mae 331 lecture 24
DESCRIPTION
aviationsTRANSCRIPT
Atmospheric Hazards to FlightRobert Stengel,
Aircraft Flight Dynamics, MAE 331, 2010
! Microbursts
! Wind Rotors
! Wake Vortices
! Clear AirTurbulence
Copyright 2010 by Robert Stengel. All rights reserved. For educational use only.http://www.princeton.edu/~stengel/MAE331.html
http://www.princeton.edu/~stengel/FlightDynamics.html
Frames of Reference
! Inertial Frames! Earth-Relative
! Wind-Relative (Constant Wind)
! Non-Inertial Frames! Body-Relative
! Wind-Relative (Varying Wind)
Alternative Reference Framesfor Translational Dynamics
! Earth-relative velocity in earth-fixed polar coordinates:
vE=
VE
!
"
#
$
%%%
&
'
(((
vE=
VE
!E
"E
#
$
%%%
&
'
(((
! Earth-relative velocity inaircraft-fixed polar coordinates(zero wind):
! Body-frame air-mass-relativevelocity:
! Airspeed, sideslip angle, angleof attack
vA=
u ! uw( )
v ! vw( )
w ! ww( )
"
#
$$$$
%
&
''''
=
uA
vA
wA
"
#
$$$
%
&
'''
VA
!A
"A
#
$
%%%
&
'
(((=
uA
2+ v
A
2+ w
A
2
sin)1vA/V
A( )
tan)1wA/V
A( )
#
$
%%%%
&
'
((((
!rI= H
B
IvB
!vB=1
mFBvA( ) +H I
BgI! ""
BvB
!! = L
B
I"
B
!!B= I
B
"1M
BvA( ) " "! B
IB!
B#$ %&
! Rate of change ofTranslational Position
! Rate of change of AngularPosition
! Rate of change ofTranslational Velocity
! Rate of change ofAngular Velocity
Rigid-Body Equations of Motion
! Aerodynamic forces and moments depend on air-relative velocityvector, not the earth-relative velocity vector
Wind Shear Distributions Exert Momentson Aircraft Through Damping Derivatives
! 3-dimensional wind field changes in space and time
wEx,t( ) =
wxx, y, z,t( )
wyx, y, z,t( )
wzx, y, z,t( )
!
"
####
$
%
&&&&E
! Gradient of wind produces different relative airspeedsover the surface of an aircraft
! Wind gradient expressed in body axes
!Clshear" Clpwing
#w
#y$ Clpfin
#v
#x
!Cmshear" Cmqwing ,body ,stab
#w
#x
!Cnshear" Cnrfin ,body
#v
#x
WB= H
E
BW
EH
B
E
WE=
!wx!x !w
x!y !w
x!z
!wy!x !w
y!y !w
y!z
!wz!x !w
z!y !w
z!z
"
#
$$$$
%
&
''''
Aircraft Modes of Motion
! Longitudinal Motions
! Lateral-Directional Motions
!Lon(s) = s
2+ 2"#
ns+ #
n
2( )Ph
s2
+ 2"#ns+ #
n
2( )SP
!LD(s) = s" #
S( ) s" #R( ) s2 + 2$%ns+ %
n
2( )DR
! Wind inputs thatresonate with modes ofmotion are especiallyhazardous
Natural frequency : !n , rad / s
Natural Period : Tn =2"
!n
, sec
Natural Wavelength : Ln = VN Tp , m
Pitch Angle and Normal VelocityFrequency Response to Axial Wind
! !"# j$( )
"Vwind j$( )
! VN!" j#( )
!Vwind j#( )
MacRuer, Ashkenas, and Graham, 1973
! Pitch angle resonance at phugoid natural frequency
! Normal velocity (~ angle of attack) resonance at phugoid andshort period natural frequencies
Pitch Angle and Normal VelocityFrequency Response to Vertical Wind
MacRuer, Ashkenas, and Graham, 1973
! Pitch angle resonance at phugoid and short period natural frequencies
! Normal velocity (~ angle of attack) resonance at short period natural frequency
!!" j#( )
VN!$wind j#( )
=!" j#( )
!"wind j#( )
Sideslip and Roll Angle FrequencyResponse to Vortical Wind
=!" j#( )
!pwind j#( )
=!" j#( )
!pwind j#( )
MacRuer, Ashkenas, and Graham, 1973
! Sideslip angle resonance at Dutch roll natural frequency
! Roll angle is integral of vortical wind input
Sideslip and Roll AngleFrequency Response to Side Wind
MacRuer, Ashkenas, and Graham, 1973
! Sideslip and roll angle resonance at Dutch roll natural frequency
!" j#( )
!"wind j#( )
=!" j#( )
!$wind j#( )
Microbursts
1/2-3-km-wide“Jet”impinges on surface
High-speed outflowfrom jet core
Ring vortexforms inoutlow
Outflow strong enough toknock down trees
