Page 269 - Aircraft Stuctures for Engineering Student
P. 269

250  Airworthiness and airframe loads

                   We see from either Eq. (8.15) or Eq. (8.16) that the smaller the radius of the flight
                 path, that is the more severe the pull-out, the greater the value of n. It is quite possible
                 therefore for a severe pull-out to overstress the aircraft by subjecting it to loads which
                 lie outside the flight envelope and which may even exceed the proof or ultimate loads.
                 In practice, the control surface movement may be limited by  stops incorporated in
                 the control circuit. These stops usually operate only above a certain speed giving
                 the aircraft adequate manoeuvrability at lower speeds. For hydraulically operated
                 controls  'artificial feel'  is built in to the system whereby the  stick force increases
                 progressively as the speed increases; a necessary precaution in this type of system
                 since the pilot is merely opening and closing valves in the control circuit and therefore
                 receives no direct physical indication of control surface forces.
                   Alternatively, at low speeds, a severe pull-out or pull-up may stall the aircraft.
                 Again safety precautions are usually incorporated in the form of stall warning devices
                 since, for modern high speed aircraft, a stall can be disastrous, particularly at low
                 altitude.


                 8.5.2  Correctly banked turn                      -
                             -__.)1_---                                                 I
                 In this manoeuvre the aircraft flies in a horizontal turn with no sideslip at constant
                 speed. If the radius of the turn is R and the angle of bank 4, then the forces acting
                 on the aircraft are those shown in Fig. 8.12. The horizontal component of the lift
                 vector in this case provides the force necessary to produce the centripetal acceleration
                 of the aircraft towards the centre of the turn. Thus
                                                       wv2
                                              Lsin4 =-                              (8.17)
                                                       gR
                 and for vertical equilibrium
                                               Leos+= w                             (8.18)
                 or
                                               L= Wsec4                             (8.19)




















                 Fig. 8.12  Correctly banked turn.
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