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  • 8/11/2019 Mae 331 Lecture 16

    1/19

    Aircraft Control Devicesand Systems

    Robert Stengel, Aircraft Flight Dynamics, MAE 331,2012

    Copyright 2012 by Robert Stengel. All rights reserved. For education al use only.http://www.princeton.edu/~stengel/MAE331.html

    http://www.princeton.edu/~stengel/FlightDynamics.html

    Control surfaces

    Control mechanisms

    Flight control systems

    Design for Control

    Elevator/stabilator:pitch control

    Rudder:yaw control

    Ailerons:roll control

    Trailing-edge flaps:low-angle lift control

    Leading-edge flaps/slats:High-anglelift control

    Spoilers:Roll, lift, and drag control

    Thrust:speed/altitude control

    Critical Issues for Control Effect of control surface deflections on aircraft motions

    Generation of control forces and rigid-body moments on the aircraft

    Rigid-body dynamics of the aircraft

    Eis an input for longitudinal motion

    !!! ="

    Mechanical, Power-Boosted System

    Grumman A-6

    McDonnell Douglas F-15

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    Critical Issues for Control

    Command and control of the control surfaces

    Displacements, forces, and hinge moments of thecontrol mechanisms

    Dynamics of control linkages included in model

    Eis a state for mechanical dynamics

    !!!E ="

    Control Surface Dynamicsand Aerodynamics

    Aerodynamic andMechanical Momentson Control Surfaces

    Increasing size and speed of aircraft

    leads to increased hinge moments This leads to need for mechanical or

    aerodynamic reduction of hingemoments

    Need for aerodynamically balancedsurfaces

    Elevator hinge moment

    Helevator

    =CH

    elevator

    1

    2!V

    2Sc

    Aerodynamic and MechanicalMoments on Control Surfaces

    CHsurface =CH!!!!+CH

    !

    ! +CH"

    "+CHcommand + ...

    CH!!

    : aerodynamic/mechanical damping moment

    CH!

    : aerodynamic/mechanical spring moment

    CH"

    : floating tendency

    CHcommand

    :pilot or autopilot input

    Hinge-moment coefficient, CH Linear model of dynamic effects

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    Angle of Attack andControl Surface Deflection

    Horizontal tail atpositive angle of attack

    Horizontal tail withelevator controlsurface

    Horizontal tail withpositive elevator

    deflection

    Floating and RestoringMoments on a Control Surface

    Positive elevator deflection produces a negative (restoring)moment, H

    , on elevator due to aerodynamic or mechanical spring

    Positive angle of attack produces negative moment on the elevator

    With stick free

    , i.e., no opposing torques, elevator floats

    up dueto negative H

    Dynamic Model of a ControlSurface Mechanism

    !!!" H!!

    !!" H!! = H

    ##+ H

    command + ...

    mechanism dynamics

    =

    external forcing

    Approximate controldynamics by a 2nd-

    order LTI system

    Bring all torques and inertias to right side

    !!!E=H

    elevator

    Ielevator

    =

    CH

    elevator

    1

    2"V2Sc

    Ielevator

    = CH!!E

    !!E+ CH!E

    !E+ CH##+ C

    Hcommand+ ...$%

    &'

    1

    2"V2Sc

    Ielevator

    ( H !!E

    !!E+ H!E!E+ H##+ Hcommand + ...

    Dynamic Model of a ControlSurface Mechanism

    Ielevator

    =effective inertia of surface, linkages, etc.

    H!!E =" H

    elevator I

    elevator( )"!!

    ; H!E

    =

    " Helevator

    Ielevator( )

    "!

    H# =

    " Helevator

    Ielevator( )

    "#

    Stability and control derivatives ofthe control mechanism

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    Coupling of System Model and ControlMechanism Dynamics

    2nd-order model of control-deflection dynamics Command input from cockpit

    Forcing by aerodynamic effects Control surface deflection

    Aircraft angle of attack and angular rates

    Short period approximation

    Coupling with mechanism dynamics

    !!xSP = FSP!xSP +GSP!uSP = FSP!xSP + F"ESP!x

    "E

    ! !q

    !!#

    $

    %&&

    '

    ())*

    Mq M#

    1 +L#VN

    $

    %

    &&&

    '

    (

    )))

    !q

    !#

    $

    %&&

    '

    ())+

    M"E 0

    +L"EVN

    0

    $

    %

    &&&

    '

    (

    )))

    !"E

    !!"E

    $

    %&

    '

    ()

    !!x"E=

    F"E!x

    "E+G

    "E!u

    "E+FSP

    "E!xSP

    !!"E

    ! !!"E

    #

    $%%

    &

    '(()