The Insidious Nature ofMicroburst Encounter
! The wavelength of the phugoid mode and the disturbanceinput are comparable
DELTA 191 (Lockheed L-1011)
http://www.youtube.com/watch?v=BxxxevZ0IbQ&NR=1
Importance of Proper Responseto Microburst Encounter
! FAA Windshear Training Aid, 1987,addresses proper operatingprocedures for suspected windshear
! Stormy evening July 2, 1994
! USAir Flight 1016, Douglas DC-9,Charlotte
! Windshear alert issued as 1016 begandescent along glideslope
! DC-9 encountered 61-kt windshear,executed missed approach
! Plane continued to descend, strikingtrees and telephone poles beforeimpact
! Go-around procedure was beguncorrectly -- aircraft's nose rotated up -- but power was not advanced
! That, together with increasingtailwind, caused the aircraft to stall
! Crew lowered nose to eliminate stall,but descent rate increased, causingground impact
Optimal Flight PathThrough Worst JAWS Profile
! Graduate research of Mark Psiaki
! Joint Aviation Weather Study (JAWS)measurements of microbursts (ColoradoHigh Plains, 1983)
! Negligible deviation from intended pathusing available controllability
! Aircraft has sufficient performancemargins to stay on the flight path
Downdraft
Headwind
Airspeed
Angle of Attack
Pitch Angle
Throttle Setting
Optimal and 15° PitchAngle Recovery during
Microburst Encounter
! Graduate Research of Sandeep Mulgund
! Airspeed vs. Time! Altitude vs. Time
! Angle of Attack vs. Time
Encounteringoutflow
Rapid arrestof descent
Nonlinear-Inverse-Dynamic Control
! Nonlinear system with additive control:
! Output vector:
! Differentiate output until control appears ineach element of the derivative output:
! Inverting control law:
!x t( ) = f x t( )!" #$ +G x t( )!" #$u t( )
y t( ) = h x t( )!" #$
y
d( )t( ) = f * x t( )!" #$ +G * x t( )!" #$u t( ) ! v t( )
u t( ) = G * x t( )!" #$ vcommand % f * x t( )!" #$!" #$
Landing Abort using Nonlinear-Inverse-Dynamic Control
! from Mulgund
400
500
600
700
800
900
1 103
-7500 -5000 -2500 0 2500 5000 7500
Umax
= 60 ft/sec
Umax
= 70 ft/sec
Umax
= 80 ft/sec
Umax
= 90 ft/sec
Umax
= 100 ft/sec
Umax
= 110 ft/sec
Altitude (
ft)
Range (ft)
100
150
200
250
300
350
-7500 -5000 -2500 0 2500 5000 7500
Umax
= 60 ft/sec
Umax
= 70 ft/sec
Umax
= 80 ft/sec
Umax
= 90 ft/sec
Umax
= 100 ft/sec
Umax
= 110 ft/sec
Airspeed (
ft/s
ec)
Range (ft)
-5
0
5
10
15
-7500 -5000 -2500 0 2500 5000 7500
Umax
= 60 ft/sec
Umax
= 70 ft/sec
Umax
= 80 ft/sec
Umax
= 90 ft/sec
Umax
= 100 ft/sec
Umax
= 110 ft/sec
Alp
ha
(d
eg
)
Range (ft)
Angle of Attack Limit
Wind Shear Safety Advisor
! Graduate research of Alexander Stratton
! LISP-based expert system
ON-BOARD DATA
Reactive sensorsWeather radarForward-lookingLightning sensorsFuture products
AIRCRAFT
SYSTEMS
CREW
Interface
ADVISORYSYSTEM LOGIC
GROUND-BASEDDATA
LLWASTDWRPIREPSForecastsWeather dataFuture products
Estimating the Probability ofHazardous Microburst Encounter
! Bayesian Belief Network! Infer probability of hazardous
encounter from
• pilot/control towerreports
• measurements
• location
• time of day
Wind Rotors
Aircraft Encounters witha Wind Rotor
Radius, ft
TangentialVelocity,
ft/s
! Tangential velocity vs. radius forLamb-Oseen Vortex
Geometry and Flight Condition of JetTransport Encounters with Wind Rotor
! Graduate researchof Darin Spilman
! Flight Condition! True Airspeed = 160 kt
! Altitude = 1000 ft AGL
! Flight Path Angle = -3˚
! Weight = 76,000 lb
! Flaps = 30˚
! Open-Loop Control
! Wind Rotor! Maximum Tangential
Velocity = 125 ft/s
! Core Radius = 200 ft
a) co-axial, ! = 0
b) ! ! 0
35
35
vortex
vortex
wind
!
