Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend...

21
Atmospheric Hazards to Flight Robert Stengel, Aircraft Flight Dynamics, MAE 331, 2016 ! Microbursts ! Wind Rotors ! Wake Vortices ! Clear Air Turbulence Copyright 2016 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) Earth-Relative Velocity Wind Velocity Air-Relative Velocity Angle of Attack, ! Flight Path Angle, " Pitch Angle, #

Transcript of Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend...

Page 1: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Atmospheric Hazards to Flight!Robert Stengel, !

Aircraft Flight Dynamics, MAE 331, 2016

!! Microbursts!! Wind Rotors!! Wake Vortices!! Clear Air

Turbulence

Copyright 2016 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)

Earth-Relative Velocity Wind Velocity

Air-Relative Velocity

Angle of Attack, !!

Flight Path Angle, ""

Pitch Angle, ##

Page 2: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Pitch Angle and Normal Velocity Frequency 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 and

short period natural frequencies

Pitch Angle and Normal Velocity Frequency 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#( )

Page 3: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Sideslip and Roll Angle Frequency Response 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 Angle !Frequency 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#( )

Page 4: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Microbursts

1/2-3-km-wide Jet impinges on surface

High-speed outflow from jet core

Ring vortex forms in outlow

Outflow strong enough to knock down trees

The Insidious Nature of Microburst Encounter

!! The wavelength of the phugoid mode and the disturbance input are comparable

DELTA 191 (Lockheed L-1011)http://www.youtube.com/watch?v=BxxxevZ0IbQ&NR=1

HeadwindDowndraft

TailwindLanding Approach

Page 5: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Importance of Proper Response !to Microburst Encounter

!! Stormy evening July 2, 1994!! USAir Flight 1016, Douglas DC-9, Charlotte!! Windshear alert issued as 1016 began descent along glideslope!! DC-9 encountered 61-kt windshear, executed missed approach!! Plane continued to descend, striking trees and telephone poles

before impact!! Go-around procedure was begun correctly -- aircraft's nose rotated

up -- but power was not advanced!! That, together with increasing tailwind, caused the aircraft to stall !! Crew lowered nose to eliminate stall, but descent rate increased,

causing ground impact

Optimal Flight Path !Through Worst JAWS Profile

!! Graduate research of Mark Psiaki!! Joint Aviation Weather Study (JAWS)

measurements of microbursts (Colorado High Plains, 1983)

!! Negligible deviation from intended path using available controllability

!! Aircraft has sufficient performance margins to stay on the flight path

Downdraft

Headwind

Airspeed

Angle of Attack

Pitch Angle

Throttle Setting

Page 6: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Optimal and 15° Pitch Angle Recovery during !

Microburst Encounter

!! Graduate Research of Sandeep Mulgund!! Airspeed vs. Time!! Altitude vs. Time

!! Angle of Attack vs. Time

Encountering outflow

Rapid arrest of descent

!! FAA Windshear Training Aid, 1987, addresses proper operating procedures for suspected windshear

Wind Rotors

Page 7: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Aircraft Encounters with !a Wind Rotor

Radius, ft

TangentialVelocity,

ft/s

!! Tangential velocity vs. radius for Lamb-Oseen Vortex

Geometry and Flight Condition of Jet Transport Encounters with Wind Rotor

!! Graduate research of 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

3535

vortex

vortex

wind

!

35

Page 8: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Typical Flight Paths in !Wind Rotor Encounter

!! from Spilman

-50

0

50

100

150

200

250

! [d

eg]

0 5 10 15 20 25 30Time [sec]

" i = 0" i = 60˚

-60

-50

-40

-30

-20

-10

0

! [d

eg]

10

20

0 5 10 15 20Time [sec]

25 30

" i = 0˚" i = 60˚

-300

-200

-100

0

100

200

300

-400 -300

h [f

t]

-200 -100 0 100 200 300y [ft]

400

rotor core radius

flight path

initial entry point

-500

0

500

1000

1500

0 5

h [f

t]

10 15 20 25 30

!i = 0˚!i = 60

Time [sec]

ground

Linear-Quadratic/Proportional-!Integral Filter (LQ/PIF) Regulator

Page 9: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

LQ/PIF Regulation of !Wind Rotor Encounter

!! from Spilman

-50

0

50

100

150

200

! [

deg

]

0 2 4 6 8 10Time [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 Testhttp://www.dfrc.nasa.gov/gallery/movie/C-5A/480x/EM-0085-01.mov

L-1011 Wing Tip Vortex Flight Testhttp://www.dfrc.nasa.gov/gallery/movie/L-1011/480x/EM-0085-01.mov

Page 10: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Models of Single and Dual !Wake Vortices

TangentialVelocity,

ft/s

Radius, ft

Wake Vortex

Wind Rotor

TangentialVelocity,

ft/s

Radius, ft

Wake Vortex Descent and Downwash

Page 11: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Wake Vortex Descent and !Effect of Crosswind

!! from FAA Wake Turbulence Training Aid, 1995

Magnitude and Decay of !B-757 Wake Vortex

!! from Richard Page et al, FAA Technical Center

Page 12: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

NTSB Simulation of US Air 427 and FAA Wake Vortex Flight Test

!! B-737 behind B-727 in FAA flight test!! Control actions subsequent to wake vortex

encounter may be problematical!! US427 rudder known to be hard-over from DFDR

24

Page 13: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

NTSB Simulation of American Flight 587

!! Flight simulation derived from digital flight data recorder (DFDR) tape

25

Digital Flight Data Recorder Data for American 587

Page 14: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Causes of !Clear Air Turbulence

