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84 Rotor<br />

The force includes a term proportional to the rotor thrust and an input blockage factor fB =ΔT/T ≥ 0.<br />

This term accounts for blockage or download, as an alternative to including the drag of the fuselage<br />

or a lifting surface in the aircraft trim. For example, fB can model the tail-rotor blockage caused by<br />

operation near the vertical tail. The rotor loads in aircraft axes acting at the center of gravity are then:<br />

where Δz F = z F hub − zF cg.<br />

F F = C FS F S<br />

M F = C FS M S + Δz F F F<br />

The wind axis lift L and drag X are calculated from the net rotor-hub force F F and the rotor velocity<br />

v F . The velocity relative to the air gives the propulsive-force direction ep = v F /|v F | (no interference)<br />

and the velocity magnitude V = |v F |. The drag and lift components of the force are X = −e T p F F and<br />

L = |(I −epe T p )F F |, respectively. Thus XV = −(v F ) T F F and L 2 = |F F | 2 −|X| 2 . The rotor contribution<br />

to vertical force is the z-axis component of the force in inertial axes, FV = −k T C IF F F .<br />

11–4 Aerodynamics<br />

The rotor velocity relative to the air is vF = vF AC + ωF ACΔzF in aircraft axes. The velocities in shaft<br />

axes are<br />

v S = C SF v F ⎛<br />

=ΩR⎝<br />

−μx<br />

⎞<br />

rμy ⎠<br />

μz<br />

ω S = C SF ω F ⎛ ⎞<br />

r ˙αx<br />

AC =Ω⎝<br />

˙αy ⎠<br />

r ˙αz<br />

where ΩR is the rotor tip speed. The advance ratio μ, inflowratio λ, and shaft angle-of-attack α are<br />

defined as<br />

μ =<br />

<br />

μ 2 x + μ 2 y<br />

λ = λi + μz<br />

α = tan −1 (μz/μ)<br />

The blade velocity relative to the air has the maximum amplitude (advancing tip velocity) of μat =<br />

(1 + μ) 2 + μ 2 z, from which the advancing tip Mach number is Mat = Mtipμat, using the tip Mach<br />

number Mtip =(ΩR)/cs. The rotor thrust coefficient is defined as CT = T/ρA(ΩR) 2 . The dimensionless<br />

ideal induced velocity λi is calculated from μ, μz, and CT ; then the dimensional velocity is vi =ΩRλi.<br />

The ideal induced power is then Pideal = Tvi. Note that for these inflow velocities, the subscript “i”<br />

denotes “ideal.” The ideal induced velocity could be solved based on the reference velocity vh rather<br />

than the tip speed ΩR, but the advance ratio is required for other purposes as well.<br />

11-4.1 Ideal Inflow<br />

The ideal wake-induced velocity is obtained from the momentum theory result of Glauert:<br />

λi =<br />

CT<br />

2 λ2 sλ<br />

=<br />

+ μ2 2 h <br />

λ2 + μ2 where λ = λi + μz, λ 2 h = |CT |/2 (λh is always positive) and s = sign CT . This expression is generalized<br />

to<br />

λi = λh sF(μ/λh,sμz/λh)

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