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Phase II Final Report - NASA's Institute for Advanced Concepts

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Planetary Exploration Using Biomimetics<br />

An Entomopter <strong>for</strong> Flight on Mars<br />

0.165<br />

0<br />

Cm( acos( 0.75) , t)<br />

0.2<br />

− 0.235 0.4<br />

0 0.1 0.2<br />

0 t<br />

0.167<br />

Figure 3-122: Moment Coefficient vs. Time<br />

3.892<br />

5<br />

Cp( acos( 0.75) , t)<br />

0<br />

− 1.648<br />

5<br />

0 0.1 0.2<br />

0 t<br />

Figure 3-123: Power Coefficient vs. Time<br />

0.167<br />

3.3.3.9 Validation of Results<br />

Figure 3-124 gives the CFD results of the unblown case <strong>for</strong> the same baseline configuration.<br />

Although the curve depicts the total value of lift and thrust <strong>for</strong>ce as a function of time, if normalized,<br />

the C L values vary from approximately -2 to +4, which are bit higher than those obtained<br />

by the analytical model. This is because the leading edge vortex has not been modeled in the<br />

analytical model. Second, camber effects have been neglected, which will contribute to increase<br />

the lift coefficient value, but it can be deduced that the analytical model though approximate,<br />

gives the same shape of curve and the results are in the same range.<br />

140<br />

<strong>Phase</strong> <strong>II</strong> <strong>Final</strong> <strong>Report</strong>

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