introductory review for flight

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  • Review Flow Characterization Quantities - Mach number - Reynolds number Flow Physics - Continuity - Conservation of momentum - Conservation of energy Standard Atmosphere - Equation of state - Standard atmosphere Aircraft Instruments Parts of an Airplane

    1

  • Incompressible vs. Compressible Function of Mach number

    Air is an example of a compressible fluid Its density changes if temperature changes, or if some

    external force is applied A flow is said to be incompressible if there are no

    changes in density attributable to (or caused by) the velocity or speed of the flow

    Theory and observations in wind tunnels suggest that most flows may be treated as incompressible (i.e., constant density) until the Mach number is sufficiently high (>0.4 or so)

    M = Velocity / Speed of Sound 2

  • Speed of Sound From thermodynamics, and compressible flow theory,

    sound travels at the following speed:

    where, a is Speed of Sound is Ratio of Specific Heats (1.4 for air) R is Gas Constant T is Temperature (in oK or degrees oR)

    So, really depends on Temperature!

    RTa =

    3

  • Why a function of M? If there is sufficient time for the sound waves to travel

    before the body arrives, the fluid particles downstream will hear the message and tend to get out of the way

    Otherwise, there will be a crush (compression), or even a large jump in density (shock wave)

    4

  • Viscid vs. Inviscid Flow Function of Reynolds Number (Rn)

    Streamlines describe the path the fluid particles will take

    Flow velocity is tangential to the streamline

    Viscosity alters the shape of streamlines around bluff bodies

    Scientists inject smoke particles into streamlines to make them visible to the naked eye

    Reynolds number can be thought of as the ratio of pressure and viscous forces of the fluid.

    Inviscid (ideal) flow

    Viscous flow dia.Cylinder D

    VDNumber Reynolds

    =

    =

    where

    5

  • Streamlines over an Airfoil

    6

  • Flow Physics

    Continuity Conservation of Momentum Conservation of Energy

    7

  • Continuity Equation

    Area A1 Density 1 Velocity V1

    Area A2 Density 2 Velocity V2

    Rate at which mass enters=1A1V1 Rate at which mass leaves=2A2V2

    8

  • Conservation of Momentum Newtons 2nd Law

    Rate of change of momentum is sum of forces, i.e., F = ma

    Consider a small slice of stream tube

    Rate of change of momentum of the fluid particles within this stream tube slice must be due to forces acting on it Force = time rate of change of Momentum

    9

  • Momentum Equation: Rate of Change of Momentum

    Density velocity V Area = A

    Density +d velocity V+dV Area = A+dA

    Mass Flow Rate in = Mass Flow rate out (Continuity) VA = (+d)(V+dV)(A+dA)

    Momentum rate in = Mass flow rate times velocity = V2A

    Momentum Rate out = Mass flow rate times velocity = VA (V+dV)

    Rate of change of momentum within this element = Momentum rate out - Momentum rate in

    = VA (V+dV) - V2A = VA dV 10

  • Momentum Equation: Forces Acting on Stream Tube

    Pressure times

    Area = pA (p+dp)(A+dA)

    Horizontal Force = Pressure times area of the ring = (p+dp/2)dA

    Area of ring = dA

    Net force = pA + (p+dp/2)dA-(p+dp)(A+dA) =- Adp - dpdA/2 -Adp

    Product of two small numbers

    11

  • Momentum Equation Rate of change of momentum = AVdV Forces acting on the stream tube = -Adp

    Note: We have neglected all other forces: viscous, gravity, electrical and magnetic forces

    Equating the two factors (and divide by A), we get

    Eulers equation

    VdV + dp = 0

    12

  • Momentum Equation for Incompressible Flow

    For incompressible flows ( constant), Eulers equation can be integrated:

    called Bernoullis Equation This total pressure is constant along a streamline,

    High Reynolds number, low Mach number

    TpConstpV

    dpVdV

    dpVdV

    ==+

    =+

    =+

    2

    21

    0

    0

    13

  • Ideal Gas Law or Equation of State

    Most gases satisfy the following relationship between density, temperature and pressure:

    p = RT p = Pressure (in lb/ft2 or N/m2) = Rho , density (in slugs/ft3 or kg/m3) T = Temperature (in Degrees R or degrees K) R = Gas Constant, varies from one gas to another. Equals 287.1 J/Kg/K or 1715.7 ft lbf/slug/oR for air

    14

  • What is a standard atmosphere?

    Weather conditions vary around the globe, from day to day.

    Taking all these variations into design is impractical. A standard atmosphere is therefore defined, that

    relates flight tests, wind tunnel tests and general airplane design to a common reference.

    This common reference is called a standard atmosphere.

    15

  • International Standard Atmosphere Standard Sea Level Conditions

    Pressure 101325 Pa 2116.7 lbf/ft2 Density 1.225 Kg/m3 0.002378 slug/ft3 Temperature 15 oC or 288 K 59 oF or 518.4 oR

    16

  • Standard Atmosphere Variation of temperature, density and

    pressure with altitude can be computed for a standard atmosphere.

    These properties may be tabulated, as shown in Appendix A of the text by Nelson.

    Short programs called applets exist on the world wide web for computing atmospheric properties.

    17

  • Aircraft Instruments Airspeed Indicator Altimeter Rate of Climb Indicator Machmeter Angle of Attack Indicator

    18

  • Airspeed Designations Indicated airspeed (IAS): Airspeed indicated by the

    airspeed instrument, which is affected by altitude, compressibility, instrument, and position errors.

    Calibrated airspeed (CAS): Indicated airspeed corrected for instrument and position errors.

