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university of florida thesis or dissertation formatting template

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Figure 6-3 and Figure 6-4 illustrate a sequence <strong>of</strong> images visualizing the flow computed on<br />

the left wing (looking aft f<strong>or</strong>ward) f<strong>or</strong> the sinusoidal rolling motion depicting Mach = 1<br />

boundary and instantaneous v<strong>or</strong>ticity magnitude iso-surfaces, respectively, with the pressure<br />

col<strong>or</strong>ing the aircraft surface. The roll angle is shown as a function <strong>of</strong> time in the lower right-hand<br />

c<strong>or</strong>ner in each set <strong>of</strong> images. The left set <strong>of</strong> images, A) and B), display the 1Hz ±2° case results,<br />

and the 8Hz ±0.5° case results are presented in C) and D) on the right. Looking at Figure 6-3, it<br />

is difficult to see a difference in the Mach=1 iso-surface as the aircraft rolls. Upon animation, it<br />

maintains a fairly constant size f<strong>or</strong> the 1Hz ±2° case and appears to grow in size at the top <strong>of</strong> the<br />

roll oscillation f<strong>or</strong> the 8Hz ±0.5° case. The growth <strong>of</strong> this iso-surface f<strong>or</strong> the 8Hz ±0.5° case<br />

appears to lag behind the rolling motion <strong>of</strong> the aircraft, which is indicative <strong>of</strong> a phase<br />

shift/hysteresis in the flow. This iso-surface also maintains a mostly constant position on the aft<br />

p<strong>or</strong>tion <strong>of</strong> the wing, parallel to the TE. As the aircraft rolls left-wing-down, the Mach=1 iso-<br />

surface begins to wrap around the wingtip at the LE to the bottom surface <strong>of</strong> the wing.<br />

Figure 6-4 displays evidence <strong>of</strong> the v<strong>or</strong>tices coming <strong>of</strong>f <strong>of</strong> the strake in the cave-like<br />

feature on the inboard p<strong>or</strong>tion <strong>of</strong> the wing f<strong>or</strong> both cases. These v<strong>or</strong>tices remain stationary<br />

despite the motion <strong>of</strong> the aircraft when animated. Indication <strong>of</strong> the wing tip v<strong>or</strong>tices<br />

strengthening can be seen at the peak <strong>of</strong> the rolling cycle, and diminishing at the bottom <strong>of</strong> the<br />

cycle, so that the strength <strong>of</strong> the v<strong>or</strong>tices is <strong>of</strong>fset asymmetrically on the wingtips. There is also a<br />

delay in the strengthening <strong>of</strong> the tip v<strong>or</strong>tex. It actually develops further as the wing begins to roll<br />

down, and delays its shrinking until the wing has already begun its downward rolling motion.<br />

This indicates a lag in the flow’s reaction to the rolling motion.<br />

The instantaneous Cp measurements plotted against non-dimensional ch<strong>or</strong>d are plotted in<br />

Figure 6-5 at 93% span and in Figure 6-6 at 88% span on the left wing f<strong>or</strong> one developed cycle<br />

72

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