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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 />

These regions are at the joint <strong>of</strong> the vane and the impeller hub and approximately at 1/3 length along the vane tip. It<br />

may also be noted that other areas <strong>of</strong> the vane, such as the vane face are relatively unaffected and thus do not<br />

fracture.<br />

This analysis is verified in dry run simulations where impeller vanes are known to break from the above two regions<br />

only<br />

Fig 6 displacement <strong>of</strong> vane with undisplaced position overlay<br />

Fig 6 indicates the relative displacement magnitude w.r.t the original position over the whole geometry. It is seen that<br />

the impeller vane first starts moving from one face because <strong>of</strong> unequal friction coefficients.<br />

Fig 7 indicates the stress distribution over the whole geometry. A higher stress at a point indicates a higher chance <strong>of</strong><br />

failure at that point. The .higher stress regions are indicated in red and yellow<br />

These regions are at the joint <strong>of</strong> the vane and the impeller hub, along the impeller face and approximately at 1/3<br />

length along the vane tip. A possible cause <strong>of</strong> this high stress may be the frictional forces as well torsion effect <strong>of</strong> the<br />

moment load from the motor.<br />

This analysis is verified in dry run simulations where impeller vanes are known to break from the above two regions<br />

only.<br />

310

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