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72 Fuselage<br />

9–3 Aerodynamics<br />

The aerodynamic velocity of the fuselage relative to the air, including interference, is calculated in<br />

component axes, v B . The angle-of-attack αfus, sideslip angle βfus (hence C BA ), and dynamic pressure<br />

q are calculated from v B . The reference area for the fuselage forward-flight drag is the fuselage wetted<br />

area Swet, which is input or calculated as described previously. The reference area for the fuselage<br />

vertical drag is the fuselage projected area Sproj, which is input or calculated as described previously.<br />

9-3.1 Drag<br />

The drag area or drag coefficient is defined for forward flight, vertical flight, and sideward flight.<br />

In addition, the forward-flight drag area or drag coefficient is defined for fixtures and fittings, and<br />

for rotor-body interference. The effective angle-of-attack is αe = αfus − αDmin, where αDmin is the<br />

angle of minimum drag; in reverse flow (|αe| > 90), αe ← αe − 180 signαe. For angles of attack less<br />

than a transition angle αt, the drag coefficient equals the forward-flight (minimum) drag CD0, plus an<br />

angle-of-attack term. Thus if |αe| ≤αt<br />

and otherwise<br />

CDt = CD0 (1 + Kd|αt| Xd )<br />

CD = CDt +<br />

CD = CD0 (1 + Kd|αe| Xd )<br />

<br />

Sproj<br />

CDV − CDt<br />

Swet<br />

<br />

<br />

π<br />

sin<br />

2<br />

<br />

|αe|−αt<br />

π/2 − αt<br />

and similarly for the transition of payload drag (D/q)pay and contingency drag (D/q)cont. Optionally<br />

there might be no angle-of-attack variation at low angles (Kd =0), or quadratic variation (Xd =2). With<br />

an input transition angle, there will be a jump in the slope of the drag coefficient at αt. For a smooth<br />

transition, the transition angle that matches slopes as well as coefficients is found by solving<br />

<br />

2Xd<br />

− 1 α<br />

π Xd<br />

t − Xdα Xd−1<br />

t + (Sproj/Swet)CDV − CD0<br />

=0<br />

KdCD0<br />

This calculation of the transition angle is only implemented with quadratic variation, for which<br />

αt = 1<br />

⎛ <br />

⎝1+<br />

a<br />

1 − a (Sproj/Swet)CDV<br />

⎞<br />

− CD0 ⎠<br />

KdCD0<br />

with a =(4/π) − 1; αt is, however, required to be between 15 and 45 degree. For sideward flight<br />

(v B x =0) the drag is obtained using φv = tan −1 (−v B z /v B y ) to interpolate between sideward and vertical<br />

coefficients:<br />

CD = CDS cos 2 φv + Sproj<br />

CDV sin<br />

Swet<br />

2 φv<br />

Then the drag force is<br />

<br />

D = qSwet CD + CDfit + <br />

<br />

CDrb + q (D/q)pay +(D/q)cont<br />

including drag coefficient for fixtures and fittings CDfit and rotor-body interference CDrb (summed over<br />

all rotors); drag area of the payload (specified for flight state); and contingency drag area.<br />

9-3.2 Lift and Pitch Moment<br />

The fuselage lift and pitch moment are defined in fixed form (L/q and M/q), or scaled form<br />

(CL and CM, based on the fuselage wetted area and fuselage length). The effective angle-of-attack is

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