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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V total / ωr<br />
1.0<br />
0.9<br />
0.8<br />
Classical Angular Momentum<br />
Average Wake Deficit<br />
Gaussian Wake<br />
0.7<br />
0.2 0.3 0.4 0.5 0.6<br />
r/R<br />
0.7 0.8 0.9 1.0<br />
FIGURE 6.37 Local relative flow velocities using three different viscous swirl models.<br />
Of the three models considered, the classical angular momentum provides the best<br />
Chapter 6<br />
agreement with the OVERFLOW-D results presented earlier. The Gaussian wake model<br />
as currently implemented has no effect <strong>and</strong> the average wake deficit model grossly<br />
under-predicts the sectional thrust <strong>and</strong> torque. None of these models provides an ideal<br />
solution. The angular momentum model is appropriate in the outer blade region where<br />
the <strong>Reynolds</strong> numbers are higher <strong>and</strong> the local annular solidity much lower, but inboard,<br />
the models based on actual viscous wake profiles <strong>and</strong> a direct accounting of local<br />
solidity should more accurately represent the flowfield. In spite of these issues, the<br />
classical angular momentum correction is satisfactory overall <strong>for</strong> analysis since higher<br />
fidelity is not needed inboard due to the triangular loadings typical of rotors.<br />
6.7.2 Effect of Wake Modeling on Per<strong>for</strong>mance Estimation<br />
The impact on per<strong>for</strong>mance estimation of the two wake models, the classical Pr<strong>and</strong>tl tip<br />
loss correction <strong>and</strong> the contracted vortex ring model, has also been explored using the<br />
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