35
Typical Flight Paths inWind Rotor Encounter
! from Spilman
-50
0
50
100
150
200
250
! [
deg
]
0 5 10 15 20 25 30Time [sec]
"i = 0
"i = 60˚
-60
-50
-40
-30
-20
-10
0
! [
deg
]
10
20
0 5 10 15 20Time [sec]
25 30
"i = 0˚
"i = 60˚
-300
-200
-100
0
100
200
300
-400 -300
h [
ft]
-200 -100 0 100 200 300y [ft]
400
rotor core radius
flight path
initial entry point
Linear-Quadratic/Proportional-Integral Filter (LQ/PIF) Regulator
LQ/PIF Regulation ofWind Rotor Encounter
! from Spilman
-50
0
50
100
150
200
! [
deg
]
0 2 4 6 8 10
Time [sec]
LQR-PIF controlno control input
0
200
400
600
800
1000
1200
h (
AG
L)
[ft]
0 2 4 6 8 10
LQR-PIF control
Time [sec]
no control input
Wake Vortices
C-5A Wing Tip Vortex Flight Test
http://www.dfrc.nasa.gov/gallery/movie/C-5A/480x/EM-0085-01.mov
L-1011 Wing Tip Vortex Flight Test
http://www.dfrc.nasa.gov/gallery/movie/L-1011/480x/EM-0085-01.mov
Models of Single and DualWake Vortices
Wake Vortex Descentand Downwash
Wake Vortex Descent andEffect of Crosswind
! from FAA Wake Turbulence Training Aid, 1995
Magnitude and Decay ofB-757 Wake Vortex
! from Richard Page et al, FAA Technical Center
Aircraft as Wake VortexGenerators and Receivers
! Vorticity, !, generated by lift in 1-g flight
! =KgeneratorW
"VNb
! Rolling acceleration response to vortexaligned with the aircraft's longitudinal axis
Kgenerator
!4
!
Kreceiver
!
CL!
2"VNb
!p =
Kreceiver
1
2!VN
2Sb
Ixx"
Rolling Response vs. Vortex-Generating Strength for 125 Aircraft
! Undergraduate summer project of James Nichols
FAA Wake Vortex Flight Test andNTSB Simulation of US Air 427
! B-737 behind B-727 in FAA flight test
! Control actions subsequent to wake vortexencounter may be problematical
! US427 rudder known to be hard-over from DFDR
NTSB Simulation of American 587
! Flight simulation obtained from digital flight data recorder (DFDR)tape
Digital Flight Data RecorderData for American 587
American 587 (Airbus A-300-600)Encounter with B-747 Wake
! PIO and/oraggressive use ofrudder seen aspossible cause
! Aviation Daily,5/22/02! Boeing Issues Detailed
Guidance On RudderUse For Roll Control
Causes ofClear Air Turbulence
! from Bedard
DC-10 Encounter with Vortex-Induced Clear Air Turbulence
! from Parks, Bach, Wingrove, and Mehta
DC-8 and B-52H Encounterswith Clear Air Turbulence
! DC-8: One engine and 12 ft ofwing missing after CATencounter over Rockies
! Specially instrumented for airturbulence research after someoperational B-52s were lost
! Vertical tail lost after a severeand sustained burst (+5 sec) ofclear air turbulence violentlybuffeted the aircraft
! The Boeing test crew flewaircraft to Blytheville AFB,Arkansas and landed safely
Conclusions
! Critical role of decision-making, alerting, andintelligence
! Reliance on human factors and counter-intuitive strategies
! Need to review certification procedures
! Opportunity to reduce hazard through flightcontrol system design! Disturbance rejection
! Failure Accommodation
! Importance of Eternal vigilance