    0 1

    H"E

    H!"E

    #

    $%%

    &

    '((

    !"E

    !!"E

    #

    $%

    &

    '(+

    0

    *H"E

    #

    $%%

    &

    '((!"E

    command+

    0 0

    Hq H

    +

    #

    $%%

    &

    '((

    !q

    !+

    #

    $%%

    &

    '((

    Short Period Model Augmented byControl Mechanism Dynamics

    Augmented dynamic equation

    Augmented stability and control matrices

    FSP/!E

    =

    FSP

    F!E

    SP

    FSP

    !EF!E

    "

    #

    $$

    %

    &

    ''=

    Mq M

    ( M

    !E 0

    1 )L(VN

    )L!EVN

    0

    0 0 0 1

    Hq H

    ( H

    !E H!!E

    "

    #

    $$$$$$

    %

    &

    ''''''

    !xSP ' =

    !q

    !"

    !#E!!#E

    $

    %

    &&

    &&&

    '

    (

    ))

    )))

    !!xSP /"E

    = FSP/"E

    !xSP /"E

    +GSP /"E

    !"Ecommand

    State Vector

    GSP /!E

    =

    0

    0

    0

    H!E

    "

    #

    $$$$

    %

    &

    ''''

    Roots of the Augmented ShortPeriod Model

    Characteristic equation for short-period/elevator dynamics

    !SP/"E s( ) = sIn # FSP/"E =

    s #Mq( ) #M$ #M"E 0

    #1 s+L

    $

    VN( ) L

    "E

    VN0

    0 0 s #1

    #Hq #H$ #H"E s#H!"E( )

    = 0

    !SP /"E s( ) = s

    2+ 2#

    SP$

    nSPs +$

    nSP

    2( ) s2 +2#"E$n"Es +$n"E2( )

    Short Period Control Mechanism

    Roots of the Augmented ShortPeriod Model

    Coupling of the modes

    depends on designparameters

    M!E

    ,L

    !E

    VN

    ,Hq, andH

    "

    Desirable for mechanical naturalfrequency > short-period naturalfrequency

    Coupling dynamics can beevaluated by root locus analysis

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    Horn Balance

    CH

    !CH

    "

    "+ CH#E

    #E+ CHpilot input

    Stick-free case Control surface free to float

    CH

    !CH

    "

    " +CH

    #E

    #E

    Normally

    CH

    !

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    Control Surface Types

    Elevator

    Horizontal tail and elevatorin wing wake at selectedangles of attack

    Effectiveness of lowmounting is unaffected bywing wake athigh angle ofattack

    Effectiveness of high-mountedelevator is unaffected by wingwake atlow to moderate angleof attack

    Ailerons

    When one aileron goes up, the other goes down Average hinge moment affects stick force

    Compensating Ailerons

    Frise aileron

    Asymmetric contour, with hinge line at orbelow lower aerodynamic surface

    Reduces hinge moment

    Cross-coupling effects can be adverseorfavorable, e.g. yaw rate with roll

    Up travel of one>down travel of other tocontrol yaw effect

    Abzug & Larrabee, 2002

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    Spoilers Spoiler reduces lift, increases drag

    Speed control

    Differential spoilers Roll control

    Avoid twist produced by outboardailerons on long, slender wings

    free trailing edge for larger high-liftflaps

    Plug-slot spoiler on P-61 BlackWidow:low control force

    Hinged flap has high hinge moment

    North American P-61

    Abzug & Larrabee, 2002

    Elevons

    Combined pitch and roll controlusing symmetric andasymmetric surface deflection

    Principally used on

    Delta-wing configurations

    Swing-wing aircraft

    Grumman F-14

    General Dynamics F-106

    Canards Pitch control

    Ahead of wing downwash

    High angle of attackeffectiveness

    Desirable flying qualitieseffect (TBD)

    Dassault Rafale

    SAAB Gripen

    Yaw Control of Tailless Configurations

    Typically unstable in pitch and yaw

    Dependent on flight control systemfor stability

    Split ailerons or differential dragflaps produce yawing moment

    McDonnell Douglas X-36

    Northrop Grumman B-2

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    Rudder Rudder provides yaw control

