30.01.2013 Views

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

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

FIGURE 4.6 Converged wake streamlines <strong>for</strong> a c<strong>and</strong>idate rotor after 6 iterations.<br />

Chapter 4<br />

The inviscid induced rotor inflow velocities are calculated using second order central-<br />

differencing of the stream-function along the blade. These velocities are utilized to<br />

derive a modified κ distribution. Eliminating κ <strong>and</strong> directly using the results to modify<br />

the inflow velocities is inconsistent with the initial separation of viscous <strong>and</strong> inviscid<br />

components of the thrust <strong>and</strong> torque equations as derived earlier. Utilizing a corrected κ<br />

allows the classically derived equations to be used in an unmodified <strong>for</strong>m. The inviscid<br />

momentum <strong>and</strong> blade element thrust equations may be solved <strong>for</strong> BΓ <strong>and</strong> equivalently<br />

Γ ∞ blades :<br />

x/R<br />

2<br />

1.5<br />

1<br />

0.5<br />

0<br />

0.5<br />

1<br />

1.5<br />

4πru( u + U∞) = =<br />

----------------------------------<br />

( Ωr – v)<br />

BΓ Γ ∞ blades<br />

0.5 1 1.5 2<br />

y/R<br />

(4.44)<br />

69

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!