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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 />

Figure 3-78: Lift Coefficient <strong>for</strong> the Oscillating Wing Case<br />

Figure 3-79: Drag Coefficient <strong>for</strong> the Oscillating Wing Case<br />

3.3.1.4.2.2 Thin 3D Wing Geometry<br />

To further investigate the low Reynolds number high-α behavior, a thin 3D wing was modeled<br />

after the North American cicada wing (Figure 3-80). The plan<strong>for</strong>m was approximated as a semiellipse<br />

with an aspect ratio of 3. Even though the cicada has hind wings (the right one is shown<br />

in Figure 3-80), the CFD model used only the <strong>for</strong>ewing. The wing is thin (thickness-to-maximum<br />

chord ratio ~ 0.02), has a slight camber, and a slight curvature in the span wise direction.<br />

The hind wing can rotate about the leading edge, which <strong>for</strong>ms a common line of contact with the<br />

<strong>for</strong>ewing trailing edge. It appears that one of the functions of the hind wing is to act as a control<br />

surface to control camber during the stroke cycle. As discussed by Dickinson, et al. [57, 58, 56],<br />

the wing undergoes large changes in orientation during pronation and supination in order to provided<br />

optimum lift and thrust during the entire stroke cycle. The other interesting feature to note<br />

96<br />

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

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