    True airspeed (TAS): Actual airspeed. Equivalent airspeed (EAS): Equivalent airspeed at

    sea level standard atmosphere corresponding to the true dynamic pressure. 122 = 122

    19

  • Pitot Tube: Measure Airspeed using Bernoullis Equation

    Measure local pressure of air: pS, static pressure

    Measure pressure after bringing to zero speed relative to instrument (i.e., bring to stagnation): pT, total pressure

    From Bernoulli:

    Determine velocity of flow with respect to instrument:

    Note: really only need difference between pS and pT

    TS ppV =+2

    21

    ( )

    ST ppV = 2

    20

  • Pitot Tube

    (Wikopedia)

    Measure pressure difference ( )

    ST ppV = 221

  • Pitot-static system Total pressure probe(s) not

    behind propulsion sources, near front of aircraft usually on sides of fuselage near front or front of a wing

    Static pressure port(s) in location with minimum disturbance from aircraft itself usually sides of fuselage

    Airspeed indicator shows measured airspeed to pilot

    2 on each side of this Boeing 757 22

  • Airspeed Indicator

    is air density at sea level in a standard atmosphere

    Mechanically uses Bernoullis equation to show airspeed not corrected for density

    Aircraft are typically flown via this so-called indicated airspeed (not corrected for density, mechanical errors, etc.) in knots

    ( )std

    2

    ST ppV =

    23

  • Using Mach Number in Energy Equations

    20

    02

    02

    0

    2

    21-1 ,

    21-1 :get to1)-/(by throughDivide

    121get to

    1 Use

    2

    MTTOr

    TT

    RTVRT

    RTVRTRCC

    TCVTC

    Vp

    pp

    +=

    =+

    =+

    ==

    =+

    llyadiabatica and reversiblyrest brought to are they if have, willparticles theproerties theare Theselyrespective pressure, stagnation

    and density, stagnation pressure, stagnation called are quantities The2

    1-1

    21-1

    :relations isentropic of aid theWith

    1200

    11

    211

    00

    000 , T, p

    Mpp

    MTT

    +=

    =

    +=

    =

    Mach meter (M

  • Measuring Airspeed, 0.3 < M < 1

    =

    11-

    21

    0

    ppM

    +

    =

    111-

    21

    std

    0stdcalibrated

    pppaV

    =

    11-

    21

    0

    ppaV

    ( )

    ppV = 02

    Only for incompressible flow!

    25

  • For M>1: Must include the effect of shock waves on Pitot tube measurements. Rayleighs formula:

    5.3

    2

    22

    1752.01

    617

    ++

    =

    MMM

    ppo

    Where po is the measured stagnation pressure and p is flow static pressure. Note: The above formula is not valid for very high Mach numbers or very high altitudes.

    26

  • Parts of an Airplane

    27

  • Aerodynamic Controls Elevators control pitch angle Ailerons control roll angle Rudder controls yaw angle Flaps increase lift and drag Leading edge slats increase lift Drag brakes increase drag Spoilers reduce lift and increase drag

    28

  • Body Axes of an Airplane

    xb

    Normal or Vertical axis

    yb

    zb

    29

  • Roll The longitudinal axis extends

    lengthwise through the fuselage from the nose to the tail.

    Movement of the airplane around the longitudinal axis is known as roll and is controlled by movement of the ailerons. xb

    Normal or Vertical axis

    yb

    zb

    30

  • Pitch

    The lateral axis extends crosswise from wingtip to wing tip.

    Movement of the airplane around the lateral axis is known as pitch.

    Pitch is controlled by movement of the elevators.

    xb

    Normal or Vertical axis

    yb

    zb

    31

  • Yaw

    The vertical or normal axis is normal to xbyb passing throug the center of gravity.

    Movement of the airplane around the vertical axis is yaw.

    Yaw is controlled by movement of the rudder.

    xb

    Normal or Vertical axis

    yb

    zb

    32

  • Definition of Forces, Moments, and Velocity Components

    In body fixed coordinates: Angular rates: p, q, r Relative air velocity components: u. v. w Aerodynamic force components: X, Y, Z Aerodynamic moment components: L, M, N Moments of Inertia: Ix, Iy, Iz Products of Inertia: Ixy, Iyz, Ixz

    33

  • Definition of airspeed, angle of attack and sideslip angle

    Airspeed is the magnitude of aircraft velocity relative to air.

    Angle of attack is the angle from

    the projected air velocity vector in body xz-plane to body x-axis, positive in a clockwise sense when looking from the port side.

    Sideslip angle is the angle from

    the body xz-plane to relative air velocity vector, positive in a clockwise sense when looking from the top.

    222 wvuV ++=

    uw1tan=

    222

    1sinwvu

    v++

    =

    34

    ReviewIncompressible vs. CompressibleFunction of Mach numberSpeed of SoundWhy a function of M?Viscid vs. Inviscid Flow Function of Reynolds Number (Rn)Streamlines over an AirfoilFlow PhysicsContinuity EquationConservation of MomentumMomentum Equation: Rate of Change of MomentumMomentum Equation: Forces Acting on Stream TubeMomentum EquationMomentum Equation for Incompressible FlowIdeal Gas Law orEquation of StateWhat is a standard atmosphere?Slide Number 16Standard AtmosphereAircraft InstrumentsAirspeed DesignationsPitot Tube: Measure Airspeed using Bernoullis EquationPitot TubePitot-static systemAirspeed IndicatorUsing Mach Number in Energy EquationsMeasuring Airspeed, 0.3 < M < 1Slide Number 26Parts of an AirplaneAerodynamic ControlsBody Axes of an AirplaneRollPitchYawDefinition of Forces, Moments, and Velocity ComponentsDefinition of airspeed, angle of attack and sideslip angle