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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Thrust per unit span (g)<br />
3.5<br />
3.0<br />
2.5<br />
2.0<br />
1.5<br />
1.0<br />
0.5<br />
Classical Angular Momentum<br />
Average Wake Deficit<br />
Gaussian Wake<br />
0.0<br />
0.2 0.3 0.4 0.5 0.6<br />
r/R<br />
0.7 0.8 0.9 1.0<br />
Chapter 6<br />
FIGURE 6.35 Predicted spanwise torque distributions <strong>for</strong> the 4-blade 2.5cm rotor using three<br />
different viscous swirl models.<br />
The trends are consistent across the span <strong>and</strong> globally <strong>for</strong> both metrics. The Gaussian<br />
wake model predicts the highest thrust <strong>and</strong> required power, 0.0455N <strong>and</strong> 0.485W. For<br />
this example, the localized nature of the Gaussian velocity deficit distribution results in<br />
zero viscous swirl effect all along the blade except at the inner-most stations. The thrust<br />
<strong>and</strong> power values drop 5.5% <strong>and</strong> 4.7% respectively <strong>for</strong> the angular momentum model.<br />
The average wake deficit model results in the lowest values, 17.4% <strong>and</strong> 15.3% lower<br />
than the global thrust <strong>and</strong> power required predicted with the average wake deficit model.<br />
It was initially thought that the choice of viscous swirl model might have a<br />
significant effect on both the inflow angle <strong>and</strong> the local flow velocity, but this has proven<br />
not to be the case. Due to the coupling between the vertical <strong>and</strong> tangential induced<br />
velocities in the rotor relations, the effect on inflow angle is minimal. The predominant<br />
effect of the viscous swirl corrections is a reduction in the flow velocity, resulting in a<br />
reduction in <strong>Reynolds</strong> number <strong>and</strong> dynamic pressure.<br />
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