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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 />

.<br />

Figure 3-115: LEV Formation (View 1) Figure 3-116: LEV Formation (View 2)<br />

The wake de<strong>for</strong>mations also play a major role in thrust characteristics of the vehicle at these low<br />

Reynolds numbers. Many researchers have tried to visualize the flow patterns of these wakes<br />

and have suggested that these tend to augment the thrust tremendously. These unsteady wakes<br />

also cannot be modeled using the conventional fixed wing aerodynamics.<br />

Another approach is to model flapping wing as a propeller as suggested by Theodore Theoderson<br />

[255]. Azuma [12] has also used this approach to predict flapping wing per<strong>for</strong>mance. Rotorcraft<br />

aerodynamics has different approaches <strong>for</strong> computation of <strong>for</strong>ces, which are as follows:<br />

3.3.3.2.4 Momentum Theory<br />

This is a very basic back-of-the-envelope type calculation approach which considers the propeller<br />

or rotor as a rotating disc and then computes <strong>for</strong>ces based on mass and momentum conservation.<br />

This cannot be used as <strong>for</strong> case of flapping because the wing is not covering the entire 360 o<br />

or 2π radians, and also direction of rotation is changing twice within each cycle during the<br />

upbeat and downbeat.<br />

3.3.3.2.5 Blade Element Theory<br />

This approach divides each propeller blade into different equal-length small strips/segments and<br />

then each strip/segment is analyzed separately taking into account the incoming flow velocity as<br />

well as angular velocity. The <strong>for</strong>ces on the entire blade are then computed by summation of<br />

<strong>for</strong>ces on all the segments. This approach considers the effective angle of attack at different segments,<br />

but still assumes a uni<strong>for</strong>m inflow. This model has been modified to account <strong>for</strong> the non<br />

uni<strong>for</strong>m flow by blade element momentum theory. Still these models do not consider the leading<br />

122<br />

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

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