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Aerodynamics and Design for Ultra-Low Reynolds Number Flight

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Chapter 6<br />

116<br />

Incidence (deg.)<br />

20<br />

16<br />

0<br />

12<br />

8<br />

4<br />

FIGURE 6.20 Comparison of laser scanning incidence data <strong>and</strong> quadratic fit with error bounds<br />

<strong>for</strong> one blade of the Sample-1 four-blade 2.5cm rotor.<br />

The incidence distributions <strong>for</strong> the Sample-1, Sample-2, <strong>and</strong> Sample-3 rotors based on<br />

quadratic fitting of the scan data are shown in Figures 6.21, 6.22 <strong>and</strong> 6.23. The cause of<br />

these variations is not clear at this time. The SDM process results in the correct<br />

geometry prior to the part being removed from the substrate, so the de<strong>for</strong>mation must<br />

occur either during the extraction of the finished part or after production due to material<br />

aging or environmental factors. This is one area <strong>for</strong> further study, but is outside the focus<br />

of this work.<br />

0 2 4 6 8 10 12 14<br />

r (mm)<br />

Knowledge of the as-tested rotor geometries does permit further insight into some of the<br />

variations seen in the thrust <strong>and</strong> power required data presented earlier <strong>for</strong> rotors that are<br />

ostensibly the same design. The rotor per<strong>for</strong>mance with dissimilar blades is difficult to<br />

estimate quantitatively, the rapid analysis method assumes identical blades, as does the<br />

current OVERFLOW-D calculations using a periodic domain, but reasonable qualitative<br />

arguments can be made using this in<strong>for</strong>mation.<br />

Scanning Data<br />

Quadratic Fit<br />

Fit +/- Atan(t/c)

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