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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Chapter 4<br />
Beyond the assumptions intrinsic in blade element / actuator ring theory, the only<br />
additional assumptions are that lift is inviscid <strong>and</strong> plays no direct role in the viscous<br />
swirl <strong>and</strong> any tip loss/wake corrections are neglected in the substitution of the thrust<br />
equation. There are no small angle approximations <strong>and</strong> the simplicity of the final <strong>for</strong>m is<br />
due to exact cancellation. Viscous swirl as defined here also incorporates the pressure<br />
drag of the section since both are included in the section drag coefficient. The versatility<br />
of this model appears to extend reasonably well to the ultra-low <strong>Reynolds</strong> number<br />
regime.<br />
4.4 Development of Stream-Function-Based Vortex<br />
Ring Wake Model<br />
Blade-element theory <strong>and</strong> actuator ring theory alone provide a simple model <strong>for</strong> the<br />
wake <strong>and</strong> its effects on the rotor. They do not account <strong>for</strong> any effects of discrete vorticity<br />
in the wake due to a finite blade count, instead assuming the wake is composed of<br />
continuously shed stream-wise vorticity along stream-tubes. The physical analog is the<br />
presence of an infinite number of blades. This model typically overestimates the lift<br />
generated near the blade tips.<br />
The Pr<strong>and</strong>tl tip loss correction described earlier is a significant improvement. It is based<br />
upon helical vortices of constant strength <strong>and</strong> diameter emanating from each blade tip.<br />
The vertical component of the shed vorticity is neglected <strong>and</strong> the wake model reduces to<br />
a semi-infinite column of vortex rings. The spacing of the rings is determined from the<br />
blade spacing <strong>and</strong> the wake tip helix angle, assuming uni<strong>for</strong>m down-wash. From this<br />
potential flow model, the vorticity distribution on the blade is determined <strong>and</strong> expressed<br />
as a correction (κ) to the infinite blade solution. This model is well suited <strong>for</strong> lightly<br />
loaded rotors <strong>and</strong> rotors with large advance ratios. In these two cases, the assumption of<br />
a cylindrical wake is reasonable. The tendency of the helical wake to contract as it<br />
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