    Turn coordination

    Countering adverse yaw

    Crosswind correction

    Countering yaw due to engine loss

    Strong rolling effect, particularly at high #

    Only control surface whose nominalaerodynamic angle is zero

    Possible nonlinear effect at low deflectionangle

    Insensitivity at high supersonic speed Wedge shape, all-moving surface on North

    American X-15

    Martin B-57

    Bell X-2

    Rudder Has Mechanical As Well asAerodynamic Effects

    ! American Airlines 587 takeoff behind Japan Air 47, Nov. 12, 2001

    ! Excessive periodic commands to rudder caused vertical tail failure

    Japan B-747American A-300

    http://www.usatoday.com/story/travel/flights/2012/11/19/airbus-rudder/1707421/

    NTSB Simulation of AmericanFlight 587

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

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    Control MechanizationEffects

    Control Mechanization Effects

    Fabric-covered controlsurfaces(e.g., DC-3, Spitfire)subject to distortion under airloads, changing stability andcontrol characteristics

    Control cable stretching

    Elasticity of the airframechanges cable/pushrodgeometry

    Nonlinear control effects friction

    breakout forces

    backlash

    Douglas DC-3

    SupermarineSpitfire

    Nonlinear Control Mechanism Effects

    Friction

    Deadzone

    Control Mechanization Effects

    Breakout force

    Force threshold

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    B-52 Control Compromises toMinimize Required Control Power

    Limited-authority rudder, allowed by

    Low maneuvering requirement

    Reduced engine-out requirement (1 of

    8 engines) Crosswind landing gear

    Limited-authority elevator, allowed by

    Low maneuvering requirement

    Movable stabilator for trim

    Fuel pumping to shift center of mass

    Small manually controlled "feeler"ailerons with spring tabs

    Primary roll control from poweredspoilers, minimizing wing twist

    Internally BalancedControl Surface

    ! B-52 application!

    Control-surface finwithflexible sealmoves within aninternal cavity inthe main surface

    ! Differentialpressuresreducecontrol hingemoment

    CH !CH"" + CH## + CHpilot input

    Boeing B-52

    B-52 Rudder Control Linkages

    B-52 MechanicalYaw Damper

    Combined stable rudder tab, low-friction bearings, smallbobweight, and eddy-current damper for B-52

    Advantages Requires no power, sensors, actuators, or computers

    May involve simple mechanical components

    Problems Misalignment, need for high precision

    Friction and wear over time

    Jamming, galling, and fouling

    High sensitivity to operating conditions, design difficulty

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    Boeing B-47 Yaw Damper Yaw rate gyrodrives rudder to increase

    Dutch roll damping

    Comment: The plane wouldnt need thiscontraption if it had been designed rightin the first place.

    However, mode characteristics --

    especially damping -- vary greatly withaltitude, and most jet aircraft have yawdampers

    Yaw rate washoutto reduce opposition tosteady turns

    Northrop YB-49 Yaw Damper

    Minimal directional stability due to small vertical surfacesand short moment arm

    Clamshell rudders, like drag flapson the B-2 Spirit

    The first stealth aircraft, though that was not intended

    Edwards AFBnamed after test pilot, Glen Edwards,Princeton MSE, killed testing the aircraft

    B-49swere chopped up after decision not to go intoproduction

    Northrop had the last word: it built theB-2

    Northrop YB-49

    Northrop/Grumman B-2

    Northrop N-9M

    Instabilities Due ToControl Mechanization

    Aileron buzz(aero-mechanical instability; P-80)

    Rudder snaking(Dutch roll/mechanical coupling; Meteor, He-162)

    Aeroelastic coupling (B-47, Boeing 707 yaw dampers)

    Rudder Snaking Control-free dynamics

    Nominally symmetric control position

    Internal friction

    Aerodynamic imbalance

    Coupling of mechanical motion with

    Dutch roll mode

    Douglas DC-2

    Solutions Trailing-edge bevel

    Flat-sided surfaces

    Fully powered controls

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    Roll/Spiral Limit CycleDue to Aileron Imbalance

    Unstable nonlinearoscillation growsuntil it reaches asteady state

    This is called alimit cycle

    Lockheed P-38

    Control Surface Buzz

    North American FJ-4

    At transonic speed, normal shocksmay occur on control surface

    With deflection, shocks movedifferentially

    Possibility of self-sustainednonlinear oscillation (limit cycle)

    ARC R&M 3364

    Solutions

    Splitter-plate rudderfixes shock locationfor small deflections

    Blunt trailing edge

    Fully poweredcontrolswithactuators at thesurfaces

    Rudder Lock Rudder deflected to stops at high

    sideslip; aircraft trims at high#

    3 necessary ingredients Low directional stability at high

    sideslip due to stalling of fin

    High (positive) hinge moment-due-to-sideslip at high sideslip(e.g., B-26)

