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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 />

Cm = Coefficient of Moment<br />

Cp = Coefficient of Power Required.<br />

Table 3-8: List of Symbols (Continued)<br />

3.3.3.7 Model Formulation <strong>for</strong> Baseline Case<br />

It was assumed that the plan<strong>for</strong>m shape of the Entomopter wing is fixed in three dimensions and<br />

<strong>for</strong> parametric analysis, as we change the span of the wing, the chord length will vary all along<br />

the wing, so the shape of the plan<strong>for</strong>m is just defined by one parameter: span. Also it is assumed<br />

that the axis of rotation ("a") is constant. Hence, the total number of variables considered reduce<br />

to five: span, velocity, flapping frequency, flapping amplitude, and pitch amplitude. A cycle is<br />

defined as one complete upbeat and one downbeat, starting with h = 0 at t = 0, and then it moves<br />

(upwards) to -hamp at 1/4 time period, and then starts the down beat, continuing until the 3/4<br />

time period. In the final 1/4 time period, it comes back to the zero position. The angle of attack<br />

stays constant during the upbeat and downbeat and it flips during the 1/20th portion of time<br />

period at the extremes of the upbeat and down beat. A computer code was written in Mathcad<br />

2000 to evaluate these results. The values and equations used <strong>for</strong> baseline case are as follows:<br />

(NOTE: the notation used below ":=" means "defined as".)<br />

V:= 14 freq := 16 Plamp := 75 Pitamp := 8<br />

sspan<br />

span<br />

:=<br />

2<br />

a:= −0.25<br />

ω :=<br />

4⋅<br />

freq<br />

⋅ Plamp ⋅<br />

⎛<br />

⎜<br />

⎝<br />

π<br />

180<br />

hamp := sspan ⋅ sin Plamp ⋅<br />

αamp := Pitamp ⋅<br />

t :=<br />

0<br />

,<br />

100⋅<br />

freq<br />

π<br />

180<br />

1<br />

100⋅<br />

freq<br />

π<br />

180<br />

⎞<br />

⎠<br />

1<br />

..<br />

freq<br />

Since the instantaneous flapping height changes linearly, it was decided that different coefficients<br />

would be calculated <strong>for</strong> the first quarter cycle, then from 1/4 until 3/4 and finally <strong>for</strong> the<br />

last quarter of the cycle. This will give close to linear change effects. A similar approach was<br />

adopted <strong>for</strong> pitching motion coefficients and different coefficients were evaluated <strong>for</strong> flipping<br />

from positive to negative and vice versa. These coefficients were determined by solving a system<br />

of nonlinear simultaneous equations.<br />

( )<br />

h01 + h11 ⋅ cos φh1 0<br />

128<br />

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

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