified this explanation <strong>for</strong> <strong>the</strong> temperature variation <strong>in</strong> <strong>the</strong> heatedzone (Figure 70) as did <strong>the</strong> CFD simulations (Figure 71). In Figure 77 and Figure 79, <strong>the</strong> coolestair temperatures correspond to <strong>the</strong> exit<strong>in</strong>g air temperatures from <strong>the</strong> south half <strong>of</strong> <strong>the</strong> model,where <strong>the</strong> w<strong>in</strong>d-driven air is enter<strong>in</strong>g <strong>the</strong> model. However, <strong>the</strong> heat sources at <strong>the</strong> floor andsome amount <strong>of</strong> radiation to <strong>the</strong> ceil<strong>in</strong>g causes <strong>the</strong> <strong>the</strong>rmocouples near <strong>the</strong> floor and ceil<strong>in</strong>g torecord higher temperatures. Some <strong>of</strong> <strong>the</strong> cooler air enters <strong>in</strong>to <strong>the</strong> first floor north half <strong>of</strong> <strong>the</strong>model over <strong>the</strong> rail<strong>in</strong>g, caus<strong>in</strong>g cooler temperature measurements near <strong>the</strong> floor. There is someamount <strong>of</strong> jet flow, <strong>in</strong>troduc<strong>in</strong>g <strong>the</strong> cooler air at <strong>the</strong> mid-height <strong>of</strong> <strong>the</strong> space. These flow patternswere visible with <strong>the</strong> airflow visualization technique and also provided with <strong>the</strong> CFDsimulations.Figure 70. Airflow Patterns <strong>for</strong> Reduced-Scale Air Model with Stacks Open: Comb<strong>in</strong>ed W<strong>in</strong>d-Buoyancy Case144

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