Aerodynamics and Design for Ultra-Low Reynolds Number Flight
Aerodynamics and Design for Ultra-Low Reynolds Number Flight
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)