    Negative rudder yawing moment

    Problematical if rudder isunpoweredand requires highfoot-pedal force (rudder floatoflarge WWII aircraft)

    Solutions Increase high-sideslip directional

    stability by adding a dorsal fin(e.g., B-737-100 (before),B-737-400 (after))

    Hydraulically powered rudder

    Martin B-26

    Boeing 737-100

    Boeing 737-400

    Control Systems

    SAS = Stability Augmentation System

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    Downsprings and Bobweights Adjustment of

    Stick-free pitch trim moment

    Stick-force sensitivity toairspeed*

    Downspring

    Mechanical spring with low springconstant

    Exerts a ~constant trailing-edgedown moment on the elevator

    Bobweight

    Similar effect to that of thedownspring

    Weight on control column thataffects feel or basic stability

    Mechanical stability augmentation(weight is sensitive to aircraftsangular rotation)

    Beechcraft B-18

    * See pp. 541-545, Section 5.5, Flight Dynamics

    Effect of Scalar Feedback Controlon Roots of the System

    !y(s)=H(s)!u(s)=kn(s)

    d(s)!u(s)=

    kn(s)

    d(s)K!"(s)

    Block diagram algebra

    H(s)=kn(s)

    d(s)

    =KH(s) !yc(s)"!y(s)[ ]

    !y(s)=KH(s)!yc(s)"KH(s)!y(s)

    K

    Closed-Loop Transfer Function

    1+KH(s)[ ]!y(s)= KH(s)!yc(s)

    !y(s)

    !yc(s)

    =

    KH(s)

    1+KH(s)[ ]

    Roots of the Closed-Loop System

    Closed-loop roots are solutions to

    !closedloop

    (s) =d(s) +Kkn(s) =0

    orKkn(s)

    d(s)=!1

    !y(s)

    !yc(s)

    =

    Kkn(s)

    d(s)

    1+Kkn(s)

    d(s)

    "

    #$%

    &'

    =

    Kkn(s)

    d(s)+Kkn(s)

    [ ]

    =

    Kkn(s)

    !closedloop

    s

    ( )

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    Root Locus Analysis of Pitch Rate Feedback toElevator (2nd-Order Approximation)

    KH s( ) = K !q(s)

    !"E(s)= K

    kq

    s #zq( )

    s2+2$SP%nSP s+%nSP

    2 = #1

    ! # of roots = 2

    ! # of zeros = 1

    ! Destinations of roots (for k=#):

    ! 1 rootgoes to zero ofn(s)

    ! 1 rootgoes toinfinite radius

    ! Angles of asymptotes, $, forthe roots going to#

    ! K-> +#: 180 deg

    ! K-> #: 0 deg

    Root Locus Analysis of PitchRate Feedback to Elevator

    (2nd-OrderApproximation)

    Center of gravity: doesnt

    matter

    Locus on real axis K> 0: Segment to the left of

    the zero

    K< 0: Segment to the right ofthe zero

    Feedback effect is analogousto changing Mq

    Root Locus Analysis of AngularFeedback to Elevator(4th-OrderModel)*

    Flight Path Angle

    Pitch Rate

    Pitch Angle Angle of Attack

    * p. 524, Flight Dynamics

    Root Locus Analysis of AngularFeedback to Thrust(4th-OrderModel)

    Flight Path Angle

    Pitch Rate

    Pitch Angle Angle of Attack

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    Direct Lift andPropulsion Control

    Direct-Lift Control-ApproachPower Compensation

    F-8 Crusader Variable-incidence wing,

    better pilot visibility

    Flight path controlat low

    approach speeds requires throttle use

    could not be accomplishedwith pitch control alone

    Engine response time is slow

    Flight test of direct lift control(DLC), using ailerons as flaps

    Approach powercompensationfor A-7 CorsairIIand direct lift controlstudiedusing Princetons Variable-Response Research Aircraft

    Princeton VRA

    Vought A-7

    Vought F-8

    Direct-Lift/DragControl

    Direct-lift control on S-3AViking

    Implemented with spoilers

    Rigged up

    during landingto allow lift.

