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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 />

135

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