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

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Figure 49. Comparison <strong>of</strong> S<strong>in</strong>gle Zone CFD Model without and with Heat Loss through AtriumWallsA CFD simulation was also created to evaluate <strong>the</strong> <strong>in</strong>fluence <strong>of</strong> <strong>the</strong> work<strong>in</strong>g fluid used on <strong>the</strong>result<strong>in</strong>g flow pattern. The s<strong>in</strong>gle zone case was used due to its simplicity and <strong>the</strong> ability tocalibrate <strong>the</strong> CFD model with exist<strong>in</strong>g data. Data were provided <strong>for</strong> a s<strong>in</strong>gle-zone, reduced-scalewater model <strong>of</strong> a similar configuration <strong>of</strong> a s<strong>in</strong>gle heated zone connected to an atrium. However,<strong>the</strong> reduced-scale water model was not geometrically similar to <strong>the</strong> reduced-scale air model.These data were used to validate a CFD model with <strong>the</strong> geometry <strong>of</strong> <strong>the</strong> orig<strong>in</strong>al water model,and <strong>the</strong>n <strong>the</strong> CFD model was modified to be geometrically similar to <strong>the</strong> reduced-scale airmodel. The ideal air model simulation was used, with no heat loss through <strong>the</strong> envelope. Theresult<strong>in</strong>g temperature distribution is provided <strong>in</strong> Figure 50. The temperatures have been scaledus<strong>in</strong>g <strong>the</strong> reference temperatures, so that <strong>the</strong>y are comparable. The <strong>in</strong>let jet at <strong>the</strong> w<strong>in</strong>dowdissipated quite differently <strong>for</strong> <strong>the</strong> two fluids. The jet <strong>in</strong> <strong>the</strong> air model spreads along <strong>the</strong> floor <strong>of</strong><strong>the</strong> heated zone, reach<strong>in</strong>g <strong>the</strong> far end <strong>of</strong> <strong>the</strong> atrium wall, while <strong>the</strong> <strong>in</strong>let jet <strong>in</strong> <strong>the</strong> water model justreaches <strong>the</strong> junction between <strong>the</strong> heated zone and <strong>the</strong> atrium. The temperature stratificationpatterns with<strong>in</strong> <strong>the</strong> heated space also differ with <strong>the</strong> work<strong>in</strong>g fluid used. The warm fluid <strong>in</strong> <strong>the</strong>heated space permeates lower <strong>in</strong>to <strong>the</strong> heated zone <strong>in</strong> <strong>the</strong> air model than <strong>in</strong> <strong>the</strong> water model, dueto <strong>the</strong> differences <strong>in</strong> <strong>the</strong>rmal properties <strong>of</strong> each fluid.125

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