59. Golden Nugget Airlines had great success with their free bar near the tail
of the airplane. (See Problem 5.40) However, when they purchased a much
larger airplane to handle the passenger demand, they discovered that there
was some ‡exibility in the fuselage that caused a lot of unpleasant yawing
motion at the rear of the airplane when in turbulence and was causing the
revelers to spill their drinks. The approximate transfer function for the
dutch roll mode (See Section 10.3.1) is
r(s)
r(s)=8:75(4s2+ 0:4s+ 1)
(s=0:01 + 1)(s2+ 0:24s+ 1)
where ris the airplane’s yaw rate and ris the rudder angle. In performing
a Finite Element Analysis (FEA) of the fuselage structure and adding
those dynamics to the dutch roll motion, they found that the transfer
function needed additional terms that re‡ected the fuselage lateral bending
that occurred due to excitation from the rudder and turbulence. The
revised transfer function is
r(s)
r(s)=8:75(4s2+ 0:4s+ 1)
(s=0:01 + 1)(s2+ 0:24s+ 1) 1
(s2
!2
b
+ 2s
!b+ 1)
where !bis the frequency of the bending mode (= 10 rad/sec) and is the
bending mode damping ratio (= 0:02). Most swept wing airplanes have
a “yaw damper” which essentially feeds back yaw rate measured by a rate
gyro to the rudder with a simple proportional control law. For the new
Golden Nugget airplane, the proportional feedback gain, K= 1;where
r(s) = Kr(s):(3)
(a) Make a Bode plot of the open-loop system, determine the PM and
GM for the nominal design, and plot the step response and Bode
magnitude of the closed-loop system. What is the frequency of the
lightly damped mode that is causing the difficulty?
(b) Investigate remedies to quiet down the oscillations, but maintain the
same low frequency gain in order not to affect the quality of the
dutch roll damping provided by the yaw rate feedback. Specifically,
investigate one at a time:
i. increasing the damping of the bending mode from = 0:02 to
= 0:04:(Would require adding energy absorbing material in
the fuselage structure)
ii. increasing the frequency of the bending mode from !b= 10
rad/sec to !b= 20 rad/sec. (Would require stronger and heavier
structural elements)