23.12.2014 Views

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

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

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

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

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 />

Thrust per unit mass flow rate = V 2 – V 1 = (9.966+002) – (3.32e+002) = 6.644e+002 N Kg -1 s = 664.4 N Kg -1 s<br />

Fig 3.10: Pressure distribution in the proposed model (sectional view)<br />

Fig 3.11: Pressure distribution in the proposed model (side view)<br />

Pressure difference between the front and rear faces would result into form or pressure drag which is detrimental<br />

to the model.<br />

Approximate pressure difference =2.094e+004-(-2.4<strong>19</strong>e+005) Pa =2.513e+005 Pa<br />

4. Conclusion<br />

Just by bringing about certain changes in the design <strong>of</strong> the body and channelling the ambient air to pass through<br />

the body in a certain way it was possible to create an additional thrust to the body without affecting the fuel<br />

consumption. After the converging passage was introduced the pressure difference was utilized to make the air<br />

exit the converging passage at high velocity, which being coherent in nature also helped to straighten out the<br />

eddies that were being formed in the wake region. In rockets channelling ambient air from the front and sides<br />

will also increase the mass flow rate <strong>of</strong> the exhaust gases: If these designs <strong>of</strong> converging passages are<br />

introduced into the body <strong>of</strong> a rocket such that the passage would channel the ambient air into the exhaust <strong>of</strong> the<br />

rocket, from where all the exhaust gasses <strong>of</strong> rocket propulsion exit the rocket, not only it would create an<br />

additional thrust for the rocket (because <strong>of</strong> the increased kinetic energy) but it would also increase the mass flow<br />

rate <strong>of</strong> the exhaust gasses which would in turn further increase the thrust for the rocket according to impulse<br />

momentum theorem. The analysis has been performed on a general aerodynamic body, its practical<br />

implementation is still a difficult task because <strong>of</strong> the complex design problems related to the real bodies.<br />

Moreover, if a method is devised to vary the outlet cross-section with the help <strong>of</strong> PID controllers, thrust<br />

generation can be optimized for different speeds. It has been established by the above result that circular and<br />

rectangular section provides a higher maximum out velocity, however an elliptical cross-section provides a<br />

more coherent flow field. Structurally, a circular section is easy to carve out and most symmetrical thus must be<br />

preferred. The structure can have any cross-section suiting to the particular application.<br />

280

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!