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

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Table 32. Conduction Heat Loss <strong>for</strong> S<strong>in</strong>gle Heated Zone Model <strong>for</strong> Various CasesHeat LossW/m 2Total Heat LossWAtrium HeatLossPercent Heat Lossthru Atrium7W<strong>in</strong>dow 1Stack 23.36 290.93 90.78 31.2%7W<strong>in</strong>dow 2Stack 14.66 182.65 80.18 43.9%7W<strong>in</strong>dow 3Stack 8.62 107.39 69.16 64.4%5 W<strong>in</strong>dow 1Stack 21.28 265.10 92.83 35.0%5 W<strong>in</strong>dow 2Stack 11.81 147.12 80.39 54.6%5 W<strong>in</strong>dow 3Stack 8.62 107.40 73.12 68.1%2 W<strong>in</strong>dow 1Stack 22.11 275.34 98.64 35.8%2 W<strong>in</strong>dow 2Stack 13.30 165.66 85.26 51.5%2 W<strong>in</strong>dow 3Stack 9.81 122.17 80.02 65.5%The heat loss due to conduction through <strong>the</strong> envelope had to be accounted <strong>for</strong> <strong>in</strong> <strong>the</strong> CFDsimulations, s<strong>in</strong>ce as much as 60 percent <strong>of</strong> <strong>the</strong> heat loss was due to conduction <strong>in</strong> <strong>the</strong> 7 w<strong>in</strong>dow,1 stack case. As it was determ<strong>in</strong>ed that most <strong>of</strong> <strong>the</strong> heat loss occurred <strong>in</strong> <strong>the</strong> atrium, <strong>the</strong> CFDmodel was modified to account <strong>for</strong> heat loss through <strong>the</strong> atrium walls as a negative heat flux. Byadjust<strong>in</strong>g <strong>the</strong> CFD model to account <strong>for</strong> <strong>the</strong> conduction issues found <strong>in</strong> <strong>the</strong> s<strong>in</strong>gle heated zonemodel, <strong>the</strong> result<strong>in</strong>g data <strong>for</strong> <strong>the</strong> numerical models were comparable to <strong>the</strong> experimental ones.Figure 48. Airflow Patterns <strong>for</strong> S<strong>in</strong>gle Heated Zone Case from Airflow Visualization <strong>in</strong> <strong>the</strong>Model: a) Lower W<strong>in</strong>dows, b) Upper W<strong>in</strong>dowsThe location <strong>of</strong> <strong>the</strong> w<strong>in</strong>dows <strong>in</strong>fluences <strong>the</strong> temperature distribution <strong>in</strong> <strong>the</strong> heated zone, as wasshown <strong>in</strong> <strong>the</strong> experimental and CFD models. The airflow, as measured by <strong>in</strong>let and outletvelocities, is not impacted significantly by <strong>the</strong> small height difference between <strong>the</strong> lower andupper w<strong>in</strong>dows. However, <strong>the</strong> total size <strong>of</strong> <strong>the</strong> <strong>in</strong>let and outlet open<strong>in</strong>gs does affect <strong>the</strong> <strong>in</strong>teriortemperature and airflow; restrictive open<strong>in</strong>gs caused a higher <strong>in</strong>ternal temperature, lead<strong>in</strong>g toreduced heat loss due to airflow and <strong>in</strong>creased heat loss due to conduction through <strong>the</strong> envelope.The heat loss modeled us<strong>in</strong>g PHOENICS (Figure 49) showed <strong>the</strong> impact <strong>of</strong> <strong>the</strong> prescribed heatloss at <strong>the</strong> atrium walls. The overall temperature was reduced by a scaled full build<strong>in</strong>gtemperature <strong>of</strong> approximately 0.5°C.124

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