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OCTOBER 19-20, 2012 - YMCA University of Science & Technology

OCTOBER 19-20, 2012 - YMCA University of Science & Technology

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Proceedings <strong>of</strong> the National Conference on<br />

Trends and Advances in Mechanical Engineering,<br />

<strong>YMCA</strong> <strong>University</strong> <strong>of</strong> <strong>Science</strong> & <strong>Technology</strong>, Faridabad, Haryana, Oct <strong>19</strong>-<strong>20</strong>, <strong>20</strong>12<br />

Fig 3.4: Velocity distribution in the flow field (elliptical cross-section)-side view<br />

Fig 3.5: Velocity distribution in the flow field (elliptical cross-section)-rear view<br />

Fig 3.6: Velocity distribution in the flow field (rectangular cross section) - side view<br />

All three cross sections have the same inlet and outlet area. The inlet area being 817.2 square units and the<br />

outlet area being 426.2 square units. The velocity for the rectangular cross section comes out to be highest equal<br />

to 1.014* 10^3 m/s followed by circular and then elliptical. However, the velocity distribution for the<br />

rectangular and circular pr<strong>of</strong>ile is not uniform and velocity is highest only at the periphery. In contrast, the<br />

velocity distribution for the elliptical pr<strong>of</strong>ile is more uniformly distributed at the rear cross section. This can be<br />

attributed to the fact that the passage in case <strong>of</strong> elliptical section is more constricted than the other two for any<br />

cross section <strong>of</strong> the same area. Thus it can be easily imagined that the polyhedrons used to generate mesh in<br />

case <strong>of</strong> elliptical are more in number and finer than rectangular or circular which leads to a uniform velocity.<br />

278

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