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National Conference Emerging trends of Energy Conservation in

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3. Numerical simulation and validation<br />

The velocity pr<strong>of</strong>ile obta<strong>in</strong>ed by fluent was compared with the velocity pr<strong>of</strong>ile <strong>of</strong> the w<strong>in</strong>d<br />

tunnel experimental study as shown <strong>in</strong> Fig. 4. It is observed that by <strong>in</strong>corporat<strong>in</strong>g all the<br />

consideration and boundary condition the <strong>in</strong>let velocity pr<strong>of</strong>ile are very much similar as it<br />

was <strong>in</strong> the experimental study.<br />

Figure 4. comparison <strong>of</strong> velocity pr<strong>of</strong>iles <strong>of</strong> w<strong>in</strong>d tunnel experimental study and CFD<br />

simulation.<br />

Results obta<strong>in</strong>ed through CFD simulation are fairly good and compared with experimental<br />

results [8] and w<strong>in</strong>d standards available <strong>of</strong> different countries. Pressure coefficient for all<br />

four faces <strong>of</strong> isolated build<strong>in</strong>g (Setup-1) at 0° w<strong>in</strong>d <strong>in</strong>cidence angle (Fig. 5) is presented <strong>in</strong><br />

tabular form as given <strong>in</strong> Table 1.<br />

Table 1.Comparison <strong>of</strong> results obta<strong>in</strong>ed by CFD simulation with experimental results and<br />

w<strong>in</strong>d standards <strong>of</strong> different countries for all four faces <strong>of</strong> object build<strong>in</strong>g (Setup-1) at 0° w<strong>in</strong>d<br />

<strong>in</strong>cidence angle<br />

FACE<br />

CFD<br />

results<br />

W<strong>in</strong>d<br />

Tunnel<br />

Exp.<br />

Average Face Pressure Coefficient (Cp)<br />

BS 6399-<br />

2:1997<br />

7<br />

IS-875 Part-<br />

ASCE 7-02 AS/NZ 1170.2<br />

3<br />

Face A 0.906 0.83 0.85 0.80 0.80 0.95<br />

Face B -0.827 -0.84 -0.80 -0.70 -0.65 -0.70<br />

Face C -0.508 -0.71 -0.50 -0.50 -0.50 -1.25<br />

Face D -0.827 -0.85 -0.80 -0.70 -0.65 -0.70

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