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Aerodynamics and Design for Ultra-Low Reynolds Number Flight

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Chapter 4<br />

of the pitch angle at the rotor with the vertical ring spacing held constant. Other models<br />

are possible, such as varying the separation at fixed strength, but this model is straight<br />

<strong>for</strong>ward <strong>and</strong> allows the wake length to be rigidly defined as an input.<br />

This procedure is repeated until the wake structure reaches equilibrium, typically five to<br />

ten cycles. The ring model extends downstream <strong>for</strong> five rotor radii. The variations in<br />

the computed induced velocities appear to be negligible <strong>for</strong> larger wake lengths while<br />

any increase in length also increases the computational cost due to additional rings. The<br />

equilibrium wake <strong>for</strong>m is axisymmetric <strong>and</strong> symmetric from end to end, with a ‘bell-<br />

mouth’ at the stream-tube exit equal to the rotor disk area. Additional wake length<br />

moves the exit ‘bell-mouth’ further downstream but does not significantly affect the<br />

solution <strong>and</strong> adds to the computational expense. The initial <strong>and</strong> converged ring<br />

configuration <strong>for</strong> a c<strong>and</strong>idate rotor are displayed in Figures 4.5 <strong>and</strong> 4.6. The rotor plane<br />

is at x=0 <strong>and</strong> the streamtube exit is below the lower extent of the figures.<br />

67

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