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

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Chapter 3.0 Vehicle Design<br />

3.1 Wing Sizing<br />

Chapter 3.0 Vehicle Design<br />

3.1 Wing Sizing<br />

3.1.1 Engine Energy Production Requirements<br />

The energy consumed by the wing motion during each flap can be broken down into two main<br />

components: The energy needed to move the wing mass, acceleration and deceleration, at the<br />

desired flapping rate, and the energy needed to overcome the drag on the wing due to the lift produced<br />

during flapping. The energy due to motion is much greater than that due to lift generation.<br />

Initially, there<strong>for</strong>e, only the energy due to motion will be evaluated.<br />

3.1.2 Energy Required Due to Motion<br />

The energy required to move<br />

the mass of the wing can be<br />

easily calculated based on<br />

the geometry of the wing,<br />

mass distribution along the<br />

wing, and the flapping rate.<br />

These parameters, which<br />

include wing length, flapping<br />

frequency, and the<br />

angle through which the<br />

wing moves during the flap<br />

cycle, are shown in<br />

Figure 3-1. They can be varied<br />

to try to optimize wing<br />

design and operation. The<br />

optimization consists of<br />

maximizing lift while minimizing<br />

the power required.<br />

From the structural analysis<br />

the mass distribution along a<br />

wing section length was<br />

determined. Utilizing this<br />

Figure 3-1: Parameters <strong>for</strong> Power Consumption<br />

Optimization<br />

mass distribution. Loading on the wing due to its acceleration can be determined using the mass<br />

distribution. The mass distribution and corresponding loading are shown in Figure 3-2.<br />

The wing loading shown in Figure 3-2 is due to the acceleration of the wing mass; aerodynamics<br />

and other loads are not included at this point. The <strong>for</strong>ce (F) was based on Equation 3-1, where<br />

mi is the mass of an incremental piece of the wing corresponding to a mean radial distance of ri,<br />

q is the angle through which the wing will move during the acceleration (this is equal to the<br />

maximum deflection angle used during the structural analysis), and f is the flapping frequency in<br />

cycles per second. Wing acceleration was assumed to be a constant from the beginning of the<br />

stroke where the wing is in its full upward position to the wing in a horizontal position. The<br />

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