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university of florida thesis or dissertation formatting template

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since it is prop<strong>or</strong>tional to lift, and the upper surface <strong>of</strong> the airfoil is being examined. Local<br />

vertical displacement is chosen as the independent variable as opposed to angle <strong>of</strong> attack (AOA),<br />

<strong>or</strong> some other m<strong>or</strong>e typical aerodynamic parameter, due to the fact that as this w<strong>or</strong>k continues to<br />

m<strong>or</strong>e complex motions, i.e. vibration and flutter modes, comparison will be made in a<br />

straightf<strong>or</strong>ward manner with the same technique. A low-pass filter is applied to the data at 100Hz<br />

to filter out the noise due to turbulence effects. The left-hand side <strong>of</strong> Figure 6-7 and Figure 6-9<br />

c<strong>or</strong>responds to the LE <strong>of</strong> the wing, and the right-hand side c<strong>or</strong>responds to the TE <strong>of</strong> the wing.<br />

The top <strong>of</strong> the figures c<strong>or</strong>responds to the wingtip and the bottom to the root <strong>of</strong> the wing. The left-<br />

hand side <strong>of</strong> Figure 6-8 and Figure 6-10 c<strong>or</strong>responds to the same 2-D Lissajous plots seen in<br />

Figure 6-7 and Figure 6-9, and the right-hand side c<strong>or</strong>responds to the 3-D Lissajous plots with<br />

time being the third dimension. The red circle in all figures indicates the starting point <strong>of</strong> the<br />

cycle, and the black arrows indicate the direction <strong>of</strong> rotation.<br />

It can be seen in Figure 6-7 that there is a 90° (circle) phase shift over most <strong>of</strong> the wing.<br />

The direction <strong>of</strong> rotation on the f<strong>or</strong>ward p<strong>or</strong>tion <strong>of</strong> the wing is counter-clockwise and transitions<br />

to clockwise on the aft p<strong>or</strong>tion <strong>of</strong> the wing. Near this directional rotation change (and along the<br />

TE), regions on the wing resembling figure-eights and other “odd” shapes are observed. These<br />

do not indicate a harmonic that is n<strong>or</strong>mally associated with figure-eights but a continuous phase<br />

variation within 1 cycle. Since the solution is “cyclically steady”, solutions at 0° are identical to<br />

360° solutions, any time lag that shows up during a cycle has to be “made up” and that fall-<br />

behind and catch-up nature leads to the phase variation within a cycle that is shown here. This<br />

continuous phase variation within a single cycle also accounts f<strong>or</strong> the other “odd” shapes that are<br />

not simple ovals. There is also a significant amount <strong>of</strong> “noise” along the TE.<br />

75

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