!! from Bedard

DC-10 Encounter with Vortex-Induced Clear Air Turbulence

!! from Parks, Bach, Wingrove, and Mehta

Page 15: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

DC-8 and B-52H Encounters with Clear Air Turbulence

!! DC-8: One engine and 12 ft of wing missing after CAT encounter over Rockies

!! B-52 specially instrumented for air turbulence research after some operational B-52s were lost

!! Vertical tail lost after a severe and sustained burst (+5 sec) of clear air turbulence violently buffeted the aircraft

!! The Boeing test crew flew aircraft to Blytheville AFB, Arkansas and landed safely

Conclusions

!! Critical role of decision-making, alerting, and intelligence

!! Reliance on human factors and counter-intuitive strategies

!! Need to review certification procedures!! Opportunity to reduce hazard through flight

control system design!! Disturbance rejection!! Failure Accommodation

!! Importance of Eternal vigilance

Page 16: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Supplemental Material!

Alternative Reference Frames!for Translational Dynamics

!! Earth-relative velocity in earth-fixed polar coordinates: vE =

VE!

"

#

$

%%%

&

'

(((

vE =VE!E"E

#

$

%%%

&

'

(((

!! Earth-relative velocity in aircraft-fixed polar coordinates (zero wind):

!! Body-frame air-mass-relative velocity:

!! Airspeed, sideslip angle, angle of attack

vA =

u ! uw( )v ! vw( )w ! ww( )

"

#

$$$$

%

&

''''

=

uAvAwA

"

#

$$$

%

&

'''

VA!A

"A

#

$

%%%

&

'

(((=

uA2 + vA

2 + wA2

sin)1 vA /VA( )tan)1 wA /VA( )

#

$

%%%%

&

'

((((

Page 17: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

!rI = HBI vB

!vB =

1mFB vA( ) +H I

Bg I ! """ BvB

!!! = LB

I "" B

!!! B = IB

"1 MB vA( ) " "!! BIB!! B#$ %&

!! Rate of change of Translational Position

!! Rate of change of Angular Position

!! Rate of change of Translational Velocity

!! Rate of change of Angular Velocity

Rigid-Body Equations of Motion

!! Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector

Angle of Attack, !!

Flight Path Angle, ""

Pitch Angle, ##

Wind Shear Distributions Exert Moments on Aircraft Through Damping Derivatives

!! 3-dimensional wind field changes in space and time

wE x,t( ) =wx x, y, z,t( )wy x, y, z,t( )wz x, y, z,t( )

!

"

####

$

%

&&&&E

!! Gradient of wind produces different relative airspeeds over 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 = HEBWEHB

E

WE =

!wx !x !wx !y !wx !z!wy !x !wy !y !wy !z

!wz !x !wz !y !wz !z

"

#

$$$$

%

&

''''

Page 18: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Aircraft Modes of Motion

!! Longitudinal Motions

!! Lateral-Directional Motions

"Lon (s) = s2 + 2#$ns+$n2( )Ph s

2 + 2#$ns+$n2( )SP

"LD (s) = s# $S( ) s# $R( ) s2 + 2%&ns+&n2( )DR

!! Wind inputs that resonate with modes of motion are especially hazardous

Natural frequency : !n , rad / s

Natural Period : Tn =2"!n

, sec

Natural Wavelength : Ln = VN Tp , m

Nonlinear-Inverse-Dynamic Control

!! Nonlinear system with additive control:

!! Output vector:

!! Differentiate output until control appears in each element of the derivative output:

!! Inverting control law:

!x t( ) = f x t( )!" #$ +G x t( )!" #$u t( )

y t( ) = h x t( )!" #$

yd( ) t( ) = f * x t( )!" #$ +G * x t( )!" #$u t( ) ! v t( )

u t( ) = G * x t( )!" #$ vcommand % f * x t( )!" #$!" #$

Page 19: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

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

Airs

peed

(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/secA

lpha

(deg

)

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

SYSTEMSCREW

Interface ADVISORY

SYSTEM LOGIC

GROUND-BASEDDATA

LLWASTDWRPIREPSForecastsWeather dataFuture products

Page 20: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Estimating the Probability of Hazardous Microburst Encounter

!! Bayesian Belief Network!! Infer probability of hazardous

encounter from •! pilot/control tower

reports •! measurements•! location•! time of day

GeographicalLocation

Surface Humidity

Time of Day

ConvectiveWeather

Probability ofMicroburst Wind Shear

Lightning

LightningDetection

Mod/HeavyTurbulence

TurbulenceDetection

Precipitation

WeatherRadar

PilotReport

Low-LevelWind Shear Advisory

SystemAirborne

Forward-LookingDoppler Radar

Reactive Wind ShearAlert System Terminal Doppler

Weather Radar

Aircraft as Wake Vortex Generators and Receivers

!! Vorticity, !!, generated by lift in 1-g flight

! =KgeneratorW"VNb

!! Rolling acceleration response to vortex aligned with the aircraft's longitudinal axis

Kgenerator !

4!

Kreceiver !

CL!

2"VNb

!p =

Kreceiver12!VN

2Sb

Ixx"

Page 21: Atmospheric Hazards to Flightstengel/MAE331Lecture24.pdf · Aerodynamic forces and moments depend on air-relative velocity vector, not the earth-relative velocity vector Angle of

Rolling Response vs. Vortex-Generating Strength for 125 Aircraft

!! Undergraduate summer project of James Nichols

0.0001

0.001

0.01

0.1

1 10 100

RollingResponse

Vortex Generating Strength