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Aerodynamics and Design for Ultra-Low Reynolds Number Flight

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Chapter 6<br />

method with the contracted ring wake <strong>and</strong> angular momentum swirl model have been<br />

used as a common method of comparison.<br />

The resulting chord <strong>and</strong> incidence distributions are provided in Figures 6.42 <strong>and</strong> 6.43.<br />

The largest differences are seen in the inboard half of each blade. The average wake<br />

deficit case is identical to the as-built <strong>and</strong> tested four-blade 2.5cm diameter rotor. The<br />

other two viscous swirl models predict much lower viscous swirl velocities <strong>and</strong> reduce<br />

any penalty associated with blockage due to high local solidity, this permits <strong>and</strong> makes<br />

desirable an increase in chord closer to the hub. With the reduced blockage <strong>and</strong> solidity<br />

penalty, the optimizer increases the total lifting area <strong>and</strong> increases the <strong>Reynolds</strong> number<br />

at the inboard stations, lowering the section drag coefficient.<br />

140<br />

x/R<br />

0.4<br />

0.2<br />

0.0<br />

-0.2<br />

Gaussian Wake<br />

Avg. Wake Deficit<br />

Angular Momentum<br />

-0.4<br />

0.0 0.2 0.4 0.6 0.8 1.0<br />

r/R<br />

FIGURE 6.42 Blade plan<strong>for</strong>ms obtained by applying the rapid design tool with three different<br />

viscous swirl models in conjunction with the classical Pr<strong>and</strong>tl tip loss correction.

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