    Speed brakes on T-45AGoshawkmake up for slowspool-up time of jet engine BAE Hawk's speed brake

    moved to sides for carrierlanding

    Idle speed increased from55% to 78% to allow moreeffective modulation viaspeed brakes

    Lockheed S-3A

    Boeing T-45

    Next Time:

    Flight Testing forStability and Control

    ReadingFlight Dynamics, 419-428

    Aircraft Stability and Control, Ch. 3Virtual Textbook, Part 17

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    upplementary

    aterial

    Trailing-EdgeBevel Balance

    Bevel has strong

    effect onaerodynamic hingemoments

    See discussion inAbzug and Larrabee

    CH !CH"" + CH## + CHpilot input

    Control Tabs

    Balancing or geared tabs Tab is linked to the main surface

    in opposition to control motion,reducing the hinge moment with

    little change in control effect

    Flying tabs

    Pilot's controls affect only thetab, whose hinge momentmoves the control surface

    Linked tabs

    divide pilot's input between taband main surface

    Spring tabs put a spring in the link to the

    main surface

    Control Flap Carryover Effect onLift Produced By Total Surface

    from Schlichting & Truckenbrodt

    CL!E

    CL"

    vs. c

    f

    xf +

    cf

    c f x f +c f( )

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    Aft Flap vs. All-MovingControl Surface

    Carryover effect

    Aft-flap deflection can be almost as effective as

    full surface deflection at subsonic speeds

    Negligible at supersonic speed

    Aft flap

    Mass and inertia lower, reducing likelihood ofmechanical instability

    Aerodynamic hinge moment is lower

    Can be mounted on structurally rigid mainsurface

    Mechanical and AugmentedControl Systems

    Mechanical systemPush rods, bellcranks, cables, pulleys

    Power boostPilot's input augmented by hydraulic servo that

    lowers manual force

    Fully powered (irreversible) systemNo direct mechanical path from pilot to

    controls

    Mechanical linkages from cockpit controls toservo actuators

    Boeing 767 Elevator Control System

    Abzug & Larrabee, 2002

    Boeing 777 Fly-By-Wire Control System

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    Classical

    Lateral Control Logic fora Fighter Aircraft (c.1970)

    MIL-DTL-9490E , Flight Control Systems - Design, Installation and Test ofPiloted Aircraft, General Specification for, 22 April 2008

    Superseded for new designs on same date bySAE-AS94900

    http://www.sae.org/servlets/works/documentHome.do?comtID=TEAA6A3&docID=AS94900&inputPage=dOcDeTaIlS

    The Unpowered F4DRudder Rudder not a problem under normal flight conditions

    Single-engine, delta-wing aircraft requiring small rudder inputs

    Not a factor for upright spin Rudder was ineffectual, shielded from flow by the large delta wing

    However, in an inverted spin rudder effectiveness was high

    floating tendency deflected rudder in a pro-spin direction 300 lb of pedal forceto neutralize the rudder

    Fortunately, the test aircraft had a spin chute

    Powered Flight Control Systems

    Early powered systems had a singlepowered channel, with mechanicalbackup

    Pilot-initiated reversion to

    "conventional" manual controls

    Flying qualities with manual controloften unacceptable

    Reversion typically could not beundone

    Gearing change between control stickand control to produce acceptable pilot

    load

    Flying qualities changed during a high-stress event

    Hydraulic system failure was common

    Redundancy was needed

    Alternative to eject in military aircraft

    A4D

    A3D

    B-47

    Advanced Control Systems

    Artificial-feel system

    Restores control forces to those of an

    "honest" airplane

    "q-feel" modifies force gradient

    Variation with trim stabilizer angle

    Bobweightresponds to gravity and tonormal acceleration

    Fly-by-wire/light system

    Minimal mechanical runs

    Command input and feedback signalsdrive servo actuators

    Fully powered systems

    Move from hydraulic to electric power

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    Control-Configured Vehicles Command/stability augmentation

    Lateral-directional response

    Bank without turn

    Turn without bank

    Yaw without lateral translation

    Lateral translation without yaw

    Velocity-axis roll (i.e., bank)

    Longitudinal response

    Pitch without heave

    Heave without pitch

    Normal load factor

    Pitch-command/attitude-hold

    Flight path angle

    USAF F-15 IFCS

    Princeton Variable-Response Research AircraftUSAF AFTI/F-16

    United Flight 232, DC-10Sioux City, IA, 1989

    Uncontained engine failure damaged all three flight controlhydraulic systems (http://en.wikipedia.org/wiki/United_Airlines_Flight_232)

    United Flight 232, DC-10Sioux City, IA, 1989

    Pilot maneuvered on differential control of engines to make a runway approach

    101 people died

    185 survived

    Propulsion Controlled Aircraft Proposed backup attitude control in event of flight control system failure

    Differential throttling of engines to produce control moments

    Requires feedback control for satisfactory flying qualities

    NASA MD-11 PCA Flight Test

    NASA F-15 PCA Flight Test

    Proposed retrofit to McDonnell-Douglas(Boeing) C-17